Author: "Marina Putti" - Searchworks@Jio Institute Digital Library Search Results

174 results on '"Marina Putti"'

1. Calorimetric evidence for two phase transitions in Ba1−x K x Fe2As2 with fermion pairing and quadrupling states

Author: Ilya Shipulin, Nadia Stegani, Ilaria Maccari, Kunihiro Kihou, Chul-Ho Lee, Quanxin Hu, Yu Zheng, Fazhi Yang, Yongwei Li, Chi-Ming Yim, Ruben Hühne, Hans-Henning Klauss, Marina Putti, Federico Caglieris, Egor Babaev, and Vadim Grinenko
Subjects: Science
Abstract: Abstract Materials that break multiple symmetries allow the formation of four-fermion condensates above the superconducting critical temperature (T c). Such states can be stabilized by phase fluctuations. Recently, a fermionic quadrupling condensate that breaks the Z 2 time-reversal symmetry was reported in Ba1−xKxFe2As2. A phase transition to the new state of matter should be accompanied by a specific heat anomaly at the critical temperature where Z 2 time-reversal symmetry is broken ( $${T}_{{{{{{{{\rm{c}}}}}}}}}^{{{{{{{{\rm{Z2}}}}}}}}} \, > \, {T}_{{{{{{{{\rm{c}}}}}}}}}$$ T c Z2 > T c ). Here, we report on detecting two anomalies in the specific heat of Ba1−xKxFe2As2 at zero magnetic field. The anomaly at the higher temperature is accompanied by the appearance of a spontaneous Nernst effect, indicating the breakdown of Z 2 symmetry. The second anomaly at the lower temperature coincides with the transition to a zero-resistance state, indicating the onset of superconductivity. Our data provide the first example of the appearance of a specific heat anomaly above the superconducting phase transition associated with the broken time-reversal symmetry due to the formation of the novel fermion order.
Published: 2023
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2. Superconductivity induced by gate-driven hydrogen intercalation in the charge-density-wave compound 1T-TiSe2

Author: Erik Piatti, Giacomo Prando, Martina Meinero, Cesare Tresca, Marina Putti, Stefano Roddaro, Gianrico Lamura, Toni Shiroka, Pietro Carretta, Gianni Profeta, Dario Daghero, and Renato S. Gonnelli
Subjects: Astrophysics, QB460-466, Physics, QC1-999
Abstract: Abstract Hydrogen (H) plays a key role in the near-to-room temperature superconductivity of hydrides at megabar pressures. This suggests that H doping could have similar effects on the electronic and phononic spectra of materials at ambient pressure as well. Here, we demonstrate the non-volatile control of the electronic ground state of titanium diselenide (1T-TiSe2) via ionic liquid gating-driven H intercalation. This protonation induces a superconducting phase, observed together with a charge-density wave through most of the phase diagram, with nearly doping-independent transition temperatures. The H-induced superconducting phase is possibly gapless-like and multi-band in nature, in contrast with those induced in TiSe2 via copper, lithium, and electrostatic doping. This unique behavior is supported by ab initio calculations showing that high concentrations of H dopants induce a full reconstruction of the bandstructure, although with little coupling between electrons and high-frequency H phonons. Our findings provide a promising approach for engineering the ground state of transition metal dichalcogenides and other layered materials via gate-controlled protonation.
Published: 2023
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3. Fe(Se,Te) Thin Films Deposited through Pulsed Laser Ablation from Spark Plasma Sintered Targets

Author: Michela Iebole, Valeria Braccini, Cristina Bernini, Andrea Malagoli, Nicola Manca, Alberto Martinelli, Matteo Cialone, Marina Putti, Shiv J. Singh, Giovanna Latronico, and Paolo Mele
Subjects: iron-based superconductors, thin films, pulsed laser ablation, spark plasma synthesis, critical current density, Technology, Electrical engineering. Electronics. Nuclear engineering, TK1-9971, Engineering (General). Civil engineering (General), TA1-2040, Microscopy, QH201-278.5, Descriptive and experimental mechanics, QC120-168.85
Abstract: Iron-based superconductors are under study for their potential for high-field applications due to their excellent superconducting properties such as low structural anisotropy, large upper critical fields and low field dependence of the critical current density. Between them, Fe(Se,Te) is simple to be synthesized and can be fabricated as a coated conductor through laser ablation on simple metallic templates. In order to make all the steps simple and fast, we have applied the spark plasma sintering technique to synthesize bulk Fe(Se,Te) to obtain quite dense polycrystals in a very short time. The resulting polycrystals are very well connected and show excellent superconducting properties, with a critical temperature onset of about 16 K. In addition, when used as targets for pulsed laser ablation, good thin films are obtained with a critical current density above 105 A cm−2 up to 16 T.
Published: 2024
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4. Mechanochemical Synthesis of Sustainable Ternary and Quaternary Nanostructured Cu2SnS3, Cu2ZnSnS4, and Cu2ZnSnSe4 Chalcogenides for Thermoelectric Applications

Author: Himanshu Nautiyal, Ketan Lohani, Binayak Mukherjee, Eleonora Isotta, Marcelo Augusto Malagutti, Narges Ataollahi, Ilaria Pallecchi, Marina Putti, Scott T. Misture, Luca Rebuffi, and Paolo Scardi
Subjects: Cu-based ternaries and quaternaries, thermoelectricity, Cu2ZnSnS4, Cu2ZnSnSe4, Cu2SnS3, mechanochemistry, Chemistry, QD1-999
Abstract: Copper-based chalcogenides have emerged as promising thermoelectric materials due to their high thermoelectric performance, tunable transport properties, earth abundance and low toxicity. We have presented an overview of experimental results and first-principal calculations investigating the thermoelectric properties of various polymorphs of Cu2SnS3 (CTS), Cu2ZnSnS4 (CZTS), and Cu2ZnSnSe4 (CZTSe) synthesized by high-energy reactive mechanical alloying (ball milling). Of particular interest are the disordered polymorphs of these materials, which exhibit phonon-glass–electron-crystal behavior—a decoupling of electron and phonon transport properties. The interplay of cationic disorder and nanostructuring leads to ultra-low thermal conductivities while enhancing electronic transport. These beneficial transport properties are the consequence of a plethora of features, including trap states, anharmonicity, rattling, and conductive surface states, both topologically trivial and non-trivial. Based on experimental results and computational methods, this report aims to elucidate the details of the electronic and lattice transport properties, thereby confirming that the higher thermoelectric (TE) performance of disordered polymorphs is essentially due to their complex crystallographic structures. In addition, we have presented synchrotron X-ray diffraction (SR-XRD) measurements and ab initio molecular dynamics (AIMD) simulations of the root-mean-square displacement (RMSD) in these materials, confirming anharmonicity and bond inhomogeneity for disordered polymorphs.
Published: 2023
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5. Hydrodynamical description for magneto-transport in the strange metal phase of Bi-2201

Author: Andrea Amoretti, Martina Meinero, Daniel K. Brattan, Federico Caglieris, Enrico Giannini, Marco Affronte, Christian Hess, Bernd Buechner, Nicodemo Magnoli, and Marina Putti
Subjects: Physics, QC1-999
Abstract: High-temperature superconductors are strongly coupled systems which present a complicated phase diagram with many coexisting phases. This makes it difficult to understand the mechanism which generates their singular transport properties. Hydrodynamics, which mostly relies on the symmetries of the system without referring to any specific microscopic mechanism, constitutes a promising framework to analyze these materials. In this paper we show that, in the strange metal phase of the cuprates, a whole set of transport coefficients are described by a universal hydrodynamic framework once one accounts for the effects of quantum critical charge-density waves. We corroborate our theoretical prediction by measuring the DC transport properties of Bi-2201 close to optimal doping, proving the validity of our approach. Our argument can be used as a consistency check to understand the universality class governing the behavior of high-temperature cuprate superconductors.
Published: 2020
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6. The influence of the in-plane lattice constant on the superconducting transition temperature of FeSe0.7Te0.3 thin films

Author: Feifei Yuan, Kazumasa Iida, Vadim Grinenko, Paul Chekhonin, Aurimas Pukenas, Werner Skrotzki, Masahito Sakoda, Michio Naito, Alberto Sala, Marina Putti, Aichi Yamashita, Yoshihiko Takano, Zhixiang Shi, Kornelius Nielsch, and Ruben Hühne
Subjects: Physics, QC1-999
Abstract: Epitaxial Fe(Se,Te) thin films were prepared by pulsed laser deposition on (La0.18Sr0.82)(Al0.59Ta0.41)O3 (LSAT), CaF2-buffered LSAT and bare CaF2 substrates, which exhibit an almost identical in-plane lattice parameter. The composition of all Fe(Se,Te) films were determined to be FeSe0.7Te0.3 by energy dispersive X-ray spectroscopy, irrespective of the substrate. Albeit the lattice parameters of all templates have comparable values, the in-plane lattice parameter of the FeSe0.7Te0.3 films varies significantly. We found that the superconducting transition temperature (Tc) of FeSe0.7Te0.3 thin films is strongly correlated with their a-axis lattice parameter. The highest Tc of over 19 K was observed for the film on bare CaF2 substrate, which is related to unexpectedly large in-plane compressive strain originating mostly from the thermal expansion mismatch between the FeSe0.7Te0.3 film and the substrate.
Published: 2017
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7. Universal scaling behavior of the upper critical field in strained FeSe0.7Te0.3 thin films

Author: Feifei Yuan, Vadim Grinenko, Kazumasa Iida, Stefan Richter, Aurimas Pukenas, Werner Skrotzki, Masahito Sakoda, Michio Naito, Alberto Sala, Marina Putti, Aichi Yamashita, Yoshihiko Takano, Zhixiang Shi, Kornelius Nielsch, and Ruben Hühne
Subjects: Fe-based superconductors, thin film, upper critical fields, Science, Physics, QC1-999
Abstract: Revealing the universal behaviors of iron-based superconductors (FBS) is important to elucidate the microscopic theory of superconductivity. In this work, we investigate the effect of in-plane strain on the slope of the upper critical field H _c2 at the superconducting transition temperature T _c (i.e. −d H _c2 /d T ) for FeSe _0.7 Te _0.3 thin films. The in-plane strain tunes T _c in a broad range, while the composition and disorder are almost unchanged. We show that −d H _c2 /d T scales linearly with T _c , indicating that FeSe _0.7 Te _0.3 follows the same universal behavior as observed for pnictide FBS. The observed behavior is consistent with a multiband superconductivity paired by interband interaction such as sign change s _± superconductivity.
Published: 2018
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8. IRIS-A New Distributed Research Infrastructure on Applied Superconductivity

Author: Rossi, L, Arpaia, P, Attanasio, C, Avallone, G, Avitabile, F, Balconi, L, Bellingeri, E, Beneduce, E, Benson, T, Bernini, C, Bersani, A, Bianchi, A, Broggi, F, Burioli, S, Campana, P, Cannavó, M, Canonica, L, Cialone, M, Cirillo, C, Mario, C, Domenico, D, Mario Del, F, Marta Della, T, Ernesto De, M, Salvatore De, P, Beniamino Di, G, Antonio, E, Stefania, F, Giuliana, F, Umberto, G, Raffaele, G, Gianfrancesco, G, Angelo, L, Enrico, L, Stefano Maffezzoli, F, Andrea, M, Samuele, M, Daniele, M, Giuseppe, M, Fabio, M, Anna Grazia, M, Riccardo, M, Luigi, P, Danilo, P, Marco, P, Marina, P, Silvia, R, Lucia, S, Aniello, S, Carlo, S, Ettore, S, Andrea, S, Claudio, S, Fabio, S, Massimo, S, Stefano, S, Marco, S, Andrea, T, Riccardo, V, and Alessandro, V, Rossi L, Arpaia P, Attanasio C, Avallone G, Avitabile F, Balconi L, Bellingeri E, Beneduce E, Benson T, Bernini C, Bersani A, Bianchi A, Broggi F, Burioli S, Campana P, Cannavó M, Canonica L, Cialone M, Cirillo C, Mario Cuoco, Domenico D’Agostino, Mario Del Franco, Marta Della Torre, Ernesto De Matteis, Salvatore De Pasquale, Beniamino Di Girolamo, Antonio Esposito, Stefania Farinon, Giuliana Fiorillo, Umberto Gambardella, Raffaele Gargiulo, Gianfrancesco Grauso, Angelo Leo, Enrico Leo, Stefano Maffezzoli Felis, Andrea Malagoli, Samuele Mariotto, Daniele Marré, Giuseppe Maruccio, Fabio Miletto, Anna Grazia Monteduro, Riccardo Musenich, Luigi Parodi, Danilo Pedrini, Marco Prioli, Marina Putti, Silvia Rizzato, Lucia Sabbatini, Aniello Saggese, Carlo Santini, Ettore Sarnelli, Andrea Selce, Claudio Severino, Fabio Severino, Massimo Sorbi, Stefano Sorti, Marco Statera, Andrea Traverso, Riccardo Valente, and Alessandro Vannozzi, Rossi, L, Arpaia, P, Attanasio, C, Avallone, G, Avitabile, F, Balconi, L, Bellingeri, E, Beneduce, E, Benson, T, Bernini, C, Bersani, A, Bianchi, A, Broggi, F, Burioli, S, Campana, P, Cannavó, M, Canonica, L, Cialone, M, Cirillo, C, Mario, C, Domenico, D, Mario Del, F, Marta Della, T, Ernesto De, M, Salvatore De, P, Beniamino Di, G, Antonio, E, Stefania, F, Giuliana, F, Umberto, G, Raffaele, G, Gianfrancesco, G, Angelo, L, Enrico, L, Stefano Maffezzoli, F, Andrea, M, Samuele, M, Daniele, M, Giuseppe, M, Fabio, M, Anna Grazia, M, Riccardo, M, Luigi, P, Danilo, P, Marco, P, Marina, P, Silvia, R, Lucia, S, Aniello, S, Carlo, S, Ettore, S, Andrea, S, Claudio, S, Fabio, S, Massimo, S, Stefano, S, Marco, S, Andrea, T, Riccardo, V, and Alessandro, V, Rossi L, Arpaia P, Attanasio C, Avallone G, Avitabile F, Balconi L, Bellingeri E, Beneduce E, Benson T, Bernini C, Bersani A, Bianchi A, Broggi F, Burioli S, Campana P, Cannavó M, Canonica L, Cialone M, Cirillo C, Mario Cuoco, Domenico D’Agostino, Mario Del Franco, Marta Della Torre, Ernesto De Matteis, Salvatore De Pasquale, Beniamino Di Girolamo, Antonio Esposito, Stefania Farinon, Giuliana Fiorillo, Umberto Gambardella, Raffaele Gargiulo, Gianfrancesco Grauso, Angelo Leo, Enrico Leo, Stefano Maffezzoli Felis, Andrea Malagoli, Samuele Mariotto, Daniele Marré, Giuseppe Maruccio, Fabio Miletto, Anna Grazia Monteduro, Riccardo Musenich, Luigi Parodi, Danilo Pedrini, Marco Prioli, Marina Putti, Silvia Rizzato, Lucia Sabbatini, Aniello Saggese, Carlo Santini, Ettore Sarnelli, Andrea Selce, Claudio Severino, Fabio Severino, Massimo Sorbi, Stefano Sorti, Marco Statera, Andrea Traverso, Riccardo Valente, and and Alessandro Vannozzi
Abstract: In the frame of the Next Generation Europe program, the EU program to boost after-COVID recovery, the Italian Minister of University and Research has funded a project called Innovative Research Infrastructure for applied Superconductivity (IRIS). New laboratories will be built or upgraded in six poles: Milan (hub of the infrastructure), Genoa, Frascati, Naples, Salerno, and Lecce, to carry out basic research on magnetism and superconducting materials, test of wires, tapes, and large current cables, superconducting magnets construction with advanced instrumentation, power tests of magnets, and a special facility for high current-high voltage superconducting lines. The program will be executed over three years and then will operate for at least 10 years. It includes two first demonstrators: one HTS magnet to be operated at 10-20 K and a superconducting line of 1 GW (40 kA-25 kV) about 140 m long. The demonstrators anticipate the main scope of the investment in the IRIS infrastructure: to support the use of superconductivity for improving sustainability by decreasing the energy consumption without compromising performance. This article describes the global IRIS project.
Published: 2024

9. Calorimetric evidence for two phase transitions in Ba1-xKxFe2As2 with fermion pairing and quadrupling states

Author: Ilya Shipulin, Nadia Stegani, Ilaria Maccari, Kunihiro Kihou, Chul-Ho Lee, Yongwei Li, Ruben Hühne, Hans-Henning Klauss, Marina Putti, Federico Caglieris, Egor Babaev, and Vadim Grinenko
Abstract: Materials that break multiple symmetries allow, under certain conditions, the formation of four-fermion condensates above the superconducting critical temperature (Tc). Such states can be stabilized by phase fluctuations. Recently a fermionic quadrupling condensate that breaks the Z2 time-reversal symmetry was reported in Ba1-xKxFe2As2 [V. Grinenko et al., Nat. Phys. 17, 1254 (2021)]. However, the related anomaly was not resolved in the specific heat measurements. Resolving two anomalies at Tc and the Z2 transition temperature (TcZ2 > Tc) is key evidence for the existence of two distinct electronic phases. In a broader context, the lack of an additional anomaly in the specific heat at TcZ2 is a common unsolved problem for most superconductors with broken time-reversal symmetry, even in the conventional case where TcZ2 < Tc. Here, we report on detecting two anomalies in the specific heat of Ba1-xKxFe2As2 at zero magnetic field. The anomaly at the higher temperature is accompanied by the appearance of a spontaneous Nernst effect, indicating broken Z2 symmetry. The second anomaly at the lower temperature coincides with the transition to a zero resistance state, indicating superconductivity that breaks the U(1) gauge symmetry. Our data provide the first example of the appearance of a specific heat anomaly above the superconducting phase transition associated with the broken time-reversal symmetry due to the formation of the novel fermion order.
Published: 2023

10. Proton Irradiation Effects on the Superconducting Properties of Fe(Se,Te) Thin Films

Author: Daniele Torsello, Michela Fracasso, Roberto Gerbaldo, Gianluca Ghigo, Francesco Laviano, Andrea Napolitano, Michela Iebole, Matteo Cialone, Nicola Manca, Alberto Martinelli, Laura Piperno, Valeria Braccini, Antonio Leo, Gaia Grimaldi, Angelo Vannozzi, Giuseppe Celentano, Marina Putti, and Laura Gozzelino
Subjects: Critical current, strain, critical temperature, critical fields, iron-based superconductors, proton irradiation, radiation hardness, Electrical and Electronic Engineering, Condensed Matter Physics, Electronic, Optical and Magnetic Materials
Published: 2022

11. Mn-induced Fermi-surface reconstruction in the SmFeAsO parent compound

Author: Alberto Martinelli, G. Lamura, Pietro Bonfà, M. A. Muller, Ifeanyi John Onuorah, S. Sanna, Martina Meinero, J. C. Orain, A. Provino, R. De Renzi, Toni Shiroka, Ilya Eremin, Marina Putti, Pietro Manfrinetti, Meinero M., Bonfa P., Onuorah I.J., Sanna S., De Renzi R., Eremin I., Muller M.A., Orain J.-C., Martinelli A., Provino A., Manfrinetti P., Putti M., Shiroka T., and Lamura G.
Subjects: muon spin spectroscopy, Electronic properties and materials, Science, 02 engineering and technology, 01 natural sciences, Article, Magnetization, Hall effect, Magnetic properties and materials, 0103 physical sciences, Structure of solids and liquids, 010306 general physics, Pnictogen, Physics, Multidisciplinary, Condensed matter physics, Transition temperature, superconductivity, Order (ring theory), Fermi surface, 021001 nanoscience & nanotechnology, Phase transitions and critical phenomena, magnetism, Content (measure theory), Medicine, 0210 nano-technology, Ground state
Abstract: The electronic ground state of iron-based materials is unusually sensitive to electronic correlations. Among others, its delicate balance is profoundly affected by the insertion of magnetic impurities in the FeAs layers. Here, we address the effects of Fe-to-Mn substitution in the non-superconducting Sm-1111 pnictide parent compound via a comparative study of SmFe1-xMnxAsO samples with x(Mn) = 0.05 and 0.10. Magnetization, Hall effect, and muon-spin spectroscopy data provide a coherent picture, indicating a weakening of the commensurate Fe spin-density-wave (SDW) order, as shown by the lowering of the SDW transition temperature TSDW with increasing Mn content, and the unexpected appearance of another magnetic order, occurring at T∗≈ 10 and 20 K for x= 0.05 and 0.10, respectively. We attribute the new magnetic transition at T∗, occurring well inside the SDW phase, to a reorganization of the Fermi surface due to Fe-to-Mn substitutions. These give rise to enhanced magnetic fluctuations along the incommensurate wavevector Q2= (π± δ, π± δ) , further increased by the RKKY interactions among Mn impurities., Scientific Reports, 11, ISSN:2045-2322
Published: 2021

12. The local structure and magnetic correlations in La(Fe1-Mn )AsO system

Author: Paolo Dore, Alberto Martinelli, G. Lamura, Naurang L. Saini, Eugenio Paris, Boby Joseph, Pietro Manfrinetti, K. Ozturk, Marina Putti, Giuliana Aquilanti, M. Y. Hacisalihoglu, Lara Simonelli, and A. Provino
Subjects: Superconductivity, Materials science, Extended X-ray absorption fine structure, Magnetic moment, Analytical chemistry, Iron-based pnictides, Local disorder, Substitution effect, 02 engineering and technology, General Chemistry, 010402 general chemistry, 021001 nanoscience & nanotechnology, Condensed Matter Physics, 01 natural sciences, Local structure, 0104 chemical sciences, General Materials Science, Emission spectrum, Gradual increase, 0210 nano-technology, Absorption (electromagnetic radiation), Néel temperature
Abstract: The local structure of La(Fe1-xMnx)AsO, showing suppression of long-range magnetic order by Mn-substitution, has been studied. Extended X-ray absorption fine structure (EXAFS) measurements at As K-edge and Fe K-edge are used to probe the atomic correlations in the FeAs-layer. We have found that both Fe-As and Fe-Fe bondlengths tend to increase with increasing Mn concentration. The associated mean square relative displacements (MSRD) reveal a gradual increase indicating increased local disorder in the FeAs-layer with Mn content. The results reveal that the FeAs-layer thickness, measured by the As-height (hAs) from the Fe-Fe plane, is correlated with the Neel temperature. Furthermore, Fe Kβ X-ray emission spectroscopy (XES) shows a sharp increase in the Fe local magnetic moment with Mn substitution. The importance of the FeAs layer thickness in describing magnetic correlations in La(Fe1−xMnx)AsO is discussed.
Published: 2019

13. Evidence for Longitudinal Homogeneity and No Je Degradation in Bi-2212 Wires Realized by the GDG Process

Author: Simon C. Hopkins, Amalia Ballarino, Carlo Ferdeghini, A. Leveratto, Luca Leoncino, Andrea Malagoli, Giuseppe Celentano, S. Chiarelli, and Marina Putti
Subjects: Fabrication, Materials science, Significant difference, Condensed Matter Physics, Inconel 625, 01 natural sciences, Electronic, Optical and Magnetic Materials, Overpressure, Magnetic field, 0103 physical sciences, Homogeneity (physics), Critical current, Electrical and Electronic Engineering, Composite material, 010306 general physics
Abstract: The GDG fabrication process developed at CNR-SPIN is a promising method for producing Bi-2212 wires without overpressure processing. In this paper, critical current measurements performed at ENEA on both short and long samples in magnetic fields up to 14 T are compared. The results show no significant difference in Je between short and long (∼1 m) samples, and suggest very good longitudinal uniformity, validating the effectiveness and scalability of the process. In addition, the suitability of Inconel 625 for reaction and test barrels is demonstrated, and the reasons for obtaining lower than expected absolute Je values are discussed.
Published: 2019

14. Tuning quantum phases in transition metal dichalcogenides via ionic liquid gating-induced protonation

Author: Erik Piatti, Giacomo, Prando, Gianrico, Lamura, Martina, Meinero, Montagna Bozzone, Jessica, Marina, Putti, Stefano, Roddaro, Toni, Shiroka, Pietro, Carretta, Gianni, Profeta, Dario Daghero, and Renato Gonnelli
Published: 2021

15. Mn substitution effect on the local structure of La(Fe

Author: Muammer Yasin Yasin, Hacisalihoglu, Laura, Simonelli, Carlo, Marini, Alessia, Provino, Alberto, Martinelli, Pietro, Manfrinetti, Marina, Putti, and Naurang Lal, Saini
Abstract: The local structure of La(Fe
Published: 2020

16. Uncollapsed LaFe2As2 phase: Compensated, highly doped, electron-phonon-coupled, iron-based superconductor

Author: Akira Iyo, Ilaria Pallecchi, Marina Putti, Hiraku Ogino, and Marco Affronte
Subjects: Superconductivity, Materials science, Physics and Astronomy (miscellaneous), Condensed matter physics, Doping, Electron phonon, 02 engineering and technology, Electron, 021001 nanoscience & nanotechnology, Coupling (probability), 01 natural sciences, Iron-based superconductor, Condensed Matter::Superconductivity, Phase (matter), 0103 physical sciences, General Materials Science, 010306 general physics, 0210 nano-technology, Pnictogen
Abstract: The recently discovered ${\mathrm{LaFe}}_{2}{\mathrm{As}}_{2}$ superconducting compound, member of the 122 family of iron pnictide superconductors, becomes superconducting below ${T}_{c}\ensuremath{\approx}13\phantom{\rule{0.16em}{0ex}}\mathrm{K}$, yet its nominal doping apparently places it in the extreme overdoped limit, where superconductivity should be suppressed. In this work, we investigate the normal state of magneto- and thermoelectric transport and specific heat of this compound. The experimental data are consistent with the presence of highly compensated electron and hole bands, with \ensuremath{\sim}0.42 electrons per unit cell just above ${T}_{\mathrm{c}}$, and high effective masses $\ensuremath{\sim}3{m}_{0}$. The temperature dependence of transport properties strongly resembles that of conventional superconductors, pointing to a key role of electron-phonon coupling. From this evidence, ${\mathrm{LaFe}}_{2}{\mathrm{As}}_{2}$ can be regarded as the connecting compound between unconventional and conventional superconductors.
Published: 2020

17. HE-LHC: The High-Energy Large Hadron Collider Future Circular Collider Conceptual Design Report Volume 4

Author: Pushpalatha C Bhat, B. Seeber, C. Pagliarone, Marco Statera, Victor P. Goncalves, Daria Astapovych, W. Bartmann, S. Iwamoto, M. Mentink, Alessandro Tricoli, E. R. Bielert, Laurent Chevalier, Patrick Koppenburg, Marco Calviani, C. Montag, P. Spiller, Jan Uythoven, P. Di Nezza, G. Guillermo Canton, B. Sailer, Markus Elsing, Sara Khatibi, Luca Vecchi, Luigi Palumbo, J. P. Penttinen, T. Podzorny, Maneesh Kumar, J. M. Rifflet, C. Kotnig, Jean Zinn-Justin, Christopher B. Verhaaren, A. Chernoded, Alessandro Bertarelli, L. M. Tkachenko, C. Koeberl, P. J. Mallon, M. Takeuchi, W. Venturini Delsolaro, G. Lamanna, S. Weinzierl, J. Gao, W. Kaabi, David D'Enterria, D. Barna, Paolo Castelnovo, Rajat Gupta, Oliver Boine-Frankenheim, Adarsh Pyarelal, Andreas Salzburger, Tessa Charles, M.E. Biagini, O. Panella, M. Stuart, A. Kollegger, V. Garcia Diaz, Olcay Bolukbasi, Maurizio Pierini, H. Aksakal, Tord Riemann, Abhishek M. Iyer, V. Shiltsev, D. Buttazzo, J. Blümlein, Prateek Agrawal, L. Sestini, Martin Bauer, Felicitas Pauss, S. Fiorendi, F. Bossu, Marco Nardecchia, C. Leonidopoulos, Wojciech Kotlarski, A. Saba, I. Bautista-Guzmán, W. Hillert, Giorgio Ambrosio, T. Lehtinen, Michael Andrew Parker, Silvia Taroni, Gian F. Giudice, Ph. Lebrun, Johann A. Briffa, T. Risselada, Giuseppe Lerner, A. Lechner, L. S. Miralles, M. Kuze, J. M. Valet, P. S. B. Dev, S. Holleis, Ph. Schwemling, M. Biglietti, S. Banerjee, Thomas Schörner-Sadenius, A. Sanz Ull, V. Tikhomirov, S. Savelyeva, Jiayin Gu, D. Zhou, Federico Ravotti, S. A. Bogacz, Daniele Mirarchi, R. Tomás García, Yann Coadou, F. Yu, Y. Cai, T. Lari, F. Holdener, D. Shwartz, C. Bhat, Ramesh Gupta, Markus Klute, E. Palmieri, P. Collier, Branislav Sitar, Yves Sirois, Livio Fanò, S. Rojas-Torres, E. Locci, Ruben Garcia Alia, I. Božović Jelisavić, R. Chehab, J. A. Aguilar-Saavedra, M. Pasquali, A. Di Cicco, Bernhard Auchmann, Klaus Heinemann, Alessia Tricomi, D. Lucchesi, B. Haerer, M. Morrone, Paolo Giacomelli, Sonia Carra, A. Senol, Ivan Koop, Luca Silvestrini, Anna Stakia, Heather Gray, E. Skordis, A. D. Kovalenko, Paul Langacker, R. Li, Bernardo Bordini, R. Rata, Arjan Verweij, Shehu S. AbdusSalam, Andrey Karyukhin, U. van Rienen, Gianluigi Arduini, Bernhard Holzer, S. A. Nikitin, S. S. Kozub, Satoshi Mishima, B. Di Micco, S. Izquierdo Bermudez, N. Pukhaeva, Nigel Watson, F. Prino, Jean-Michel Sallese, Sotirios Vlachos, Alessandro Vicini, A. Valassi, Daniel Treille, F. Dordei, A. M. Fernandez Navarro, B. Dziewit, Marcello Abbrescia, J. M. Hauptman, I. Chaikovska, Paolo Giubellino, Michael J. Baker, V.V. Kashikhin, Friedrich Lackner, Filippo Sala, A. Langner, D. Pulikowski, H. Eriksson, Matteo Turri, Andrea Wulzer, M. Aiba, Lisa Borgonovi, I. Morozov, V. Haurylavets, J. F. Croteau, S. Boselli, L. A. Gonzalez Gomez, Claudia Tambasco, F. Mahmoudi, Sébastien Descotes-Genon, A. Luciani, Pavel Piminov, M. Varasteh, T. Herzig, Sandra Aumon, Cristina Bernini, Joseph Bramante, Roberta Arnaldi, G. 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Gobbi, Michael Hance, A. J. Barr, V. Del Duca, V. Guzey, M. Pont, Michele Selvaggi, Oliver Brüning, J. Barreiro Guimarães da Costa, A. Drago, Y. Zhang, Giovanni Punzi, Viktor Matveev, Anadi Canepa, Clemens Lange, B. L. Militsyn, Martijn Mulders, Max Klein, V. D’Auria, M. Mylona, Valeria Braccini, S. DasBakshi, David Calvet, Sophia Borowka, David Marzocca, S. Jadach, A. A. Pankov, Christophe Ochando, A. A. Tudora, I. Masina, Jure Zupan, A. Preinerstorfer, Benjamin Fuks, H. K. Soltveit, G. Rolando, E.E. Perepelkin, T. G. Rizzo, Saleh Sultansoy, Federico Roncarolo, K. Elsener, R. Q. Pan, P. Zhuang, David Attié, Jac Perez, K. Kravalis, F. Anulli, V. Ruhlmann-Kleider, S. Malvezzi, Steffen A. Bass, E. La Francesca, Heinz Pernegger, K. Grzanka, M. T. Tiirakari, Alberto Ventura, Alessandro Cerri, Marco Peruzzi, Eric Montesinos, O. Etisken, F. Grancagnolo, S. Kartal, H. Humer, Oliver Fischer, M. Primavera, Marco Toliman Lucchini, P. Vedrine, Felix Kling, M. Altınlı, Sergio Calatroni, C. Han, Olivier Leroy, R. T. D’Agnolo, N. Klinkenberg, A. Audurier, Tatsushi Nakamoto, Ali Bozbey, Bernd A. Kniehl, Carl J. Debono, I. P. J. Shipsey, Gregorio Bernardi, Paolo Nason, William James Fawcett, J. M. Jiménez, D. Denisov, M. Serluca, David Curtin, Arif Akhundov, M. García Pérez, Iacopo Vivarelli, Emanuele Bacchiocchi, Markus Zerlauth, Julia Hrdinka, F. Butin, F. Müller, D. Tikhonov, Jorg Wenninger, A. Kilic, Fabrizio Ferro, J. Tanaka, S. A. Antipov, Miroslav Atanasov, S. Kuttimalai, A. Y. Starikov, F. R. Blánquez, S. V. Furuseth, G. Gaudio, L. Malgeri, J. Curti, B. Turbiarz, S. Li, A. Romanov, Costas G. Papadopoulos, Brennan Goddard, Frank Krauss, Lidija Zivkovic, Toms Torims, Michaela Lackner, D. A. Lyubimtsev, G. Borghello, J. F. Grosse-Oetringhaus, A. Bogomyagkov, H. Duran Yildiz, N. Foppiani, Arthur Schaffer, J. Zhou, D. Liberati, Vincenzo Guidi, Naeem A. Tahir, M. Besançon, Daniel Schoerling, Joe Incandela, Giacomo Polesello, O. Cakir, I. Ruehl, Ruggero Vaglio, Z. Zhang, Bruno Spataro, Davide Tommasini, F. Millet, H. D. Yoo, Carlo V. Fiorio, S. Deghaye, C. Bozzi, A. Shivaji, G. Corcella, I. Bellafont, Valentina Mariani, D. E. Martins, Michael Syphers, C. Hati, Peter Marquard, Nicola Bacchetta, Matthew Crouch, David Woog, Oliver Kortner, A. Milanese, Ricardo Gonçalo, Guido Montagna, Mikhail Zobov, F. Bedeschi, Eugene Bulyak, M. Aburaia, R. Tenchini, G. Marchiori, H. Rafique, G. Calderola, M. Antonello, Andrea Thamm, S. Glukhov, F. Hug, Robert Ruprecht, Veysi Erkcan Ozcan, K. Lee, Angelo Infantino, V. Makarenko, Z. Nergiz, Sergei Chekanov, Benjamin C. Allanach, C. Dachauer, H. Zhang, C. Biscari, A. J. Lankford, Scott Thomas, P. Kostka, Thomas Gehrmann, O. Azzolini, M. Ploskon, S. F. Ge, K. Oide, Andrea Bastianin, Daniela Bortoletto, Ingo Schienbein, J. L. Biarrotte, M. van Leeuwen, D. Stöckinger, Harald Ita, J. Katharina Behr, A. Cholakian, T. Kwon, L. Medina, Evgeny Starchenko, G. Mancinelli, L. Zanotto, F. Menez, L. Bellagamba, J. P. 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Béguin, Roberto Cardarelli, C. Milardi, G. Tassielli, Mario Campanelli, P. Fabbricatore, R. Rossmanith, Piergiulio Lenzi, D. P. Missiaen, R. Patterson, Sigve Haug, A. Farilla, Guilherme Milhano, D. El Khechen, Freya Blekman, O. B. Malyshev, Carlo Ferdeghini, A. Hannah, Michael Benedikt, E. Logothetis Agaliotis, M. Prausa, Maurizio Vignolo, M. Drewes, F. Marhauser, A. Ivanovs, M. Widorski, E. Santopinto, Javier Munilla, V. Mertens, Filip Moortgat, Salim Ogur, Michaela Schaumann, O. Rios Rubiras, Carsten Welsch, Fady Bishara, Michael Plagge, M. Czech, Giuseppe Iacobucci, I. Crespo Garrido, W. Dallapiazza, A. Moros, Wieslaw Placzek, A. E. Rentería-Olivo, M. Saito, H. U. Wienands, O. Verwilligen, L. Spallino, W. Snoeys, L. Duarte, A. Massimiliano, Greg Landsberg, Z. Liu, A. Ozansoy, Antonella Sciuto, T. Boccali, R. B. Appleby, M. Antonelli, J. A. Netto, Y. Nie, Johannes Gutleber, M. Skrzypek, N. Vignaroli, P. J. Clark, Emilio Bellingeri, Bennie F.L. Ward, P. Roloff, E. Perez Codina, Roman Martin, Elias Metral, B. Hegner, L. Zawiejski, Efe Yazgan, F. Couderc, G. Tonelli, G. Castorina, Patrizia Azzi, A. De Roeck, Jean-Philippe Lansberg, Riccardo Valente, A. David, F. Robert, Jeremi Niedziela, Anna Grassellino, Marie-Hélène Genest, V. Tisserand, A. Kilpinen, Y. K. Kim, A. Dominjon, Andrej Arbuzov, David Amorim, L. Kretzschmar, E. Bruna, Sergey Polozov, Vyacheslav Klyukhin, Hubert Kroha, O. Amstutz, A. Vitrano, Raymond Veness, Tilman Plehn, M. A. Mahmoud, Uşak Üniversitesi, Fen Edebiyat Fakültesi, Fizik Bölümü, FCC Collaboration (Ukupan broj autora: 1363), FCC Collaboration, Abada, A., Abbrescia, M., Abdussalam, S. S., Abdyukhanov, I., Abelleira Fernandez, J., Abramov, A., Aburaia, M., Acar, A. O., Adzic, P. R., Agrawal, P., Aguilar-Saavedra, J. A., Aguilera-Verdugo, J. J., Aiba, M., Aichinger, I., Aielli, G., Akay, A., Akhundov, A., Aksakal, H., Albacete, J. L., Albergo, S., Alekou, A., Aleksa, M., Aleksan, R., Alemany Fernandez, R. M., Alexahin, Y., Alia, R. G., Alioli, S., Alipour Tehrani, N., Allanach, B. C., Allport, P. P., Altinli, M., Altmannshofer, W., Ambrosio, G., Amorim, D., Amstutz, O., Anderlini, L., Andreazza, A., Andreini, M., Andriatis, A., Andris, C., Andronic, A., Angelucci, M., Antinori, F., Antipov, S. A., Antonelli, M., Antonello, M., Antonioli, P., Antusch, S., Anulli, F., Apolinario, L., Apollinari, G., Apollonio, A., Appelo, D., Appleby, R. B., Apyan, A., Arbey, A., Arbuzov, A., Arduini, G., Ari, V., Arias, S., Armesto, N., Arnaldi, R., Arsenyev, S. A., Arzeo, M., Asai, S., Aslanides, E., Assmann, R. W., Astapovych, D., Atanasov, M., Atieh, S., Attie, D., Auchmann, B., Audurier, A., Aull, S., Aumon, S., Aune, S., Avino, F., Avrillaud, G., Aydin, G., Azatov, A., Azuelos, G., Azzi, P., Azzolini, O., Azzurri, P., Bacchetta, N., Bacchiocchi, E., Bachacou, H., Baek, Y. W., Baglin, V., Bai, Y., Baird, S., Baker, M. J., Baldwin, M. J., Ball, A. H., Ballarino, A., Banerjee, S., Barber, D. P., Barducci, D., Barjhoux, P., Barna, D., Barnafoldi, G. G., Barnes, M. J., Barr, A., Barranco Garcia, J., Barreiro Guimaraes da Costa, J., Bartmann, W., Baryshevsky, V., Barzi, E., Bass, S. A., Bastianin, A., Baudouy, B., Bauer, F., Bauer, M., Baumgartner, T., Bautista-Guzman, I., Bayindir, C., Beaudette, F., Bedeschi, F., Beguin, M., Bellafont, I., Bellagamba, L., Bellegarde, N., Belli, E., Bellingeri, E., Bellini, F., Bellomo, G., Belomestnykh, S., Bencivenni, G., Benedikt, M., Bernardi, G., Bernardi, J., Bernet, C., Bernhardt, J. M., Bernini, C., Berriaud, C., Bertarelli, A., Bertolucci, S., Besana, M. I., Besancon, M., Beznosov, O., Bhat, P., Bhat, C., Biagini, M. E., Biarrotte, J. -L., Bibet Chevalier, A., Bielert, E. R., Biglietti, M., Bilei, G. M., Bilki, B., Biscari, C., Bishara, F., Blanco-Garcia, O. R., Blanquez, F. R., Blekman, F., Blondel, A., Blumlein, J., Boccali, T., Boels, R., Bogacz, S. A., Bogomyagkov, A., Boine-Frankenheim, O., Boland, M. 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J., Coadou, Y., Cobal, M., Coccaro, A., Cogan, J., Cogneras, E., Collamati, F., Colldelram, C., Collier, P., Collot, J., Contino, R., Conventi, F., Cook, C. T. A., Cooley, L., Corcella, G., Cornell, A. S., Corral, G. H., Correia-Rodrigues, H., Costanza, F., Costa Pinto, P., Couderc, F., Coupard, J., Craig, N., Crespo Garrido, I., Crivellin, A., Croteau, J. F., Crouch, M., Cruz Alaniz, E., Cure, B., Curti, J., Curtin, D., Czech, M., Dachauer, C., D'Agnolo, R. T., Daibo, M., Dainese, A., Dalena, B., Daljevec, A., Dallapiazza, W., D'Aloia Schwartzentruber, L., Dam, M., D'Ambrosio, G., Das, S. P., Dasbakshi, S., da Silva, W., da Silveira, G. G., D'Auria, V., D'Auria, S., David, A., Davidek, T., Deandrea, A., de Blas, J., Debono, C. J., De Curtis, S., De Filippis, N., de Florian, D., Deghaye, S., de Jong, S. J., Del Bo, C., Del Duca, V., Delikaris, D., Deliot, F., Dell'Acqua, A., Delle Rose, L., Delmastro, M., De Lucia, E., Demarteau, M., Denegri, D., Deniau, L., Denisov, D., Denizli, H., Denner, A., D'Enterria, D., de Rijk, G., De Roeck, A., Derue, F., Deschamps, O., Descotes-Genon, S., Dev, P. S. B., de Vivie de Regie, J. B., Dewanjee, R. K., Di Ciaccio, A., Di Cicco, A., Dillon, B. M., Di Micco, B., Di Nezza, P., Di Vita, S., Doblhammer, A., Dominjon, A., D'Onofrio, M., Dordei, F., Drago, A., Draper, P., Drasal, Z., Drewes, M., Duarte, L., Dubovyk, I., Duda, P., Dudarev, A., Dudko, L., Duellmann, D., Dunser, M., du Pree, T., Durante, M., Duran Yildiz, H., Dutta, S., Duval, F., Duval, J. M., Dydyshka, Y., Dziewit, B., Eisenhardt, S., Eisterer, M., Ekelof, T., El Khechen, D., Ellis, S. A., Ellis, J., Ellison, J. A., Elsener, K., Elsing, M., Enari, Y., Englert, C., Eriksson, H., Eskola, K. J., Esposito, L. S., Etisken, O., Etzion, E., Fabbricatore, P., Falkowski, A., Falou, A., Faltova, J., Fan, J., Fano, L., Farilla, A., Farinelli, R., Farinon, S., Faroughy, D. A., Fartoukh, S. D., Faus-Golfe, A., Fawcett, W. J., Felici, G., Felsberger, L., Ferdeghini, C., Fernandez Navarro, A. M., Fernandez-Tellez, A., Ferradas Troitino, J., Ferrara, G., Ferrari, R., Ferreira, L., Ferreira da Silva, P., Ferrera, G., Ferro, F., Fiascaris, M., Fiorendi, S., Fiorio, C., Fischer, O., Fischer, E., Flieger, W., Florio, M., Fonnesu, D., Fontanesi, E., Foppiani, N., Foraz, K., Forkel-Wirth, D., Forte, S., Fouaidy, M., Fournier, D., Fowler, T., Fox, J., Francavilla, P., Franceschini, R., Franchino, S., Franco, E., Freitas, A., Fuks, B., Furukawa, K., Furuseth, S. V., Gabrielli, E., Gaddi, A., Galanti, M., Gallo, E., Ganjour, S., Gao, J., Garcia Diaz, V., Garcia Perez, M., Garcia Tabares, L., Garion, C., Garzelli, M. V., Garzia, I., Gascon-Shotkin, S. M., Gaudio, G., Gay, P., Ge, S. -F., Gehrmann, T., Genest, M. H., Gerard, R., Gerigk, F., Gerwig, H., Giacomelli, P., Giagu, S., Gianfelice-Wendt, E., Gianotti, F., Giffoni, F., Gilardoni, S. S., Gil Costa, M., Giovannetti, M., Giovannozzi, M., Giubellino, P., Giudice, G. F., Giunta, A., Gladilin, L. K., Glukhov, S., Gluza, J., Gobbi, G., Goddard, B., Goertz, F., Golling, T., Goncalves, V. P., Goncalo, R., Gonzalez Gomez, L. A., Gorgi Zadeh, S., Gorine, G., Gorini, E., Gourlay, S. A., Gouskos, L., Grancagnolo, F., Grassellino, A., Grau, A., Graverini, E., Gray, H. M., Greco, M., Grenard, J. -L., Grimm, O., Grojean, C., Gromov, V. A., Grosse-Oetringhaus, J. F., Grudiev, A., Grzanka, K., Gu, J., Guadagnoli, D., Guidi, V., Guiducci, S., Guillermo Canton, G., Gunaydin, Y. O., Gupta, R., Gupta, R. S., Gutierrez, J., Gutleber, J., Guyot, C., Guzey, V., Gwenlan, C., Haberstroh, C., Hacisahinoglu, B., Haerer, B., Hahn, K., Hahn, T., Hammad, A., Han, C., Hance, M., Hannah, A., Harris, P. C., Hati, C., Haug, S., Hauptman, J., Haurylavets, V., He, H. -J., Hegglin, A., Hegner, B., Heinemann, K., Heinemeyer, S., Helsens, C., Henriques, A., Hernandez, P., Hernandez-Pinto, R. J., Hernandez-Sanchez, J., Herzig, T., Hiekkanen, I., Hillert, W., Hoehn, T., Hofer, M., Hofle, W., Holdener, F., Holleis, S., Holzer, B., Hong, D. K., Honorato, C. G., Hopkins, S. C., Hrdinka, J., Hug, F., Humann, B., Humer, H., Hurth, T., Hutton, A., Iacobucci, G., Ibarrola, N., Iconomidou-Fayard, L., Ilyina-Brunner, K., Incandela, J., Infantino, A., Ippolito, V., Ishino, M., Islam, R., Ita, H., Ivanovs, A., Iwamoto, S., Iyer, A., Izquierdo Bermudez, S., Jadach, S., Jamin, D. O., Janot, P., Jarry, P., Jeff, A., Jenny, P., Jensen, E., Jensen, M., Jiang, X., Jimenez, J. M., Jones, M. A., Jones, O. R., Jowett, J. M., Jung, S., Kaabi, W., Kado, M., Kahle, K., Kalinovskaya, L., Kalinowski, J., Kamenik, J. F., Kannike, K., Kara, S. O., Karadeniz, H., Karaventzas, V., Karpov, I., Kartal, S., Karyukhin, A., Kashikhin, V., Katharina Behr, J., Kaya, U., Keintzel, J., Keinz, P. A., Keppel, K., Kersevan, R., Kershaw, K., Khanpour, H., Khatibi, S., Khatiri Yanehsari, M., Khoze, V. V., Kieseler, J., Kilic, A., Kilpinen, A., Kim, Y. -K., Kim, D. W., Klein, U., Klein, M., Kling, F., Klinkenberg, N., Kloppel, S., Klute, M., Klyukhin, V. I., Knecht, M., Kniehl, B., Kocak, F., Koeberl, C., Kolano, A. M., Kollegger, A., Kolodziej, K., Kolomiets, A. A., Komppula, J., Koop, I., Koppenburg, P., Koratzinos, M., Kordiaczynska, M., Korjik, M., Kortner, O., Kostka, P., Kotlarski, W., Kotnig, C., Kottig, T., Kotwal, A. V., Kovalenko, A. D., Kowalski, S., Kozaczuk, J., Kozlov, G. A., Kozub, S. S., Krainer, A. M., Kramer, T., Kramer, M., Krammer, M., Krasnov, A. A., Krauss, F., Kravalis, K., Kretzschmar, L., Kriske, R. 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A., Mahmoudi, F., Maitre, J., Makarenko, V., Malagoli, A., Malcles, J., Malgeri, L., Mallon, P. J., Maltoni, F., Malvezzi, S., Malyshev, O. B., Mancinelli, G., Mandrik, P., Manfrinetti, P., Mangano, M., Manil, P., Mannelli, M., Marchiori, G., Marhauser, F., Mariani, V., Marinozzi, V., Mariotto, S., Marquard, P., Marquet, C., Marriott-Dodington, T., Martin, R., Martin, O., Martin Camalich, J., Martinez, T., Martinez Bruzual, H., Martinez-Hernandez, M. I., Martins, D. E., Marzani, S., Marzocca, D., Marzola, L., Masciocchi, S., Masina, I., Massimiliano, A., Massironi, A., Masubuchi, T., Matveev, V. A., Mazzoni, M. A., Mccullough, M., Mcintosh, P. A., Meade, P., Medina, L., Meier, A., Meignan, J., Mele, B., Mendes Saraiva, J. G., Menez, F., Mentink, M., Meoni, E., Meridiani, P., Merk, M., Mermod, P., Mertens, V., Mether, L., Metral, E., Migliorati, M., Milanese, A., Milardi, C., Milhano, G., Militsyn, B. L., Millet, F., Minashvili, I., Minervini, J. V., Miralles, L. 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A., Okumura, Y., Oleari, C., Olness, F. I., Onel, Y., Ortino, M., Osborne, J., Osland, P., Otto, T., Oyulmaz, K. Y., Ozansoy, A., Ozcan, V., Ozdemir, K., Pagliarone, C. E., Pais da Silva, H. F., Palmieri, E., Palumbo, L., Pampaloni, A., Pan, R. -Q., Panareo, M., Panella, O., Panico, G., Panizzo, G., Pankov, A. A., Pantsyrny, V., Papadopoulos, C. G., Papaefstathiou, A., Papaphilippou, Y., Parker, M. A., Parma, V., Pasquali, M., Patra, S. K., Patterson, R., Paukkunen, H., Pauss, F., Peggs, S., Penttinen, J. -P., Peon, G., Perepelkin, E. E., Perez, E., Perez, J. C., Perez, G., Perez, F., Perez Codina, E., Perez Morales, J., Perfilov, M., Pernegger, H., Peruzzi, M., Pes, C., Peters, K., Petracca, S., Petriello, F., Pezzotti, L., Pfeiffer, S., Piccinini, F., Pieloni, T., Pierini, M., Pikhartova, H., Pikurs, G., Pilicer, E., Piminov, P., Pira, C., Pittau, R., Placzek, W., Plagge, M., Plehn, T., Pleier, M. -A., Ploskon, M., Podeur, M., Podlech, H., Podzorny, T., Poggioli, L., Poiron, A., Polesello, G., Poli Lener, M., Polini, A., Polinski, J., Polozov, S. M., Ponce, L., Pont, M., Pontecorvo, L., Portaluri, T., Potamianos, K., Prasse, C., Prausa, M., Preinerstorfer, A., Premat, E., Price, T., Primavera, M., Prino, F., Prioli, M., Proudfoot, J., Provino, A., Pugnat, T., Pukhaeva, N., Pulawski, S., Pulikowski, D., Punzi, G., Putti, M., Pyarelal, A., Quack, H., Quispe, M., Racioppi, A., Rafique, H., Raginel, V., Raidal, M., Ramirez-Uribe, N. S., Ramsey-Musolf, M. J., Rata, R., Ratoff, P., Ravotti, F., Rebello Teles, P., Reboud, M., Redaelli, S., Renner, E., Renteria-Olivo, A. E., Rescigno, M., Reuter, J., Ribon, A., Ricci, A. M., Riegler, W., Riemann, S., Riemann, B., Riemann, T., Rifflet, J. M., Rimmer, R. A., Rinaldesi, R., Rinolfi, L., Rios Rubiras, O., Risselada, T., Rivetti, A., Rivkin, L., Rizzo, T., Robens, T., Robert, F., Robson, A. J., Rochepault, E., Roda, C., Rodrigo, G., Rodriguez-Cahuantzi, M., Rogan, C., Roig, M., Rojas-Torres, S., Rojo, J., Rolandi, G., Rolando, G., Roloff, P., Romanenko, A., Romanov, A., Roncarolo, F., Rosado Sanchez, A., Rosaz, G., Rossi, L., Rossi, A., Rossmanith, R., Rousset, B., Royon, C., Ruan, X., Ruehl, I., Ruhlmann-Kleider, V., Ruiz, R., Rumyantsev, L., Ruprecht, R., Ryazanov, A. I., Saba, A., Sadykov, R., Saez de Jauregui, D., Sahin, M., Sailer, B., Saito, M., Sala, F., Salam, G. P., Salfeld-Nebgen, J., Salgado, C. A., Salini, S., Sallese, J. M., Salmi, T., Salzburger, A., Sampayo, O. 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Zurita, J, Işık Üniversitesi, Mühendislik Fakültesi, İnşaat Mühendisliği Bölümü, Işık University, Faculty of Engineering, Department of Civil Engineering, Bayındır, Cihan, Universitat Politècnica de Catalunya. Departament de Teoria del Senyal i Comunicacions, Universitat Politècnica de Catalunya. RF&MW - Grup de Recerca de sistemes, dispositius i materials de RF i microones, Abada A., Abbrescia M., AbdusSalam S.S., Abdyukhanov I., Abelleira Fernandez J., Abramov A., Aburaia M., Acar A.O., Adzic P.R., Agrawal P., Aguilar-Saavedra J.A., Aguilera-Verdugo J.J., Aiba M., Aichinger I., Aielli G., Akay A., Akhundov A., Aksakal H., Albacete J.L., Albergo S., Alekou A., Aleksa M., Aleksan R., Alemany Fernandez R.M., Alexahin Y., Alia R.G., Alioli S., Alipour Tehrani N., Allanach B.C., Allport P.P., Altinli M., Altmannshofer W., Ambrosio G., Amorim D., Amstutz O., Anderlini L., Andreazza A., Andreini M., Andriatis A., Andris C., Andronic A., Angelucci M., Antinori F., Antipov S.A., Antonelli M., Antonello M., Antonioli P., Antusch S., Anulli F., Apolinario L., Apollinari G., Apollonio A., Appelo D., Appleby R.B., Apyan A., Arbey A., Arbuzov A., Arduini G., Ari V., Arias S., Armesto N., Arnaldi R., Arsenyev S.A., Arzeo M., Asai S., Aslanides E., Assmann R.W., Astapovych D., Atanasov M., Atieh S., Attie D., Auchmann B., Audurier A., Aull S., Aumon S., Aune S., Avino F., Avrillaud G., Aydin G., Azatov A., Azuelos G., Azzi P., Azzolini O., Azzurri P., Bacchetta N., Bacchiocchi E., Bachacou H., Baek Y.W., Baglin V., Bai Y., Baird S., Baker M.J., Baldwin M.J., Ball A.H., Ballarino A., Banerjee S., Barber D.P., Barducci D., Barjhoux P., Barna D., Barnafoldi G.G., Barnes M.J., Barr A., Barranco Garcia J., Barreiro Guimaraes da Costa J., Bartmann W., Baryshevsky V., Barzi E., Bass S.A., Bastianin A., Baudouy B., Bauer F., Bauer M., Baumgartner T., Bautista-Guzman I., Bayindir C., Beaudette F., Bedeschi F., Beguin M., Bellafont I., Bellagamba L., Bellegarde N., Belli E., Bellingeri E., Bellini F., Bellomo G., Belomestnykh S., Bencivenni G., Benedikt M., Bernardi G., Bernardi J., Bernet C., Bernhardt J.M., Bernini C., Berriaud C., Bertarelli A., Bertolucci S., Besana M.I., Besancon M., Beznosov O., Bhat P., Bhat C., Biagini M.E., Biarrotte J.-L., Bibet Chevalier A., Bielert E.R., Biglietti M., Bilei G.M., Bilki B., Biscari C., Bishara F., Blanco-Garcia O.R., Blanquez F.R., Blekman F., Blondel A., Blumlein J., Boccali T., Boels R., Bogacz S.A., Bogomyagkov A., Boine-Frankenheim O., Boland M.J., Bologna S., Bolukbasi O., Bomben M., Bondarenko S., Bonvini M., Boos E., Bordini B., Bordry F., Borghello G., Borgonovi L., Borowka S., Bortoletto D., Boscherini D., Boscolo M., Boselli S., Bosley R.R., Bossu F., Botta C., Bottura L., Boughezal R., Boutin D., Bovone G., Bozovic Jelisavic I., Bozbey A., Bozzi C., Bozzini D., Braccini V., Braibant-Giacomelli S., Bramante J., Braun-Munzinger P., Briffa J.A., Britzger D., Brodsky S.J., Brooke J.J., Bruce R., Bruckman De Renstrom P., Bruna E., Bruning O., Brunner O., Brunner K., Bruzzone P., Buffat X., Bulyak E., Burkart F., Burkhardt H., Burnet J.-P., Butin F., Buttazzo D., Butterworth A., Caccia M., Cai Y., Caiffi B., Cairo V., Cakir O., Calaga R., Calatroni S., Calderini G., Calderola G., Caliskan A., Calvet D., Calviani M., Camalich J.M., Camarri P., Campanelli M., Camporesi T., Canbay A.C., Canepa A., Cantergiani E., Cantore-Cavalli D., Capeans M., Cardarelli R., Cardella U., Cardini A., Carloni Calame C.M., Carra F., Carra S., Carvalho A., Casalbuoni S., Casas J., Cascella M., Castelnovo P., Castorina G., Catalano G., Cavasinni V., Cazzato E., Cennini E., Cerri A., Cerutti F., Cervantes J., Chaikovska I., Chakrabortty J., Chala M., Chamizo-Llatas M., Chanal H., Chanal D., Chance S., Chance A., Charitos P., Charles J., Charles T.K., Chattopadhyay S., Chehab R., Chekanov S.V., Chen N., Chernoded A., Chetvertkova V., Chevalier L., Chiarelli G., Chiarello G., Chiesa M., Chiggiato P., Childers J.T., Chmielinska A., Cholakian A., Chomaz P., Chorowski M., Chou W., Chrzaszcz M., Chyhyrynets E., Cibinetto G., Ciftci A.K., Ciftci R., Cimino R., Ciuchini M., Clark P.J., Coadou Y., Cobal M., Coccaro A., Cogan J., Cogneras E., Collamati F., Colldelram C., Collier P., Collot J., Contino R., Conventi F., 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Vita S., Doblhammer A., Dominjon A., D'Onofrio M., Dordei F., Drago A., Draper P., Drasal Z., Drewes M., Duarte L., Dubovyk I., Duda P., Dudarev A., Dudko L., Duellmann D., Dunser M., du Pree T., Durante M., Duran Yildiz H., Dutta S., Duval F., Duval J.M., Dydyshka Y., Dziewit B., Eisenhardt S., Eisterer M., Ekelof T., El Khechen D., Ellis S.A., Ellis J., Ellison J.A., Elsener K., Elsing M., Enari Y., Englert C., Eriksson H., Eskola K.J., Esposito L.S., Etisken O., Etzion E., Fabbricatore P., Falkowski A., Falou A., Faltova J., Fan J., Fano L., Farilla A., Farinelli R., Farinon S., Faroughy D.A., Fartoukh S.D., Faus-Golfe A., Fawcett W.J., Felici G., Felsberger L., Ferdeghini C., Fernandez Navarro A.M., Fernandez-Tellez A., Ferradas Troitino J., Ferrara G., Ferrari R., Ferreira L., Ferreira da Silva P., Ferrera G., Ferro F., Fiascaris M., Fiorendi S., Fiorio C., Fischer O., Fischer E., Flieger W., Florio M., Fonnesu D., Fontanesi E., Foppiani N., Foraz K., Forkel-Wirth D., Forte S., Fouaidy M., Fournier D., Fowler T., Fox J., Francavilla P., Franceschini R., Franchino S., Franco E., Freitas A., Fuks B., Furukawa K., Furuseth S.V., Gabrielli E., Gaddi A., Galanti M., Gallo E., Ganjour S., Gao J., Garcia Diaz V., Garcia Perez M., Garcia Tabares L., Garion C., Garzelli M.V., Garzia I., Gascon-Shotkin S.M., Gaudio G., Gay P., Ge S.-F., Gehrmann T., Genest M.H., Gerard R., Gerigk F., Gerwig H., Giacomelli P., Giagu S., Gianfelice-Wendt E., Gianotti F., Giffoni F., Gilardoni S.S., Gil Costa M., Giovannetti M., Giovannozzi M., Giubellino P., Giudice G.F., Giunta A., Gladilin L.K., Glukhov S., Gluza J., Gobbi G., Goddard B., Goertz F., Golling T., Goncalves V.P., Goncalo R., Gonzalez Gomez L.A., Gorgi Zadeh S., Gorine G., Gorini E., Gourlay S.A., Gouskos L., Grancagnolo F., Grassellino A., Grau A., Graverini E., Gray H.M., Greco M., Grenard J.-L., Grimm O., Grojean C., Gromov V.A., Grosse-Oetringhaus J.F., Grudiev A., Grzanka K., Gu J., Guadagnoli D., Guidi V., Guiducci S., Guillermo Canton G., Gunaydin Y.O., Gupta R., Gupta R.S., Gutierrez J., Gutleber J., Guyot C., Guzey V., Gwenlan C., Haberstroh C., Hacisahinoglu B., Haerer B., Hahn K., Hahn T., Hammad A., Han C., Hance M., Hannah A., Harris P.C., Hati C., Haug S., Hauptman J., Haurylavets V., He H.-J., Hegglin A., Hegner B., Heinemann K., Heinemeyer S., Helsens C., Henriques A., Hernandez P., Hernandez-Pinto R.J., Hernandez-Sanchez J., Herzig T., Hiekkanen I., Hillert W., Hoehn T., Hofer M., Hofle W., Holdener F., Holleis S., Holzer B., Hong D.K., Honorato C.G., Hopkins S.C., Hrdinka J., Hug F., Humann B., Humer H., Hurth T., Hutton A., Iacobucci G., Ibarrola N., Iconomidou-Fayard L., Ilyina-Brunner K., Incandela J., Infantino A., Ippolito V., Ishino M., Islam R., Ita H., Ivanovs A., Iwamoto S., Iyer A., Izquierdo Bermudez S., Jadach S., Jamin D.O., Janot P., Jarry P., Jeff A., Jenny P., Jensen E., Jensen M., Jiang X., Jimenez J.M., Jones M.A., Jones O.R., Jowett J.M., Jung S., Kaabi W., Kado M., Kahle K., Kalinovskaya L., Kalinowski J., Kamenik J.F., Kannike K., Kara S.O., Karadeniz H., Karaventzas V., Karpov I., Kartal S., Karyukhin A., Kashikhin V., Katharina Behr J., Kaya U., Keintzel J., Keinz P.A., Keppel K., Kersevan R., Kershaw K., Khanpour H., Khatibi S., Khatiri Yanehsari M., Khoze V.V., Kieseler J., Kilic A., Kilpinen A., Kim Y.-K., Kim D.W., Klein U., Klein M., Kling F., Klinkenberg N., Kloppel S., Klute M., Klyukhin V.I., Knecht M., Kniehl B., Kocak F., Koeberl C., Kolano A.M., Kollegger A., Kolodziej K., Kolomiets A.A., Komppula J., Koop I., Koppenburg P., Koratzinos M., Kordiaczynska M., Korjik M., Kortner O., Kostka P., Kotlarski W., Kotnig C., Kottig T., Kotwal A.V., Kovalenko A.D., Kowalski S., Kozaczuk J., Kozlov G.A., Kozub S.S., Krainer A.M., Kramer T., Kramer M., Krammer M., Krasnov A.A., Krauss F., Kravalis K., Kretzschmar L., Kriske R.M., Kritscher H., Krkotic P., Kroha H., Kucharczyk M., Kuday S., Kuendig A., Kuhlmann G., Kulesza A., Kumar M., Kusina A., Kuttimalai S., Kuze M., Kwon T., Lackner F., Lackner M., La Francesca E., Laine M., Lamanna G., La Mendola S., Lancon E., Landsberg G., Langacker P., Lange C., Langner A., Lankford A.J., Lansberg J.P., Lari T., Laycock P.J., Lebrun P., Lechner A., Lee K., Lee S., Lee R., Lefevre T., Le Guen P., Lehtinen T., Leith S.B., Lenzi P., Leogrande E., Leonidopoulos C., Leon-Monzon I., Lerner G., Leroy O., Lesiak T., Levai P., Leveratto A., Levichev E., Li G., Li S., Li R., Liberati D., Liepe M., Lissauer D.A., Liu Z., Lobko A., Locci E., Logothetis Agaliotis E., Lombardo M.P., Long A.J., Lorin C., Losito R., Louzguiti A., Low I., Lucchesi D., Lucchini M.T., Luciani A., Lueckhof M., Lunt A.J.G., Luzum M., Lyubimtsev D.A., Maggiora M., Magnin N., Mahmoud M.A., Mahmoudi F., Maitre J., Makarenko V., Malagoli A., Malcles J., Malgeri L., Mallon P.J., Maltoni F., Malvezzi S., Malyshev O.B., Mancinelli G., Mandrik P., Manfrinetti P., Mangano M., Manil P., Mannelli M., Marchiori G., Marhauser F., Mariani V., Marinozzi V., Mariotto S., Marquard P., Marquet C., Marriott-Dodington T., Martin R., Martin O., Martin Camalich J., Martinez T., Martinez Bruzual H., Martinez-Hernandez M.I., Martins D.E., Marzani S., Marzocca D., Marzola L., Masciocchi S., Masina I., Massimiliano A., Massironi A., Masubuchi T., Matveev V.A., Mazzoni M.A., McCullough M., McIntosh P.A., Meade P., Medina L., Meier A., Meignan J., Mele B., Mendes Saraiva J.G., Menez F., Mentink M., Meoni E., Meridiani P., Merk M., Mermod P., Mertens V., Mether L., Metral E., Migliorati M., Milanese A., Milardi C., Milhano G., Militsyn B.L., Millet F., Minashvili I., Minervini J.V., Miralles L.S., Mirarchi D., Mishima S., Missiaen D.P., Mitselmakher G., Mitshuhashi T., Mnich J., Mohammadi Najafabadi M., Mohapatra R.N., Mokhov N., Molson J.G., Monge R., Montag C., Montagna G., Monteil S., Montenero G., Montesinos E., Moortgat F., Morange N., Morello G., Moreno Llacer M., Moretti M., Moretti S., Morley A.K., Moros A., Morozov I., Morretta V., Morrone M., Mostacci A., Muanza S., Muchnoi N., Muhlegger M., Mulder M., Mulders M., Muller B., Muller F., Muller A.-S., Munilla J., Murray M.J., Muttoni Y., Myers S., Mylona M., Nachtman J., Nakamoto T., Nardecchia M., Nardini G., Nason P., Nergiz Z., Nesterenko A.V., Netto J.A., Nettstrater A., Neubuser C., Neundorf J., Niccoli F., Nicrosini O., Nie Y., Niedermayer U., Niedziela J., Niemi A., Nikitin S.A., Nisati A., No J.M., Nonis M., Nosochkov Y., Novak M., Novokhatski A., O'Callaghan J.M., Ochando C., Ogur S., Ohmi K., Oide K., Okorokov V.A., Okumura Y., Oleari C., Olness F.I., Onel Y., Ortino M., Osborne J., Osland P., Otto T., Oyulmaz K.Y., Ozansoy A., Ozcan V., Ozdemir K., Pagliarone C.E., Pais da Silva H.F., Palmieri E., Palumbo L., Pampaloni A., Pan R.-Q., Panareo M., Panella O., Panico G., Panizzo G., Pankov A.A., Pantsyrny V., Papadopoulos C.G., Papaefstathiou A., Papaphilippou Y., Parker M.A., Parma V., Pasquali M., Patra S.K., Patterson R., Paukkunen H., Pauss F., Peggs S., Penttinen J.-P., Peon G., Perepelkin E.E., Perez E., Perez J.C., Perez G., Perez F., Perez Codina E., Perez Morales J., Perfilov M., Pernegger H., Peruzzi M., Pes C., Peters K., Petracca S., Petriello F., Pezzotti L., Pfeiffer S., Piccinini F., Pieloni T., Pierini M., Pikhartova H., Pikurs G., Pilicer E., Piminov P., Pira C., Pittau R., Placzek W., Plagge M., Plehn T., Pleier M.-A., Ploskon M., Podeur M., Podlech H., Podzorny T., Poggioli L., Poiron A., Polesello G., Poli Lener M., Polini A., Polinski J., Polozov S.M., Ponce L., Pont M., Pontecorvo L., Portaluri T., Potamianos K., Prasse C., Prausa M., Preinerstorfer A., Premat E., Price T., Primavera M., Prino F., Prioli M., Proudfoot J., Provino A., Pugnat T., Pukhaeva N., Pulawski S., Pulikowski D., Punzi G., Putti M., Pyarelal A., Quack H., Quispe M., Racioppi A., Rafique H., Raginel V., Raidal M., Ramirez-Uribe N.S., Ramsey-Musolf M.J., Rata R., Ratoff P., Ravotti F., Rebello Teles P., Reboud M., Redaelli S., Renner E., Renteria-Olivo A.E., Rescigno M., Reuter J., Ribon A., Ricci A.M., Riegler W., Riemann S., Riemann B., Riemann T., Rifflet J.M., Rimmer R.A., Rinaldesi R., Rinolfi L., Rios Rubiras O., Risselada T., Rivetti A., Rivkin L., Rizzo T., Robens T., Robert F., Robson A.J., Rochepault E., Roda C., Rodrigo G., Rodriguez-Cahuantzi M., Rogan C., Roig M., Rojas-Torres S., Rojo J., Rolandi G., Rolando G., Roloff P., Romanenko A., Romanov A., Roncarolo F., Rosado Sanchez A., Rosaz G., Rossi L., Rossi A., Rossmanith R., Rousset B., Royon C., Ruan X., Ruehl I., Ruhlmann-Kleider V., Ruiz R., Rumyantsev L., Ruprecht R., Ryazanov A.I., Saba A., Sadykov R., Saez de Jauregui D., Sahin M., Sailer B., Saito M., Sala F., Salam G.P., Salfeld-Nebgen J., Salgado C.A., Salini S., Sallese J.M., Salmi T., Salzburger A., Sampayo O.A., Sanfilippo S., Santiago J., Santopinto E., Santoro R., Sanz Ull A., Sarasola X., Sarpun I.H., Sauvain M., Savelyeva S., Sawada R., Sborlini G.F.R., Schaffer A., Schaumann M., Schenk M., Scheuerlein C., Schienbein I., Schlenga K., Schmickler H., Schmidt R., Schoerling D., Schoning A., Schorner-Sadenius T., Schott M., Schulte D., Schwaller P., Schwanenberger C., Schwemling P., Schwerg N., Scibile L., Sciuto A., Scomparin E., Sebastiani C., Seeber B., Segreti M., Selva P., Selvaggi M., Senatore C., Senol A., Serin L., Serluca M., Serra N., Seryi A., Sestini L., Sfyrla A., Shaposhnikov M., Shaposhnikova E., Sharkov B.Y., Shatilov D., Shelton J., Shiltsev V., Shipsey I.P., Shirkov G.D., Shivaji A., Shwartz D., Sian T., Sidorov S., Siemko A., Silvestrini L., Simand N., Simon F., Singh B.K., Siodmok A., Sirois Y., Sirtori E., Sirvinskaite R., Sitar B., Sjostrand T., Skands P., Skordis E., Skovpen K., Skrzypek M., Slade E., Slavich P., Slovak R., Smaluk V., Smirnov V., Snoeys W., Soffi L., Sollander P., Solovyanov O., Soltveit H.K., Song H., Sopicki P., Sorbi M., Spallino L., Spannowsky M., Spataro B., Sphicas P., Spiesberger H., Spiller P., Spira M., Srivastava T., Stachel J., Stakia A., Stanyard J.L., Starchenko E., Starikov A.Y., Stasto A.M., Statera M., Steerenberg R., Steggemann J., Stenvall A., Stivanello F., Stockinger D., Stoel L.S., Stoger-Pollach M., Strauss B., Stuart M., Stupakov G., Su S., Sublet A., Sugita K., Sulak L., Sullivan M.K., Sultansoy S., Sumida T., Suzuki K., Sylva G., Syphers M.J., Sznajder A., Taborelli M., Tahir N.A., Takeuchi M., Tal Hod E., Tambasco C., Tanaka J., Tang K., Tapan I., Taroni S., Tartarelli G.F., Tassielli G., Tavian L., Taylor T.M., Taylor G.N., Teixeira A.M., Tejeda-Munoz G., Telnov V.I., Tenchini R., ten Kate H.H.J., Terashi K., Tesi A., Testa M., Tetrel C., Teytelman D., Thaler J., Thamm A., Thomas S., Tiirakari M.T., Tikhomirov V., Tikhonov D., Timko H., Tisserand V., Tkachenko L.M., Tkaczuk J., Tock J.P., Todd B., Todesco E., Tomas Garcia R., Tommasini D., Tonelli G., Toral F., Torims T., Torre R., Townsend Z., Trant R., Treille D., Trentadue L., Tricoli A., Tricomi A., Trischuk W., Tropin I.S., Tuchming B., Tudora A.A., Turbiarz B., Turk Cakir I., Turri M., Tydecks T., Usovitsch J., Uythoven J., Vaglio R., Valassi A., Valchkova F., Valdivia Garcia M.A., Valente P., Valente R.U., Valente-Feliciano A.-M., Valentino G., Vale Silva L., Valet J.M., Valizadeh R., Valle J.W.F., Vallecorsa S., Vallone G., van Leeuwen M., van Rienen U.H., van Riesen-Haupt L., Varasteh M., Vecchi L., Vedrine P., Velev G., Veness R., Ventura A., Venturini Delsolaro W., Verducci M., Verhaaren C.B., Vernieri C., Verweij A.P., Verwilligen O., Viazlo O., Vicini A., Viehhauser G., Vignaroli N., Vignolo M., Vitrano A., Vivarelli I., Vlachos S., Vogel M., Vogt D.M., Volkl V., Volkov P., Volpini G., von Ahnen J., Vorotnikov G., Voutsinas G.G., Vysotsky V., Wagner U., Wallny R., Wang L.-T., Wang R., Wang K., Ward B.F.L., Watson T.P., Watson N.K., Ws Z., Weiland C., Weinzierl S., Welsch C.P., Wenninger J., Widorski M., Wiedemann U.A., Wienands H.-U., Wilkinson G., Williams P.H., Winter A., Wohlfahrt A., Wojton T., Wollmann D., Womersley J., Woog D., Wu X., Wulzer A., Yanehsari M.K., Yang G., Yang H.J., Yao W.-M., Yazgan E., Yermolchik V., Yilmaz A., Yoo H.-D., Yost S.A., You T., Young C., Yu T.-T., Yu F., Zaborowska A., Zadeh S.G., Zahnd M., Zanetti M., Zanotto L., Zawiejski L., Zeiler P., Zerlauth M., Zernov S.M., Zevi Dell Porta G., Zhang Z., Zhang Y., Zhang C., Zhang H., Zhao Z., Zhong Y.-M., Zhou J., Zhou D., Zhuang P., Zick G., Zimmermann F., Zinn-Justin J., Zivkovic L., Zlobin A.V., Zobov M., Zupan J., Zurita J., BAİBÜ, Fen Edebiyat Fakültesi, Fizik Bölümü, Denizli, Haluk, TOBB ETU, Faculty of Engineering, Department of Electrical & Electronics Engineering, TOBB ETU, Faculty of Engineering, Department of Material Science & Nanotechnology Engineering, TOBB ETÜ, Mühendislik Fakültesi, Elektrik ve Elektronik Mühendisliği Bölümü, TOBB ETÜ, Mühendislik Fakültesi, Malzeme Bilimi ve Nanoteknoloji Mühendisliği Bölümü, Bozbey, Ali, Sultansoy, Saleh, Özdemir, Kadri, Giresun Üniversitesi, UCL - SST/IRMP - Institut de recherche en mathématique et physique, and Ege Üniversitesi
Subjects: Beam losses, IMPACT, Physics::Instrumentation and Detectors, Physics beyond the Standard Model, EVENT BUILDER, hadron collider, General Physics and Astronomy, Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP], 01 natural sciences, 7. Clean energy, law.invention, Subatomär fysik, chemistry.chemical_compound, Conceptual design, Colliding beam accelerators, law, HE-LHC, Subatomic Physics, General Materials Science, Hadron colliders, Física::Física de partícules::Hadrons [Àrees temàtiques de la UPC], Large Hadron Collider, Acceleradors de partícules, Physics, Settore FIS/01 - Fisica Sperimentale, Beams (radiation), Settore FIS/02 - Fisica Teorica, Modelli e Metodi Matematici, Upgrade, Impact, collimators, partikkelfysikk, Future Circular Collider, High-Energy, Systems engineering, HE-LHC: The High-Energy Large Hadron Collider, Col·lisionadors d'hadrons, Applied physics, Collimators, Socio-culturale, Fizik, Hadrons, Accelerator Physics and Instrumentation, HE-LHC physics, Condensed Matter::Materials Science, 0103 physical sciences, Physics::Atomic and Molecular Clusters, beam losses, ddc:530, High Energy Physics, partikkelakselerator, Physical and Theoretical Chemistry, Niobium-tin, 010306 general physics, Collider, Particle Physics, Beams (radiation) | Collimators | Beam losses, Energies::Energia nuclear [Àrees temàtiques de la UPC], Large Hadron Collider HE-LHC, 010308 nuclear & particles physics, High Energy Physics::Phenomenology, Colliders (Nuclear physics), Acceleratorfysik och instrumentering, Event builder, Accelerators and Storage Rings, Particle accelerators, chemistry, Experimental High Energy Physics, Physics::Accelerator Physics, High Energy Physics::Experiment, Future Colliders
Abstract: Authors: A. AbadaM. AbbresciaS. S. AbdusSalamI. AbdyukhanovJ. Abelleira FernandezA. AbramovM. AburaiaA. O. AcarP. R. AdzicP. AgrawalJ. A. Aguilar-SaavedraJ. J. Aguilera-VerdugoM. AibaI. AichingerG. AielliA. AkayA. AkhundovH. AksakalJ. L. AlbaceteS. AlbergoA. AlekouM. AleksaR. AleksanR. M. Alemany FernandezY. AlexahinR. G. AlíaS. AlioliN. Alipour TehraniB. C. AllanachP. P. AllportM. AltınlıW. AltmannshoferG. AmbrosioD. AmorimO. AmstutzL. AnderliniA. AndreazzaM. AndreiniA. AndriatisC. AndrisA. AndronicM. AngelucciF. AntinoriS. A. AntipovM. AntonelliM. AntonelloP. AntonioliS. AntuschF. AnulliL. ApolinárioG. ApollinariA. ApollonioD. AppelöR. B. ApplebyA. ApyanA. ApyanA. ArbeyA. ArbuzovG. ArduiniV. ArıS. AriasN. ArmestoR. ArnaldiS. A. ArsenyevM. ArzeoS. AsaiE. AslanidesR. W. AßmannD. AstapovychM. AtanasovS. AtiehD. AttiéB. AuchmannA. AudurierS. AullS. AumonS. AuneF. AvinoG. AvrillaudG. AydınA. AzatovG. AzuelosP. AzziO. AzzoliniP. AzzurriN. BacchettaE. BacchiocchiH. BachacouY. W. BaekV. BaglinY. BaiS. BairdM. J. BakerM. J. BaldwinA. H. BallA. BallarinoS. BanerjeeD. P. BarberD. BarducciP. BarjhouxD. BarnaG. G. BarnaföldiM. J. BarnesA. BarrJ. Barranco GarcíaJ. Barreiro Guimarães da CostaW. BartmannV. BaryshevskyE. BarziS. A. BassA. BastianinB. BaudouyF. BauerM. BauerT. BaumgartnerI. Bautista-GuzmánC. BayındırF. BeaudetteF. BedeschiM. BéguinI. BellafontL. BellagambaN. BellegardeE. BelliE. BellingeriF. BelliniG. BellomoS. BelomestnykhG. BencivenniM. BenediktG. BernardiJ. BernardiC. BernetJ. M. BernhardtC. BerniniC. BerriaudA. BertarelliS. BertolucciM. I. BesanaM. BesançonO. BeznosovP. BhatC. BhatM. E. BiaginiJ. -L. BiarrotteA. Bibet ChevalierE. R. BielertM. BigliettiG. M. BileiB. BilkiC. BiscariF. BisharaO. R. Blanco-GarcíaF. R. BlánquezF. BlekmanA. BlondelJ. BlümleinT. BoccaliR. BoelsS. A. BogaczA. BogomyagkovO. Boine-FrankenheimM. J. BolandS. BolognaO. BolukbasiM. BombenS. BondarenkoM. BonviniE. BoosB. BordiniF. BordryG. BorghelloL. BorgonoviS. BorowkaD. 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ChattopadhyayR. ChehabS. V. ChekanovN. ChenA. ChernodedV. ChetvertkovaL. ChevalierG. ChiarelliG. ChiarelloM. ChiesaP. ChiggiatoJ. T. ChildersA. ChmielińskaA. CholakianP. ChomazM. ChorowskiW. ChouM. ChrzaszczE. ChyhyrynetsG. CibinettoA. K. CiftciR. CiftciR. CiminoM. CiuchiniP. J. ClarkY. CoadouM. CobalA. CoccaroJ. CoganE. CognerasF. CollamatiC. ColldelramP. CollierJ. CollotR. ContinoF. ConventiC. T. A. CookL. CooleyG. CorcellaA. S. CornellG. H. CorralH. Correia-RodriguesF. CostanzaP. Costa PintoF. CoudercJ. CoupardN. CraigI. Crespo GarridoA. CrivellinJ. F. CroteauM. CrouchE. Cruz AlanizB. CuréJ. CurtiD. CurtinM. CzechC. DachauerR. T. D’AgnoloM. DaiboA. DaineseB. DalenaA. DaljevecW. DallapiazzaL. D’Aloia SchwartzentruberM. DamG. D’AmbrosioS. P. DasS. DasBakshiW. da SilvaG. G. da SilveiraV. D’AuriaS. D’AuriaA. DavidT. DavidekA. DeandreaJ. de BlasC. J. DebonoS. De CurtisN. De FilippisD. de FlorianS. DeghayeS. J. de JongC. Del BoV. Del DucaD. DelikarisF. DeliotA. Dell’AcquaL. Delle RoseM. DelmastroE. De LuciaM. DemarteauD. DenegriL. DeniauD. DenisovH. DenizliA. DennerD. d’EnterriaG. de RijkA. De RoeckF. DerueO. DeschampsS. Descotes-GenonP. S. B. DevJ. B. de Vivie de RégieR. K. DewanjeeA. Di CiaccioA. Di CiccoB. M. DillonB. Di MiccoP. Di NezzaS. Di VitaA. DoblhammerA. DominjonM. D’OnofrioF. DordeiA. DragoP. DraperZ. DrasalM. DrewesL. DuarteI. DubovykP. DudaA. DudarevL. DudkoD. DuellmannM. DünserT. du PreeM. DuranteH. Duran YildizS. DuttaF. DuvalJ. M. DuvalY. DydyshkaB. DziewitS. EisenhardtM. EistererT. EkelofD. El KhechenS. A. EllisJ. EllisJ. A. EllisonK. ElsenerM. ElsingY. EnariC. EnglertH. ErikssonK. J. EskolaL. S. EspositoO. EtiskenE. EtzionP. FabbricatoreA. FalkowskiA. FalouJ. FaltovaJ. FanL. FanòA. FarillaR. FarinelliS. FarinonD. A. FaroughyS. D. FartoukhA. Faus-GolfeW. J. FawcettG. FeliciL. FelsbergerC. FerdeghiniA. M. Fernandez NavarroA. Fernández-TéllezJ. Ferradas TroitinoG. FerraraR. FerrariL. FerreiraP. Ferreira da SilvaG. FerreraF. FerroM. FiascarisS. 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LehtinenS. B. LeithP. LenziE. LeograndeC. LeonidopoulosI. Leon-MonzonG. LernerO. LeroyT. LesiakP. LévaiA. LeverattoE. LevichevG. LiS. LiR. LiD. LiberatiM. LiepeD. A. LissauerZ. LiuA. LobkoE. LocciE. Logothetis AgaliotisM. P. LombardoA. J. LongC. LorinR. LositoA. LouzguitiI. LowD. LucchesiM. T. LucchiniA. LucianiM. LueckhofA. J. G. LuntM. LuzumD. A. LyubimtsevM. MaggioraN. MagninM. A. MahmoudF. MahmoudiJ. MaitreV. MakarenkoA. MalagoliJ. MalclésL. MalgeriP. J. MallonF. MaltoniS. MalvezziO. B. MalyshevG. MancinelliP. MandrikP. ManfrinettiM. ManganoP. ManilM. MannelliG. MarchioriF. MarhauserV. MarianiV. MarinozziS. MariottoP. MarquardC. MarquetT. Marriott-DodingtonR. MartinO. MartinJ. Martin CamalichT. MartinezH. Martinez BruzualM. I. Martínez-HernándezD. E. MartinsS. MarzaniD. MarzoccaL. MarzolaS. MasciocchiI. MasinaA. MassimilianoA. MassironiT. MasubuchiV. A. MatveevM. A. MazzoniM. McCulloughP. A. McIntoshP. MeadeL. MedinaA. MeierJ. MeignanB. MeleJ. G. Mendes SaraivaF. MenezM. MentinkE. MeoniP. MeridianiM. MerkP. MermodV. MertensL. MetherE. MétralM. MiglioratiA. MilaneseC. MilardiG. MilhanoB. L. MilitsynF. MilletI. MinashviliJ. V. MinerviniL. S. MirallesD. MirarchiS. MishimaD. P. MissiaenG. MitselmakherT. MitshuhashiJ. MnichM. Mohammadi NajafabadiR. N. MohapatraN. MokhovJ. G. MolsonR. MongeC. MontagG. MontagnaS. MonteilG. MonteneroE. MontesinosF. MoortgatN. MorangeG. MorelloM. Moreno LlácerM. MorettiS. MorettiA. K. MorleyA. MorosI. MorozovV. MorrettaM. MorroneA. MostacciS. MuanzaN. MuchnoiM. MühleggerM. MulderM. MuldersB. MüllerF. MüllerA. -S. MüllerJ. MunillaM. J. MurrayY. MuttoniS. MyersM. MylonaJ. NachtmanT. NakamotoM. NardecchiaG. NardiniP. NasonZ. NergizA. V. NesterenkoJ. A. NettoA. NettsträterC. NeubüserJ. NeundorfF. NiccoliO. NicrosiniY. NieU. NiedermayerJ. NiedzielaA. NiemiS. A. NikitinA. NisatiJ. M. NoM. NonisY. NosochkovM. NovákA. NovokhatskiJ. M. O’CallaghanC. OchandoS. OgurK. OhmiK. OideV. A. OkorokovY. OkumuraC. OleariF. I. OlnessY. OnelM. OrtinoJ. OsborneP. OslandT. OttoK. Y. OyulmazA. OzansoyV. ÖzcanK. ÖzdemirC. E. PagliaroneH. F. Pais da SilvaE. PalmieriL. PalumboA. PampaloniR. -Q. PanM. PanareoO. PanellaG. PanicoG. PanizzoA. A. PankovV. PantsyrnyC. G. PapadopoulosA. PapaefstathiouY. PapaphilippouM. A. ParkerV. ParmaM. PasqualiS. K. PatraR. PattersonH. PaukkunenF. PaussS. PeggsJ. -P. PenttinenG. PeónE. E. PerepelkinE. PerezJ. C. PerezG. PerezF. PérezE. Perez CodinaJ. Perez MoralesM. PerfilovH. PerneggerM. PeruzziC. PesK. PetersS. PetraccaF. PetrielloL. PezzottiS. PfeifferF. PiccininiT. PieloniM. PieriniH. PikhartovaG. PikursE. PilicerP. PiminovC. PiraR. PittauW. PłaczekM. PlaggeT. PlehnM. -A. PleierM. PłoskońM. PodeurH. PodlechT. PodzornyL. PoggioliA. PoironG. PoleselloM. Poli LenerA. PoliniJ. PolinskiS. M. PolozovL. PonceM. PontL. PontecorvoT. PortaluriK. PotamianosC. PrasseM. PrausaA. PreinerstorferE. PrematT. PriceM. PrimaveraF. PrinoM. PrioliJ. ProudfootA. ProvinoT. PugnatN. PukhaevaS. PuławskiD. PulikowskiG. PunziM. PuttiA. PyarelalH. QuackM. QuispeA. RacioppiH. RafiqueV. RaginelM. RaidalN. S. Ramírez-UribeM. J. Ramsey-MusolfR. RataP. RatoffF. RavottiP. Rebello TelesM. ReboudS. RedaelliE. RennerA. E. Rentería-OlivoM. RescignoJ. ReuterA. RibonA. M. RicciW. RieglerS. RiemannB. RiemannT. RiemannJ. M. RiffletR. A. RimmerR. RinaldesiL. RinolfiO. Rios RubirasT. RisseladaA. RivettiL. RivkinT. RizzoT. RobensF. RobertA. J. RobsonE. RochepaultC. RodaG. RodrigoM. Rodríguez-CahuantziC. RoganM. RoigS. Rojas-TorresJ. RojoG. RolandiG. RolandoP. RoloffA. RomanenkoA. RomanovF. RoncaroloA. Rosado SanchezG. RosazL. RossiA. RossiR. RossmanithB. RoussetC. RoyonX. RuanI. RuehlV. Ruhlmann-KleiderR. RuizL. RumyantsevR. RuprechtA. I. RyazanovA. SabaR. SadykovD. Saez de JaureguiM. SahinB. SailerM. SaitoF. SalaG. P. SalamJ. Salfeld-NebgenC. A. SalgadoS. SaliniJ. M. SalleseT. SalmiA. SalzburgerO. A. SampayoS. SanfilippoJ. SantiagoE. SantopintoR. SantoroA. Sanz UllX. SarasolaI. H. SarpünM. SauvainS. SavelyevaR. SawadaG. F. R. SborliniA. SchafferM. SchaumannM. SchenkC. ScheuerleinI. SchienbeinK. SchlengaH. SchmicklerR. SchmidtD. SchoerlingA. SchoningT. Schörner-SadeniusM. SchottD. SchulteP. SchwallerC. SchwanenbergerP. SchwemlingN. SchwergL. ScibileA. SciutoE. ScomparinC. SebastianiB. SeeberM. SegretiP. SelvaM. SelvaggiC. SenatoreA. SenolL. SerinM. SerlucaN. SerraA. SeryiL. SestiniA. SfyrlaM. ShaposhnikovE. ShaposhnikovaB. Y. SharkovD. ShatilovJ. SheltonV. ShiltsevI. P. ShipseyG. D. ShirkovA. ShivajiD. ShwartzT. SianS. SidorovA. SiemkoL. SilvestriniN. SimandF. SimonB. K. SinghA. SiódmokY. SiroisE. SirtoriR. SirvinskaiteB. SitarT. SjöstrandP. SkandsE. SkordisK. SkovpenM. SkrzypekE. SladeP. SlavichR. SlovakV. SmalukV. SmirnovW. SnoeysL. SoffiP. SollanderO. SolovyanovH. K. SoltveitH. SongP. SopickiM. SorbiL. SpallinoM. SpannowskyB. SpataroP. SphicasH. SpiesbergerP. SpillerM. SpiraT. SrivastavaJ. StachelA. StakiaJ. L. StanyardE. StarchenkoA. Y. StarikovA. M. StaśtoM. StateraR. SteerenbergJ. SteggemannA. StenvallF. StivanelloD. StöckingerL. S. StoelM. Stöger-PollachB. StraussM. StuartG. StupakovS. SuA. SubletK. SugitaL. SulakM. K. SullivanS. SultansoyT. SumidaK. SuzukiG. SylvaM. J. SyphersA. SznajderM. TaborelliN. A. TahirM. TakeuchiE. Tal HodC. TambascoJ. TanakaK. TangI. TapanS. TaroniG. F. TartarelliG. TassielliL. TavianT. M. TaylorG. N. TaylorA. M. TeixeiraG. Tejeda-MuñozV. I. TelnovR. TenchiniH. H. J. ten KateK. TerashiA. TesiM. TestaC. TetrelD. TeytelmanJ. ThalerA. ThammS. ThomasM. T. TiirakariV. TikhomirovD. TikhonovH. TimkoV. TisserandL. M. TkachenkoJ. TkaczukJ. P. TockB. ToddE. TodescoR. Tomás GarciaD. TommasiniG. TonelliF. ToralT. TorimsR. TorreZ. TownsendR. TrantD. TreilleL. TrentadueA. TricoliA. TricomiW. TrischukI. S. TropinB. TuchmingA. A. TudoraB. TurbiarzI. Turk CakirM. TurriT. TydecksJ. UsovitschJ. UythovenR. VaglioA. ValassiF. ValchkovaM. A. Valdivia GarciaP. ValenteR. U. ValenteA. -M. Valente-FelicianoG. ValentinoL. Vale SilvaJ. M. ValetR. ValizadehJ. W. F. ValleS. VallecorsaG. ValloneM. van LeeuwenU. H. van RienenL. van Riesen-HauptM. VarastehL. VecchiP. VedrineG. VelevR. VenessA. VenturaW. Venturini DelsolaroM. VerducciC. B. VerhaarenC. VernieriA. P. VerweijO. VerwilligenO. ViazloA. ViciniG. ViehhauserN. VignaroliM. VignoloA. VitranoI. VivarelliS. VlachosM. VogelD. M. VogtV. VölklP. VolkovG. VolpiniJ. von AhnenG. VorotnikovG. G. VoutsinasV. VysotskyU. WagnerR. WallnyL. -T. WangR. WangK. WangB. F. L. WardT. P. WatsonN. K. WatsonZ. WsC. WeilandS. WeinzierlC. P. WelschJ. WenningerM. WidorskiU. A. WiedemannH. -U. WienandsG. WilkinsonP. H. WilliamsA. WinterA. WohlfahrtT. WojtońD. WollmannJ. WomersleyD. WoogX. WuA. WulzerM. K. YanehsariG. YangH. J. YangW. -M. YaoE. YazganV. YermolchikA. YilmazA. YilmazH. -D. YooS. A. YostT. YouC. YoungT. -T. YuF. YuA. ZaborowskaS. G. ZadehM. ZahndM. ZanettiL. ZanottoL. ZawiejskiP. ZeilerM. ZerlauthS. M. ZernovG. Zevi Dell PortaZ. ZhangY. ZhangC. ZhangH. ZhangZ. ZhaoY. -M. ZhongJ. ZhouD. ZhouP. ZhuangG. ZickF. ZimmermannEmail authorJ. Zinn-JustinL. ZivkovicA. V. ZlobinM. ZobovJ. ZupanJ. Zuritathe FCC Collaboration, In response to the 2013 Update of the European Strategy for Particle Physics (EPPSU), the Future Circular Collider (FCC) study was launched as a world-wide international collaboration hosted by CERN. The FCC study covered an energy-frontier hadron collider (FCC-hh), a highest-luminosity high-energy lepton collider (FCC-ee), the corresponding 100km tunnel infrastructure, as well as the physics opportunities of these two colliders, and a high-energy LHC, based on FCC-hh technology. This document constitutes the fourth volume of the FCC Conceptual Design Report, devoted to the High-Energy Large Hadron Collider HE-LHC. It summarizes the HE-LHC physics discovery opportunities, presents the HE-LHC accelerator design, performance reach, and operation plan, discusses the underlying technologies, the civil engineering and technical infrastructure, and also sketches a possible implementation. Combining ingredients from the Large Hadron Collider (LHC), the high-luminosity LHC upgrade and adding novel technologies and approaches, the HE-LHC design aims at a hadron collider with about twice the centre-of-mass collision energy that the LHC can reach. Its performance aims at exploring physics beyond the Standard Model, signi cantly extending the LHC's direct and indirect sensitivity to new physics and discoveries.
Published: 2020

18. Hydrodynamical description for magneto-transport in the strange metal phase of Bi-2201

Author: Bernd Buechner, Nicodemo Magnoli, Enrico Giannini, Martina Meinero, Christian Hess, Marina Putti, Federico Caglieris, Marco Affronte, Daniel K. Brattan, and Andrea Amoretti
Subjects: Superconductivity, High Energy Physics - Theory, Thermoelectric transport, Materials science, Condensed matter physics, Strongly Correlated Electrons (cond-mat.str-el), superconductivity, Doping, FOS: Physical sciences, Metal, Condensed Matter - Strongly Correlated Electrons, High Energy Physics - Theory (hep-th), visual_art, Phase (matter), Condensed Matter::Superconductivity, visual_art.visual_art_medium, Condensed Matter::Strongly Correlated Electrons, Cuprate, Magneto
Abstract: High temperature superconductors are strongly coupled systems which present a complicated phase diagram with many coexisting phases. This makes it difficult to understand the mechanism which generates their singular transport properties. Hydrodynamics, which mostly relies on the symmetries of the system without referring to any specific microscopic mechanism, constitutes a promising framework to analyze these materials. In this paper we show that in the strange metal phase of the cuprates, a whole set of transport coefficients are described by a universal hydrodynamic framework once one accounts for the effects of quantum critical charge density waves. We corroborate our theoretical prediction by measuring the DC transport properties of Bi-2201 close to optimal doping, proving the validity of our approach. Our argument can be used as a consistency check to understand the universality class governing the behavior of high temperature cuprate superconductors., Version to appear on Physical Review Research
Published: 2020

19. Epitaxial Zr-doped CeO2films by chemical solution deposition as buffer layers for Fe(Se,Te) film growth

Author: Achille Angrisani Armenio, Laura Piperno, Francesco Rizzo, Antonella Mancini, Valeria Braccini, Giuseppe Celentano, Angelo Vannozzi, Alessandro Rufoloni, Andrea Augieri, Giulia Sylva, Simone Prili, Andrea Masi, Marina Putti, Valentina Pinto, Enrico Silva, Pietro Manfrinetti, Vannozzi, A., Prili, S., Sylva, G., Masi, A., Armenio, A. A., Mancini, A., Pinto, V., Rufoloni, A., Piperno, L., Augieri, A., Rizzo, F., Manfrinetti, P., Braccini, V., Putti, M., Silva, E., and Celentano, G.
Subjects: Aluminium oxides, Materials science, epitaxial growth, Doping, iron based superconductors, chemical solution deposition, dewetting, magnetic characterization, Metals and Alloys, Surface finish, Condensed Matter Physics, Epitaxy, iron based superconductor, Surface coating, Chemical engineering, Materials Chemistry, Ceramics and Composites, Irradiation, Dewetting, Electrical and Electronic Engineering, Deposition (chemistry)
Abstract: The epitaxial growth of Zr-doped CeO2 (CZO) films by chemical solution deposition (CSD) on single crystal substrates such as Al2O3, SrTiO3 and Y2O3-stabilized ZrO2 (YSZ) and their use as buffer layers for Fe(Se,Te) film growth are reported. The growth of 30 nm thin CZO films is mostly dominated by dewetting issues, leading to highly incomplete substrate coverage due to the strong tendency of CZO grains to agglomerate. This effect is less severe on YSZ substrate and, in addition, can be fully controlled by setting the deposition temperature at 950 °C and operating under Ar-H2 reducing atmosphere. These conditions promote the growth of epitaxial and compact CZO films on YSZ, showing a flat surface morphology with root-mean-square roughness around 2.5 nm. Preliminary results on Fe(Se,Te) film deposited by pulsed laser deposition on CZO-buffered YSZ are reported. Although good epitaxial growth is achieved on CZO buffer layer, Fe(Se,Te) films exhibit poor superconducting properties. On the other hand, Fe(Se,Te) films show excellent properties when a seed layer is used, exhibiting a sharp superconducting transition at about 17 K and a critical current density exceeding 1 MA cm-2 at 4.2 K in self field. The main role of the seed layer, consisting of a non-superconducting Fe(Se,Te) film, is to favour the crystal and chemical matching between buffer layer and film, allowing for the growth of high-quality superconducting Fe(Se,Te) at deposition temperature as low as 200 °C. In perspective of applications, this result is a significant step towards process simplification and cost reduction of Fe(Se,Te)-based coated conductor technology development, being the first demonstration of superconducting Fe(Se,Te) films grown on CSD buffer layer.
Published: 2020

20. Evidence of the isoelectronic character of F doping in SmFeAsO

Author: Fabio, Bernardini, Federico, Caglieris, Ilaria, Pallecchi, and Marina, Putti
Abstract: We study the electronic structure of the SmFeAsO
Published: 2019

21. Band filling and disorder effects on the normal state thermoelectric behavior in MgB

Author: Ilaria, Pallecchi, Marco, Monni, Pietro, Manfrinetti, and Marina, Putti
Abstract: The goal of this work is providing a comprehensive interpretation framework for the wide and varied experimental phenomenology of the Seebeck effect in MgB
Published: 2019

22. In-plane and out-of-plane properties of a BaFe2As2 single crystal

Author: Federico Caglieris, Marina Putti, Hiroshi Eisaki, Alessandra Continenza, I. Pallecchi, G. Lamura, Martina Meinero, and Shigeyuki Ishida
Subjects: Superconductivity, Materials science, Condensed matter physics, Ab initio, 02 engineering and technology, 021001 nanoscience & nanotechnology, Condensed Matter Physics, 01 natural sciences, Magnetic susceptibility, Crystal, Thermal conductivity, Electrical resistivity and conductivity, 0103 physical sciences, General Materials Science, 010306 general physics, 0210 nano-technology, Anisotropy, Single crystal
Abstract: Anisotropy of transport and magnetic properties of parent compounds of iron based superconductors is a key ingredient of superconductivity. In this work, we investigate in-plane and out-of-plane properties, namely thermal, electric, thermoelectric transport and magnetic susceptibility in a high quality BaFe2As2 single crystal of the 122 parent compound, using a combined experimental and theoretical approach. Combining the ab initio calculation of the band structure and the measured in-plane and out-of-plane resistivity, we evaluate the scattering rates which turn out to be strongly anisotropic and determined by spin excitations in the antiferromagnetic state. The observed anisotropy of thermal conductivity is discussed in terms of anisotropy of sound velocities which we estimate to be [Formula: see text]. Remarkably, we find that thermal conductivity is characterized by a sizeable electronic contribution at low temperature, which is ascribed to the high purity of our crystal.
Published: 2019

23. Anisotropic Effect of Proton Irradiation on Pinning Properties of Fe(Se,Te) Thin Films

Author: Luca Pellegrino, Laura Gozzelino, Angela Nigro, Emilio Bellingeri, Carlo Ferdeghini, Sandro Pace, Giulia Sylva, Alberto Martinelli, Marina Putti, Gaia Grimaldi, Ilaria Pallecchi, Daniele Torsello, Gianluca Ghigo, Antonio Leo, and Valeria Braccini
Subjects: Superconducting materials radiation effects, iron chalcogenide wires, critical temperature and critical fields, resistance measurement, Materials science, Proton, Magnetoresistance, 01 natural sciences, critical temperature and critical fields, Condensed Matter::Superconductivity, 0103 physical sciences, Electronic, Cuprate, Irradiation, Optical and Magnetic Materials, Thin film, Electrical and Electronic Engineering, 010306 general physics, Anisotropy, Critical field, Superconductivity, iron chalcogenide wires, resistance measurement, Superconducting materials radiation effects, Electronic, Optical and Magnetic Materials, Condensed Matter Physics, Condensed matter physics
Abstract: At the present day, iron-based superconductors (IBS) can be considered as competitors of cuprates for the fabrication of superconducting cables for high field application in the presence of particle irradiation. In particular, it has been demonstrated that 11-IBS are very robust against proton irradiation. In this paper, we analyze the effect of this kind of irradiation on the anisotropy of superconducting and pinning properties of Fe(Se,Te) thin films grown on CaF2. By electrical transport measurements, we evaluate the upper critical field as a function of the temperature and the pinning activation energy as function of the applied magnetic field, for different orientation between the material crystal structure and the field itself, in pristine and irradiated samples. The aim is to recognize if and how proton irradiation modifies the anisotropy of the material properties.
Published: 2019

24. Evidence for Longitudinal Homogeneity and No Je Degradation in Bi-2212 Wires Realized by the GDG Process

Author: Luca Leoncino, Giuseppe Celentano, Sandro Chiarelli, Alessandro Leveratto, Marina Putti, Carlo Ferdeghini, Amalia Ballarino, Simon C. Hopkins, Andrea Malagoli
Published: 2019
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25. Analysis of Fe(Se,Te) films deposited on unbuffered invar 36

Author: Valeria Braccini, Carlo Ferdeghini, Giulia Sylva, Giuseppe Celentano, Andrea Malagoli, Amalia Ballarino, Emilio Bellingeri, Alexander J.G. Lunt, Marina Putti, Angelo Vannozzi, Simon C. Hopkins, Sylva, G., Malagoli, A., Bellingeri, E., Putti, M., Ferdeghini, C., Vannozzi, A., Celentano, G., Hopkins, S. C., Lunt, A., Ballarino, A., and Braccini, V.
Subjects: Materials science, Misorientation, Te) thin films, Iron, Fe(Se, Analytical chemistry, Iron based superconductors, Substrate (electronics), engineering.material, Epitaxy, Heat treatment, 01 natural sciences, Microanalysis, Pulsed laser deposition, Nickel, Iron based superconductor, 0103 physical sciences, Electronic, Epitaxial growth, Texture (crystalline), Optical and Magnetic Materials, Electrical and Electronic Engineering, 010306 general physics, biaxial texturing, pulsed laser deposition, coated conductor, Substrates, invar 36 alloy, coated conductors, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Fe(Se,Te) thin films, Fe(Se,Te) thin film, engineering, Layer (electronics), Invar
Abstract: In this paper, the feasibility of producing Fe(Se,Te)-coated conductors on cost-effective, unbuffered Invar 36 substrates is studied. A suitable substrate with a sharp {001} texture and a misorientation angle lower than 10° was developed, and the possibility of growing epitaxial thin films without any buffer layer was demonstrated. It was also shown that the presence of a Fe(Se,Te) seed layer can improve the in- and out-of-plane orientation of the film. A high-resolution scanning electron microscopy study was performed, and the absence of a superconducting transition has been attributed to Ni poisoning based on X-ray microanalysis.
Published: 2019

26. Weak acid leaching of MgB2 to purify magnesiothermic boron powder

Author: Gianmarco Bovone, G. Grasso, Cristina Bernini, Amalia Ballarino, Carlo Ferdeghini, Maurizio Vignolo, A. Tumino, Matteo Tropeano, Simon C. Hopkins, Marina Putti, Federico Loria, and Marco Capra
Subjects: chemistry.chemical_classification, Materials science, chemistry.chemical_element, Salt (chemistry), 02 engineering and technology, 010402 general chemistry, 021001 nanoscience & nanotechnology, 01 natural sciences, 0104 chemical sciences, Amorphous solid, Acetic acid, chemistry.chemical_compound, chemistry, Chemical engineering, Mechanics of Materials, Impurity, Phase (matter), Materials Chemistry, Degradation (geology), General Materials Science, Reactivity (chemistry), 0210 nano-technology, Boron
Abstract: We have established a new procedure for recovering boron contained in oxidized MgB2 phase. Incorrect conditions of synthesis or conservation, or excess impurities in precursors, can lead to MgO formation with consequent degradation of superconducting properties, thus representing a possible problem in the industrial production of MgB2 conductors following the ex-situ PIT process. A procedure has been developed in order to dissolve MgO (due to the oxidization of Mg in MgB2 phase) and to decompose the MgB2 phase into elemental B and a soluble Mg salt. The process can also be successfully applied to low-grade B in order to enhance the purity, providing that the B is first reacted into MgB2. In fact, MgB2 synthesis converts residual B2O3 (present in B) and other impurities to leachable compounds. For the present work, an ill-preserved MgB2 powder produced in 2008 was treated with glacial acetic acid. The reduction of impurities and secondary phases was monitored along each step of the proposed process by X-ray diffraction (XRD) technique and by energy dispersion spectroscopy (EDS) analysis. The purification process was successfully applied on two different MgB2 powders: the first was synthesized using commercial B (H. C. Starck), the second using a different magnesiothermic B with a low purity grade prepared by freeze-drying process at CNR-SPIN. An interesting result is that, after acidic treatment of MgB2, the resulting B particles are finer and more amorphous than pristine B particles. The increased surface area of B undoubtedly offers a more reactivity of powders versus the weak acid, because the impurities within the B particles are exposed to the direct action of the acid and not longer protected by B crust.
Published: 2021

27. Mn substitution effect on the local structure of La(Fe1−x Mn x )AsO studied by temperature dependent x-ray absorption measurements

Author: Pietro Manfrinetti, Naurang L. Saini, Alessia Provino, Laura Simonelli, M. Y. Hacisalihoglu, Marina Putti, Carlo Marini, and Alberto Martinelli
Subjects: Superconductivity, Materials science, Valence (chemistry), Extended X-ray absorption fine structure, Magnetic moment, superconductivity, X-ray, Mn substitution effect, 02 engineering and technology, Electronic structure, 021001 nanoscience & nanotechnology, Condensed Matter Physics, 01 natural sciences, iron pnictides, local structure, Thermal expansion, Crystallography, 0103 physical sciences, General Materials Science, Substitution effect, 010306 general physics, 0210 nano-technology
Abstract: The local structure of La(Fe1−x Mn x )AsO has been investigated using temperature dependent Fe K-edge extended x-ray absorption fine structure (EXAFS) measurements. The EXAFS data reveal distinct behavior of Fe–As and Fe–Fe atomic displacements with a clear boundary between x ⩽ 0.02 and x > 0.02. The Fe–As bondlength shows a gradual thermal expansion while the Fe–Fe bond manifests a temperature dependent anomaly at ∼180 K for x > 0.02. It is interesting to find characteristically different nature of Fe–As and Fe–Fe bondlengths shown by the temperature dependent mean square relative displacements. Indeed, the Fe–As bond, stiffer than that of the Fe–Fe, gets softer for x ⩽ 0.02 and hardly shows any change for x > 0.02. On the other hand, Fe–Fe bond tends to be stiffer for x ⩽ 0.02 followed by a substantial softening for x > 0.02. Such a distinction has been seen also in the As K-edge x-ray absorption near edge structure, probing local geometry around As atom together with the valence electronic structure. The results suggest that local atomic displacements by Mn substitution inducing increased iron local magnetic moment that should be the main reason for its dramatic effect in iron-based superconductors.
Published: 2020

28. Gd3Ni2 and Gd3CoxNi2−x: magnetism and unexpected Co/Ni crystallographic ordering

Author: Vitalij K. Pecharsky, Marina Putti, Pietro Manfrinetti, Volodymyr Smetana, Durga Paudyal, Anja-Verena Mudring, Karl A. Gschneidner, and Alessia Provino
Subjects: 010302 applied physics, Materials science, Fermi level, Intermetallic, 02 engineering and technology, General Chemistry, Crystal structure, 021001 nanoscience & nanotechnology, 01 natural sciences, Crystallography, symbols.namesake, Ferromagnetism, 0103 physical sciences, Materials Chemistry, symbols, Curie temperature, 0210 nano-technology, Single crystal, Solid solution, Monoclinic crystal system
Abstract: The crystal structure, composition and physical properties of Gd3Ni2, which was earlier reported to exist in the Gd–Ni system without any details of its structure and properties, have been determined. This rare earth binary compound is a high-temperature phase: it forms via a peritectic reaction at 988 K (715 °C) and decomposes below ≈923 K (650 °C). The compound can be retained at room temperature as a metastable phase by quenching after high temperature annealing. Gd3Ni2 crystallizes in the monoclinic Dy3Ni2 structure type [mS20, C2/m (No. 12), Z = 4; with lattice parameters a = 13.418(3) A, b = 3.720(1) A, c = 9.640(2) A, β = 106.250(3)°]. Ni can be substituted by Co up to 50% (i.e. up to and including Gd3CoNi) with no change in the structural prototype; the substitution of Co for Ni stabilizes the R3CoxNi2−x phases down to room temperature. The crystal structure, magnetic properties and magnetocaloric effect (MCE) have been investigated for both Gd3Ni2 and the related Gd3CoxNi2−x solid solution alloys (0 ≤ x ≤ 1). The crystal structure of the Gd3CoNi is a ternary ordered derivative of the monoclinic Dy3Ni2-type, where Co fully occupies only one of the two 4i Wyckoff sites available for the transition metal. To the best of our knowledge, this is the first example of an intermetallic phase showing ordered site occupations by the chemically quite similar elements Co and Ni. All compounds show long range ferromagnetic ordering, with TC progressively increasing from 147 K (for Gd3Ni2) to 176 K (for Gd3CoNi) as a cubic function of the Co content. Evidence of Co contributing to the magnetic interactions in these compounds has been found. First-principles total energy calculations predicted the ordered occupation of Co and Ni at the crystallographic sites of Gd3CoNi, which was later confirmed by single crystal X-ray diffraction. The increased conduction electronic state (3d) exchange splitting at the Fermi level supports the experimentally observed enhanced Curie temperature in Gd3CoNi compared to Gd3Ni2.
Published: 2016

29. Reverse advance internal magnesium diffusion process to produce dense MgB2 bulks and high JC wires through high pressure heat treatment

Author: Marco Capra, Andrzej Morawski, Federico Loria, Gianmarco Bovone, Simon C. Hopkins, Marina Putti, Cristina Bernini, Daniel Gajda, Giovanni Grasso, Antonio Sergio Siri, Amalia Ballarino, T. Cetner, Matteo Tropeano, Carlo Ferdeghini, and Maurizio Vignolo
Subjects: Alkaline earth metal, Materials science, Magnesium, Metals and Alloys, chemistry.chemical_element, Deformation (meteorology), Atmospheric temperature range, Condensed Matter Physics, Diffusion process, chemistry, High pressure, Materials Chemistry, Ceramics and Composites, Electrical and Electronic Engineering, Electric current, Diffusion (business), Composite material
Abstract: Here we report a new versatile technique to manufacture MgB2 massive samples, called reverse advance internal magnesium diffusion (r-AIMI). The idea focuses on the goal of obtaining dense bulk or wire samples depending on synthesis conditions. In respect to the traditional AIMI procedure, in which a central Mg rod is covered with a B corona, here a Mg tube is filled with B powder and clad in a Ti external sheath, which is quite similar to the traditional (powder in tube) technique. After cold deformation, during which several intermediate low temperature heat treatments are necessary in order to relax the Ti sheath and Mg tube, samples are reacted at high temperature and ambient pressure to form a dense MgB2 core. The MgB2 phase results are totally disconnected from metallic sheath, and can be easily extracted and characterized. Critical current density measurements show values exceeding 106 A cm−2 below 1.5 T at 20 K. In the last part of the paper, we show the effect of final heat-treatment performed under high pressure to eliminate the present void and connect the external sheath to the internal MgB2 core and so permitting the electric transfer necessary for power applications of wires.
Published: 2020

30. Unusual thermoelectric properties of BaFe2As2 in high magnetic fields

Author: Uli Zeitler, Marina Putti, Martina Meinero, A. Jost, I. Pallecchi, G. Lamura, Shigeyuki Ishida, Hiroshi Eisaki, and Federico Caglieris
Subjects: Physics, Condensed matter physics, Dirac (video compression format), Fermi level, 02 engineering and technology, 021001 nanoscience & nanotechnology, 01 natural sciences, Magnetic field, symbols.namesake, Dirac fermion, Seebeck coefficient, 0103 physical sciences, Thermoelectric effect, symbols, 010306 general physics, 0210 nano-technology, Single crystal, Nernst effect
Abstract: Electric and thermoelectric transport properties are mutually intertangled in diffusive transport equations. In particular, in high mobility multiband systems an anomalous behavior may occur, which can be tracked down to the properties of the individual bands. Here, we present magnetoelectric and magnetothermoelectric transport properties of a ${\mathrm{BaFe}}_{2}{\mathrm{As}}_{2}$ high-quality single crystal, for different magnetic field directions up to 30 T. We detect a giant Nernst effect and an anomalous field dependence of the Seebeck coefficient. The extraction of the Peltier tensor coefficients ${\ensuremath{\alpha}}_{xx}, {\ensuremath{\alpha}}_{xy}$, and ${\ensuremath{\alpha}}_{xz}$ allows us to disentangle the main transport mechanisms in play. The large ${\ensuremath{\alpha}}_{xy}$ and ${\ensuremath{\alpha}}_{xz}$ values and their field dependence provide evidence of the presence of a high mobility band, compatible with a Dirac dispersion band, crossing the Fermi level, and suggest a possible three-dimensional nature of the Dirac fermions.
Published: 2018

31. Effects of high-energy proton irradiation on the superconducting properties of Fe(Se,Te) thin films

Author: Laura Gozzelino, Giulia Sylva, Antonio Leo, Angela Nigro, Valeria Braccini, Gaia Grimaldi, Marina Putti, Ilaria Pallecchi, Daniele Torsello, Gianluca Ghigo, Luca Pellegrino, E. Bellingeri, C. Ferdeghini, and Alberto Martinelli
Subjects: Materials Chemistry2506 Metals and Alloys, Materials science, iron-based superconductors, FOS: Physical sciences, Context (language use), 02 engineering and technology, Substrate (electronics), proton irradiation, thin films, Ceramics and Composites, Condensed Matter Physics, 2506, Electrical and Electronic Engineering, 01 natural sciences, Superconductivity (cond-mat.supr-con), Electrical resistivity and conductivity, 0103 physical sciences, Materials Chemistry, Irradiation, Thin film, 010306 general physics, Critical field, Superconductivity, Condensed matter physics, Condensed Matter - Superconductivity, Transition temperature, Metals and Alloys, 021001 nanoscience & nanotechnology, iron-based superconductors, proton irradiation, thin films, 0210 nano-technology
Abstract: In this paper we explore the effects of 3.5 MeV proton irradiation on Fe(Se,Te) thin films grown on CaF2. In particular, we carry out a systematic experimental investigation with different irradiation fluences up to 7.30x10^16 cm^-2 and different proton implantation depths, in order to clarify whether and to what extent the critical current is enhanced or suppressed, what are the effects of irradiation on the critical temperature, the resistivity and the critical magnetic fields, and finally what is the role played by the substrate in this context. We find that the effect of irradiation on superconducting properties is generally small as compared to the case of other iron-based superconductors. Such effect is more evident on the critical current density Jc, while it is minor on the transition temperature Tc, on the normal state resistivity and on the upper critical field Hc2 up to the highest fluences explored in this work. In addition, our analysis shows that when protons implant in the substrate far from the superconducting film, the critical current can be enhanced up to 50% of the pristine value at 7 T and 12 K, while there is no appreciable effect on critical temperature and critical fields together with a slight decrease in resistivity. On the contrary, when the implantation layer is closer to the film-substrate interface, both critical current and temperature show a decrease accompanied by an enhancement of the resistivity and the lattice strain. This result evidences that possible modifications induced by irradiation in the substrate may affect the superconducting properties of the film via lattice strain. The robustness of the Fe(Se,Te) system to irradiation induced damage makes it a promising compound for the fabrication of magnets in high-energy accelerators., Comment: 14 pages, 11 figures, submitted to Superconductor Science and Technology
Published: 2018

32. Evidence of the isoelectronic character of F doping in SmFeAsO(1-x)F(x): a first-principles investigation

Author: Fabio Bernardini, Ilaria Pallecchi, Federico Caglieris, and Marina Putti
Subjects: Materials science, Condensed matter physics, Condensed Matter - Superconductivity, Doping, FOS: Physical sciences, Charge (physics), 02 engineering and technology, Electronic structure, 021001 nanoscience & nanotechnology, Condensed Matter Physics, 01 natural sciences, 3. Good health, Ion, Superconductivity (cond-mat.supr-con), Paramagnetism, Oxidation state, 0103 physical sciences, Antiferromagnetism, General Materials Science, 010306 general physics, 0210 nano-technology, Electronic band structure
Abstract: We study the electronic structure of the SmFeAsO(1-x)F(x) alloy by means of first-principle calculations. We find that, contrary to common believe, F-doping does not change the charge balance between electrons and holes free-carriers in SmFeAsO(1-x)F(x). For energies within a narrow energy range across E_F, the effect of F-doping on the band structure dispersion is tiny in both the paramagnetic and stripe antiferromagnetic phase. The charge balance between the conducting FeAs-layer and the SmO(1-x)F(x) charge reservoir layer is not influenced by the compositional change. The additional charge carried by fluorine, with respect to the oxygen, is compensated by a change in the oxidation state of the Sm ion from 3+ to 2+. A comparison with the SmFe(1-x)Co(x)AsO system shows that such charge compensation by the Sm ion is not shared by donors substituting at the Fe site., Comment: J. Phys.: Condens. Matter (2019)
Published: 2018
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33. Effect of the external pressure at the crossover between magnetism and superconductivity in LnFeAsO1-x Fx (Ln = La0.7Y0.3, Ce) superconductors

Author: Pietro Carretta, Giacomo Prando, S. Sanna, Marina Putti, Rustem Khasanov, R. De Renzi, Hubertus Luetkens, Alberto Martinelli, Anthony A. Amato, Sanna, S., Prando, G., Khasanov, R., Carretta, P., Amato, A., Luetkens, H., Putti, M., Martinelli, A., and De Renzi, R.
Subjects: Physics, Lanthanide, Superconductivity, muon spin spectroscopy, Condensed matter physics, Magnetism, Fe-based materials, Crossover, Statistical and Nonlinear Physics, 02 engineering and technology, Muon spin spectroscopy, 021001 nanoscience & nanotechnology, Condensed Matter Physics, 01 natural sciences, External pressure, Ion, Condensed Matter::Superconductivity, magnetism, 0103 physical sciences, 010306 general physics, 0210 nano-technology, Fe-based material
Abstract: The interplay between magnetism and superconductivity is tuned as a function of the external pressure in LnFeAsO[Formula: see text]Fx at [Formula: see text] values close to the appearance of superconductivity for lanthanide ion Ln=La[Formula: see text]Y[Formula: see text] and Ce. The results show that in these compounds, both superconductivity and magnetism are reinforced by pressure. Furthermore, muon spin rotation and relaxation measurements reveal qualitative remarkable differences among the samples: Ln=Ce displays nanoscopic coexistence of magnetism and superconductivity in the same volume fraction while Ln=La[Formula: see text]Y[Formula: see text] shows macroscopic phase separation. The Ln-dependent results can be due to a complex combination of the external and chemical pressure, the latter being driven by the different average ionic Ln radius.
Published: 2018

34. Experimental Evidence for Static Charge Density Waves in Iron Oxypnictides

Author: Alessia Provino, Pietro Manfrinetti, Alberto Martinelli, Federico Caglieris, Clemens Ritter, Alessandro Genovese, G. Lamura, and Marina Putti
Subjects: Superconductivity, Materials science, Condensed matter physics, Condensed Matter - Superconductivity, Phase (waves), FOS: Physical sciences, General Physics and Astronomy, Charge density, 02 engineering and technology, Electron, 021001 nanoscience & nanotechnology, 01 natural sciences, Density wave theory, Superconductivity (cond-mat.supr-con), Modulation, Condensed Matter::Superconductivity, 0103 physical sciences, Wave vector, 010306 general physics, 0210 nano-technology, Powder diffraction
Abstract: In this Letter we report high-resolution synchrotron X-ray powder diffraction and transmission electron microscope analysis of Mn-substituted LaFeAsO samples, demonstrating that a static incommensurate modulated structure develops across the low-temperature orthorhombic phase, whose modulation wave-vector depends on the Mn content. The incommensurate structural distortion is likely originating from a charge-density-wave instability, a periodic modulation of the density of conduction electrons associated with a modulation of the atomic positions. Our results add a new component in the physics of Fe-based superconductors, indicating that the density wave ordering is charge-driven., Comment: To be published in the Physical Review Letters
Published: 2017

35. Development and Characterization of P-doped Ba-122 Superconducting Tapes

Author: D. Contarino, Dirk Johrendt, A. Genovese, C. Bernini, C. Lohnert, Andrea Malagoli, and Marina Putti
Subjects: Superconductivity, Materials science, Condensed matter physics, Doping, 02 engineering and technology, 021001 nanoscience & nanotechnology, Condensed Matter Physics, 01 natural sciences, Electronic, Optical and Magnetic Materials, Characterization (materials science), superconducting filaments and wires, Phase (matter), 0103 physical sciences, Electronic, Grain boundary, critical current density, Electrical and Electronic Engineering, Optical and Magnetic Materials, Thin film, Deformation (engineering), 010306 general physics, 0210 nano-technology, Electrical conductor
Abstract: Among the recently discovered Fe-based superconducting compounds, the Ba-122 phase has proved to be the more attracting for the development of powder in tube (PIT) processed conductors. In fact, after some years of development, critical current densities ( Jc ) of about 105 A/cm2 at 4.2 K and magnetic fields up to 10 T have been obtained in (Ba0.6K0.4)Fe2As 2, PIT wires and tapes. To develop a safe upscaling method, the synthesis of the powders is a crucial point. In order to avoid the use of highly reactive K we have developed BaFe2(P1-xAsx)2 PIT tapes. This compound has proved to be very stable and in form of crystals and thin films exhibits excellent critical current: We succeeded in manufacturing PIT tapes with this phase with Jc values of about 103 A/cm2 at 4.2 K in self-field. Detailed microstructural and chemical investigations of the samples have been performed by high-resolution TEM, scanning TEM, and electron energy loss spectrometry analysis. A deformation network inside the grains that can induce strong pinning has been observed. However, chemical inhomogeneities at the grain boundaries are also present, which limit the transport current.
Published: 2017

36. 75As NQR signature of the isoelectronic nature of ruthenium for iron substitution in LaFe1−xRuxAsO

Author: Roberto De Renzi, A. Palenzona, Samuele Sanna, Pietro Manfrinetti, Pietro Bonfà, Giuseppe Allodi, Marcello Mazzani, Marina Putti, and Alberto Martinelli
Subjects: Superconductivity, Analytical chemistry, chemistry.chemical_element, Electronic structure, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Ruthenium, Crystallography, Delocalized electron, chemistry, Strongly correlated material, Density functional theory, Nuclear quadrupole resonance, Arsenic
Abstract: We have investigated the effects of the isovalent ruthenium substitution in LaFeRuAsO, by extensive 75As NQR (nuclear quadrupole resonance) measurements, supported by DFT (density functional theory) calculations, in order to characterize both the lattice and electronic structure details. The evidence for five different local configurations around the arsenic site emerges upon increasing ruthenium for iron substitution. DFT calculations confirm the attribution of the measured electric field gradients (EFGs) to ruthenium atom occupancies (0, 1, 2, 3, and 4) on the nearest-neighbour sites of arsenic. It is found that the low-frequency (Ru-free) NQR peak remains almost unaffected upon ruthenium substitution, providing an experimental confirmation that ruthenium does not introduce delocalized carriers in the iron plane.
Published: 2014

37. Thermoelectric properties of iron-based superconductors and parent compounds

Author: Marina Putti, Ilaria Pallecchi, and Federico Caglieris
Subjects: Materials Chemistry2506 Metals and Alloys, FOS: Physical sciences, 02 engineering and technology, quantum critical point, 01 natural sciences, Nernst effect, Superconductivity (cond-mat.supr-con), symbols.namesake, Dirac cones, magnon drag, multiband character, Seebeck effect, Electrical and Electronic Engineering, Condensed Matter Physics, Ceramics and Composites, 2506, Condensed Matter - Strongly Correlated Electrons, Condensed Matter::Superconductivity, 0103 physical sciences, Thermoelectric effect, Materials Chemistry, Spin density wave, 010306 general physics, Spin-½, Superconductivity, Physics, Condensed matter physics, Strongly Correlated Electrons (cond-mat.str-el), Condensed Matter - Superconductivity, Fermi level, Metals and Alloys, Fermi surface, 021001 nanoscience & nanotechnology, Pairing, symbols, Condensed Matter::Strongly Correlated Electrons, 0210 nano-technology
Abstract: Herewith, we review the available experimental data of thermoelectric transport properties of iron-based superconductors and parent compounds. We discuss possible physical mechanisms into play in determining the Seebeck effect, from whence one can extract information about Fermi surface reconstruction and Lifshitz transitions, multiband character, coupling of charge carriers with spin excitations and its relevance in the unconventional superconducting pairing mechanism, nematicity, quantum critical fluctuations close to the optimal doping for superconductivity, correlation. Additional information is obtained from the analysis of the Nernst effect, whose enhancement in parent compounds must be related partially to multiband transport and low Fermi level, but mainly to the presence of Dirac cone bands at the Fermi level. In the superconducting compounds, large Nernst effect in the normal state is explained in terms of fluctuating precursors of the spin density wave state, while in the superconducting state it mirrors the usual vortex liquid dissipative regime. A comparison between the phenomenology of thermoelectric behavior of different families of iron-based superconductors and parent compounds allows to evidence the key differences and analogies, thus providing clues on the rich and complex physics of these fascinating unconventional superconductors.
Published: 2016

38. Role of magnetic dopants in the phase diagram of Sm 1111 pnictides: The case of Mn

Author: Jun-ichi Shimoyama, R. De Renzi, Toni Shiroka, Maria N. Gastiasoro, G. Lamura, M. Moroni, Sabine Wurmehl, Pabitra Kumar Biswas, Pietro Carretta, Marina Putti, Federico Caglieris, S. Bordignon, Brian M. Andersen, S. J. Singh, S. Sanna, Lamura, G., Shiroka, T., Bordignon, S., Sanna, S., Moroni, M., De Renzi, R., Carretta, P., Biswas, P.K., Caglieris, F., Putti, M., Wurmehl, S., Singh, S.J., Shimoyama, J., Gastiasoro, M.N., and Andersen, B.M.
Subjects: muon spin spectroscopy, Materials science, Magnetism, 02 engineering and technology, Condensed Matter Physic, 01 natural sciences, Impurity, Condensed Matter::Superconductivity, 0103 physical sciences, Electronic, Antiferromagnetism, Optical and Magnetic Materials, 010306 general physics, Phase diagram, Superconductivity, Electronic, Optical and Magnetic Materials, Condensed Matter Physics, Condensed matter physics, Electronic, Optical and Magnetic Material, superconductivity, Order (ring theory), Muon spin spectroscopy, 021001 nanoscience & nanotechnology, magnetism, Content (measure theory), 0210 nano-technology
Abstract: The deliberate insertion of magnetic Mn dopants in the Fe sites of the optimally doped ${\mathrm{SmFeAsO}}_{0.88}{\mathrm{F}}_{0.12}$ iron-based superconductor can modify in a controlled way its electronic properties. The resulting phase diagram was investigated across a wide range of manganese contents ($x$) by means of muon-spin spectroscopy ($\ensuremath{\mu}\mathrm{SR}$), both in zero and in transverse fields, to probe the magnetic and the superconducting order, respectively. The pure superconducting phase (at $xl0.03$) is replaced by a crossover region at intermediate Mn values ($0.03\ensuremath{\le}xl0.08$), where superconductivity coexists with static magnetic order. After completely suppressing superconductivity for $x=0.08$, a further increase in Mn content reinforces the natural tendency towards antiferromagnetic correlations among the magnetic Mn ions. The sharp drop of ${T}_{c}$ and the induced magnetic order in the presence of magnetic disorder/dopants, such as Mn, are both consistent with a recent theoretical model of unconventional superconductors (M. N. Gastiasoro et al., Phys. Rev. Lett. 117, 257002 (2016)), which includes correlation-enhanced RKKY couplings between the impurity moments.
Published: 2016

39. Iron-Based Superconductors: Materials Aspects for Applications

Author: Ilaria Pallecchi and Marina Putti
Published: 2015

40. Pseudogap Analysis of Normal State Transport Behavior of 11 and 1111 Fe-Based Superconductors

Author: Marina Putti, I. Pallecchi, Matteo Tropeano, Alberto Martinelli, A. Palenzona, G. Lamura, and Carlo Ferdeghini
Subjects: Superconductivity, Materials science, Condensed matter physics, superconductivity, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Electrical resistivity and conductivity, Condensed Matter::Superconductivity, Seebeck coefficient, Density of states, Cuprate, Fe based, Pseudogap, Scaling
Abstract: In this paper we analyze transport data of different families of Fe-based superconductors, within a pseudogap framework. The Fe(Te, Se) samples exhibit s-shaped resistivity ρ(T) curves, while SmFeAs(O, F) ones present a departure from their high-temperature linear behavior. In either case, a characteristic temperature can be identified. These temperatures correspond to those at which abrupt changes in the temperature behavior of Hall resistance and of Seebeck coefficient occur, suggesting that they are signatures of pseudogaps opening in the density of states. The direct correlation between these characteristic temperatures and the superconducting transition temperatures suggests that the pseudogap and the superconducting state originate from the same mechanism. Scaling procedures of resistivity curves confirm such proportionality. On the other hand, excess Fe content in Fe(Te, Se) samples affects the pseudogap temperature much more strongly than the superconducting Tc. Finally, we find out that the pseudogap in the 1111 family is almost insensitive to disorder, as in high-Tc cuprates.
Published: 2011

41. Study of the Superconducting and Thermal Properties of ex situ GlidCop-Sheathed Practical $\hbox{MgB}_{2}$ Conductors

Author: C. Fanciulli, Andrea Malagoli, Matteo Tropeano, Marina Putti, G. Romano, Carlo Ferdeghini, Maurizio Vignolo, C. Bernini, V. Cubeda, and Valeria Braccini
Subjects: Superconductivity, Materials science, superconductivity, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Conductor, chemistry.chemical_compound, Thermal conductivity, chemistry, Electrical resistivity and conductivity, Glidcop, Magnesium diboride, Thermal stability, Electrical and Electronic Engineering, Composite material, Electrical conductor
Abstract: In dc and ac practical applications of MgB2 superconducting wires, an important role is represented by the material sheath that has to provide, among other things, a suitable electrical and thermal stabilization. One way to obtain a large-enough amount of low-resistivity material into the conductor architecture is to use it as the external sheath. In this paper, we study ex situ multifilamentary MgB2 wires fabricated with oxide-dispersion-strengthened copper (GlidCop) as the external sheath in order to reach a good compromise between critical current density and thermal properties. We prepared three GlidCop samples with different contents of dispersed submicroscopic Al2O3 particles. We characterized the superconducting and thermal properties, and we showed that the good thermal conductivity, together with the good mechanical properties and a reasonable critical current density, makes the GlidCop composite wire a useful conductor for applications where high thermal conductivity is required at temperatures above 30 K, such as superconducting fault-current limiters.
Published: 2009

42. Superconducting Properties of ${\rm V}_{3}{\rm Si}$ Thin Films Grown by Pulsed Laser Ablation

Author: Carlo Ferdeghini, Emilio Bellingeri, Matteo Tropeano, Maurizio Ferretti, Pietro Manfrinetti, R. Vaglio, Ilaria Pallecchi, Chiara Tarantini, G. Lamura, Antonello Andreone, Marina Putti, C. Fanciulli, C., Ferdeghini, E., Bellingeri, C., Fanciulli, M., Ferretti, P., Manfrinetti, I., Pallecchi, M., Putti, C., Tarantini, M., Tropeano, Andreone, Antonello, G., Lamura, and Vaglio, Ruggero
Subjects: Superconductivity, Residual resistivity, Materials science, Laser ablation, Vacuum deposition, Electrical resistivity and conductivity, Analytical chemistry, Electrical and Electronic Engineering, Thin film, Condensed Matter Physics, Critical field, Electronic, Optical and Magnetic Materials, Pulsed laser deposition
Abstract: We present a systematic study of the superconducting properties of high quality V3Si thin films, grown by high vacuum pulsed laser deposition from a stoichiometric target, a technique never reported in literature for this compound. By changing both the substrate (crystal structure and orientation) and the deposition conditions (substrate temperature, target-substrate distance, laser frequency and pulse energy) the critical temperature and the resistivity values of the samples have been finely tuned. Best results (TC = 16.1 K and Residual Resistivity Ratio RRR = 8.5) are obtained for deposition temperatures higher than 1200degC on both LaAlO3 and MgO substrates. All the samples are polycrystalline, that however does not affect the good quality of the transport properties. The possibility of multiband superconductivity in this compound is investigated, probing as a function of temperature: (i) the critical field up to 28 T using voltamperometric measurements, and (ii) the superfluid density via magnetic penetration depth measurements with a single coil inductive technique operating in the MHz region.
Published: 2009

43. High-Energy Ball Milling and Synthesis Temperature Study to Improve Superconducting Properties of ${\rm MgB}_{2}$Ex-situ Tapes and Wires

Author: Matteo Tropeano, Cristina Bernini, Marina Putti, Andrea Malagoli, Carlo Ferdeghini, Maurizio Vignolo, G Romano, Carlo Fanciulli, and Valeria Braccini
Subjects: Superconductivity, Condensed Matter - Materials Science, High energy, Materials science, Condensed matter physics, Magnesium, Condensed Matter - Superconductivity, Materials Science (cond-mat.mtrl-sci), FOS: Physical sciences, chemistry.chemical_element, Sintering, Condensed Matter Physics, Electronic, Optical and Magnetic Materials, Superconductivity (cond-mat.supr-con), chemistry, Critical current, Electrical and Electronic Engineering, Composite material, Ball mill
Abstract: MgB2 monofilamentary nickel-sheated tapes and wires were fabricated by means of the ex-situ powder-in-tube method using either high-energy ball milled and low temperature synthesized powders. All sample were sintered at 920 C in Ar flow. The milling time and the revolution speed were tuned in order to maximize the critical current density in field (Jc): the maximum Jc value of 6 x 10e4 A/cm2 at 5 K and 4 T was obtained corresponding to the tape prepared with powders milled for 144h at 180rpm. Vorious synthesis temperature were also investigated (730-900 C) finding a best Jc value for the wire prepared with powders synthesized at 745 C. We speculate that this optimal temperature is due to the fluidifying effect of unreacted magnesium content before the sintering process which could better connect the grains.
Published: 2009

44. Role of heat and mechanical treatments in the fabrication of superconducting Ba0.6K0.4Fe2As2 ex-situ Powder-In-Tube tapes

Author: A. Genovese, Dirk Johrendt, S. Marchner, E. Wiesenmayer, Marina Putti, and A. Malagoli
Subjects: Superconductivity, Materials Chemistry2506 Metals and Alloys, Fabrication, Materials science, Filling factor, Condensed Matter - Superconductivity, Metals and Alloys, FOS: Physical sciences, Ba122 wire, Microstructure, Condensed Matter Physics, Superconductivity (cond-mat.supr-con), grains connectivity, Materials Chemistry, Ceramics and Composites, Grain boundary, scalable process, Electrical and Electronic Engineering, 2506, Composite material, Porosity, Current density, Electrical conductor
Abstract: Among the recently discovered Fe-based superconducting compounds, the (K,Ba)Fe2As2 phase is attracting great attention within the scientific community interested in conductor developments. In fact, after some years of development, critical current densities Jc of about 105 A cm−2 at fields up to more than 10 T have been obtained in powder-in-tube (PIT) processed wires and tapes. Here we explore the crucial points in the wire/tape fabrication by means of the ex situ PIT method. We focus on scaling-up processes, which are crucial for industrial fabrication. We analyzed the effects on the microstructure of the different heat and mechanical treatments. By an extensive microstructural analysis correlated with the transport properties, we addressed the issues concerning the phase purity, internal porosity, and crack formation in the superconducting core region. Our best conductors, with a filling factor of about 30% heat-treated at 800 °C, exhibited Tc = 38 K, the highest value measured in this kind of superconducting tape. The microstructure analysis shows clean and well-connected grain boundaries but rather poor density: the measured Jc of about 3 104 A cm−2 in the self field is suppressed by less than a factor of seven at 7 T. Such not-yet-optimized Jc values can be accounted for by the reduced density, while the moderate in-field suppression and a rather high n-factor confirm the high homogeneity and uniformity of these tapes.
Published: 2015

45. Influence of substrate type on transport properties of superconducting FeSe0.5Te0.5 thin films

Author: Zhixiang Shi, Ichiro Tsukada, Kazumasa Iida, Ludwig Schultz, Marina Putti, Alberto Sala, Ataru Ichinose, Ruben Hühne, Feifei Yuan, Marco Langer, and Jens Hänisch
Subjects: Materials Chemistry2506 Metals and Alloys, Materials science, FOS: Physical sciences, anisotropy, 02 engineering and technology, 01 natural sciences, Pulsed laser deposition, Superconductivity (cond-mat.supr-con), Condensed Matter::Materials Science, lattice parameters, Lattice (order), Condensed Matter::Superconductivity, 0103 physical sciences, Materials Chemistry, Electrical and Electronic Engineering, Thin film, 010306 general physics, Anisotropy, substrates, Scaling, Superconductivity, Condensed matter physics, Condensed Matter - Superconductivity, Metals and Alloys, 021001 nanoscience & nanotechnology, Condensed Matter Physics, FeSe0.5Te0.5 thin films, critical current density, Ceramics and Composites, 2506, Transmission electron microscopy, 0210 nano-technology, Science, technology and society
Abstract: FeSe0.5Te0.5 thin films were grown by pulsed laser deposition on CaF2, LaAlO3 and MgO substrates and structurally and electro-magnetically characterized in order to study the influence of the substrate on their transport properties. The in-plane lattice mismatch between FeSe0.5Te0.5 bulk and the substrates shows no influence on the lattice parameters of the films, whereas the type of substrates affects the crystalline quality of the films and, therefore, the superconducting properties. The film on MgO showed an extra peak in the angular dependence of critical current density Jc({\theta}) at {\theta} = 180{\deg} (H || c), which arises from c-axis defects as confirmed by transmission electron microscopy. In contrast, no Jc({\theta}) peaks for H || c were observed in films on CaF2 and LaAlO3. Jc({\theta}) can be scaled successfully for both films without c-axis correlated defects by the anisotropic Ginzburg-Landau (AGL) approach with appropriate anisotropy ratio {\gamma}J. The scaling parameter {\gamma}J is decreasing with decreasing temperature, which is different from what we observed in FeSe0.5Te0.5 films on Fe-buffered MgO substrates., Comment: accepted for publication in SUST
Published: 2015

46. Superconducting Materials

Author: Helmut Krauth, Klaus Schlenga, Davide Nardelli, Ilaria Pallecchi, Matteo Tropeano, Roland Hott, Thomas Wolf, and Marina Putti
Published: 2015

47. The thermal conductivity of silver and silver alloy sheaths for Bi-2223 tapes

Author: Carlo Ferdeghini, D Mazzone, Marina Putti, Emilio Bellingeri, M.O Rikel, S. Roncallo, G Zanicchi, and G. Grasso
Subjects: Copper oxide, Materials science, High-temperature superconductivity, Alloy, Energy Engineering and Power Technology, engineering.material, Condensed Matter Physics, Microstructure, Electronic, Optical and Magnetic Materials, law.invention, chemistry.chemical_compound, Thermal conductivity, chemistry, law, Electrical resistivity and conductivity, engineering, Electrical and Electronic Engineering, Composite material, Calcium oxide, Strontium oxide
Abstract: We have measured the thermal and electrical conductivity of silver and silver alloy sheaths for Bi-2223 tapes. The thermal conductivity at 10 K varied from 1 to 104 W m−1 K−1 (the upper values are for Ag sheaths and the lower, 1–102 W m−1 K−1, for the alloy sheaths). The large spread of data for the alloy sheaths is due to the difference in composition and microstructure, which in case of the AgMg system depends on the thermal and mechanical history of alloy.
Published: 2002

48. Transport properties of c-oriented MgB2 thin films grown by pulsed laser deposition

Author: V. Braccini, W. Ramadan, G. Grassano, A. Palenzona, Pietro Manfrinetti, C. Ferdeghini, Marina Putti, and V. Ferrando
Subjects: Materials science, Annealing (metallurgy), Anisotropy, Critical fields, MgB2, Thin film, Electronic, Optical and Magnetic Materials, Condensed Matter Physics, Energy Engineering and Power Technology, Electrical and Electronic Engineering, FOS: Physical sciences, chemistry.chemical_element, Pulsed laser deposition, Superconductivity (cond-mat.supr-con), Electronic, Optical and Magnetic Materials, Boron, Critical field, Superconductivity, Condensed matter physics, Condensed Matter - Superconductivity, Magnetic field, chemistry
Abstract: The electronic anisotropy in MgB2, which arises from its layered crystal structure is not completely clear until now. High quality c-oriented films offer the opportunity of studying such property. MgB2 thin films were deposited by using two methods both based on room temperature precursor deposition (by Pulsed Laser Ablation) and ex-situ annealing in Mg atmosphere. The two methods differ for the starting targets: stoichiometric MgB2 in one case and Boron in the other. The two films presented in this paper are grown by means of the two techniques on MgO substrates and are both c-oriented; they present TC values of 31.5 and 37.4 K respectively. Upper critical field measurements, up to 9T, with the magnetic field in perpendicular and parallel directions in respect to the film surface evidenced anisotropy ratios of 1.8 and 1.4 respectively. In this paper we will discuss this remarkable and surprising difference also in comparison with the literature data., Presented at EUCAS 2001. submitted to Physica C
Published: 2002

49. Deposition and properties of Fe(Se,Te) thin films on vicinal CaF2substrates

Author: Alberto Sala, Marina Putti, Hagen Bryja, Sebastian Molatta, Kornelius Nielsch, Jens Hänisch, Kazumasa Iida, Ludwig Schultz, and Ruben Hühne
Subjects: Materials Chemistry2506 Metals and Alloys, Fe1+dSe0.5Te0.5thin films, Materials science, anisotropy, 02 engineering and technology, Substrate (electronics), Island growth, Epitaxy, 01 natural sciences, Pulsed laser deposition, Electrical resistivity and conductivity, 0103 physical sciences, Materials Chemistry, critical current density, Vicinal substrates, Ceramics and Composites, Condensed Matter Physics, 2506, Electrical and Electronic Engineering, Thin film, 010306 general physics, Anisotropy, Condensed matter physics, Metals and Alloys, 021001 nanoscience & nanotechnology, 0210 nano-technology, Vicinal
Abstract: We report on the growth of epitaxial Fe1+δ Se0.5Te0.5 thin films on 0°, 5°, 10°, 15° and 20° vicinal cut CaF2 single crystals by pulsed laser deposition. In situ electron and ex situ x-ray diffraction studies reveal a tilted growth of the Fe1+δ Se0.5Te0.5 films, whereby under optimized deposition conditions the c-axis alignment coincides with the substrate [001] tilted axis up to a vicinal angle of 10°. Atomic force microscopy shows a flat island growth for all films. From resistivity measurements in longitudinal and transversal directions, the ab- and c-axis components of resistivity are derived and the mass anisotropy parameter is determined. Analysis of the critical current density indicates that no effective c-axis correlated defects are generated by vicinal growth, and pinning by normal point core defects dominates. However, for Hab the effective pinning centers change from surface defects to point core defects near the superconducting transition due to the vicinal cut. Furthermore, we show in angular-dependent critical current density data a shift of the ab-planes maxima position with the magnetic field strength.
Published: 2017

50. Effect of high-pressure annealing on the normal-state transport ofLaO0.5F0.5BiS2

Author: Yoshikazu Mizuguchi, Marina Putti, Joe Kajitani, Satoshi Demura, Osuke Miura, Yoshihiko Takano, Ilaria Pallecchi, G. Lamura, and Kenzo Deguchi
Subjects: Superconductivity, Materials science, Condensed matter physics, Annealing (metallurgy), Doping, Condensed Matter Physics, Omega, Electronic, Optical and Magnetic Materials, Condensed Matter::Materials Science, Nuclear magnetic resonance, Electrical resistivity and conductivity, Lattice (order), Seebeck coefficient, Crystallite
Abstract: We study normal state electrical, thermoelectrical, and thermal transport in polycrystalline ${\mathrm{BiS}}_{2}$-based compounds, which become superconducting by F doping on the O site. In particular, we explore undoped ${\mathrm{LaOBiS}}_{2}$ and doped ${\mathrm{LaO}}_{0.5}{\mathrm{F}}_{0.5}{\mathrm{BiS}}_{2}$ samples, prepared either with or without high-pressure annealing, in order to evidence the roles of doping and preparation conditions. The high-pressure annealed sample exhibits room temperature values of resistivity \ensuremath{\rho} around 5 m\ensuremath{\Omega}cm, Seebeck coefficient $S$ around $\ensuremath{-}20\ensuremath{\mu}V/K$, and thermal conductivity \ensuremath{\kappa} around 1.5 W/Km, while the Hall resistance ${R}_{H}$ is negative at all temperatures and its value is $\ensuremath{-}10{}^{\ensuremath{-}8} m{}^{3}/\mathrm{C}$ at low temperature. The sample prepared at ambient pressure exhibits ${R}_{H}$ positive in sign and five times larger in magnitude, and $S$ negative in sign and slightly smaller in magnitude. These results reveal a complex multiband evolution brought about by high-pressure annealing. In particular, the sign inversion and magnitude suppression of ${R}_{H}$, indicating increased electron-type carrier density in the high-pressure sample, may be closely related to previous findings about change in lattice parameters and enhancement of superconducting ${T}_{c}$ by high-pressure annealing. As for the undoped sample, it exhibits 10 times larger resistivity, 10 times larger $|S|$, and 10 times larger $|{R}_{H}|$ than its doped counterpart, consistent with its insulating nature. Our results point out the dramatic effect of preparation conditions in affecting charge carrier density as well as structural, band, and electronic parameters in these systems.
Published: 2014

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