97 results on '"Low energies"'
Search Results
2. Spin waves in zigzag graphene nanoribbons and the stability of edge ferromagnetism
- Author
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Culchac, F. J., Latgé, A., and Costa, A. T.
- Subjects
Antiferromagnetic correlations ,Discontinuous transition ,Energy dispersions ,Ferromagnetic alignment ,Gate voltages ,Graphene nanoribbons ,Low energies ,Nanoribbons ,Spin excitation ,Spintronic device ,Wave vector - Published
- 2011
3. Low energy eta-baryon interaction.
- Author
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Nogueira-Santos, M.G.L. and Barros, C.C.
- Subjects
- *
DIFFERENTIAL cross sections , *BARYONS - Abstract
The η -baryon interactions at low energies are studied using a model based on effective chiral Lagrangians, which consider baryons with spin 1/2 and spin 3/2 in the intermediate states. The interacting baryons considered in this work are B = N , Λ , Σ , Ξ. We calculate the expected total and differential cross sections, phase shifts, and polarizations in the center-of-mass frame of reference for each reaction. [ABSTRACT FROM AUTHOR]
- Published
- 2023
- Full Text
- View/download PDF
4. Measurement of the antiproton–nucleus annihilation cross-section at low energy.
- Author
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Aghai-Khozani, H., Bianconi, A., Corradini, M., Hayano, R., Hori, M., Leali, M., Lodi Rizzini, E., Mascagna, V., Murakami, Y., Prest, M., Vallazza, E., Venturelli, L., and Yamada, H.
- Subjects
- *
PROTON & antiproton annihilation , *NUCLEAR cross sections , *NUCLEAR energy , *CARBON spectra , *ANTINUCLEONS - Abstract
Systematic measurements of the annihilation cross sections of low energy antinucleons were performed at CERN in the 80's and 90's. However the antiproton data on medium-heavy and heavy nuclear targets are scarce. The ASACUSA Collaboration at CERN has measured the antiproton annihilation cross section on carbon at 5.3 MeV: the value is (1.73 ± 0.25) barn. The result is compared with the antineutron experimental data and with the theoretical previsions. [ABSTRACT FROM AUTHOR]
- Published
- 2018
- Full Text
- View/download PDF
5. Low-energy antinucleon-nucleus interaction revisited.
- Author
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Friedman, E.
- Subjects
- *
NUCLEON-antinucleon interactions , *NUCLEAR cross sections , *ANTINEUTRONS , *NUCLEAR optical potentials , *COULOMB potential , *COMPARATIVE studies - Abstract
Annihilation cross sections of antiprotons and antineutrons on the proton between 50 and 400 MeV/c show Coulomb focusing below 200 MeV/c and almost no charge-dependence above 200 MeV/c. Similar comparisons for heavier targets are not possible for lack of overlap between nuclear targets studied with $\bar {p}$ and $\bar {n}$ beams. Interpolating between $\bar {p}$-nucleus annihilation cross sections with the help of an optical potential to compare with $\bar {n}$-nucleus annihilation cross sections reveal unexpected features of Coulomb interactions in the latter. Direct comparisons between $\bar {n}$-nucleus and $\bar {p}$-nucleus annihilations at very low energies could be possible if $\bar {p}$ cross sections are measured on the same targets and at the same energies as the available cross sections for $\bar {n}$. Such measurements may be feasible in the foreseeable future. [ABSTRACT FROM AUTHOR]
- Published
- 2015
- Full Text
- View/download PDF
6. Solidity without inhomogeneity: Perfectly homogeneous, weakly coupled, UV-complete solids
- Author
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Alberto Nicolis, Angelo Esposito, and Rafael Krichevsky
- Subjects
Global Symmetries ,High Energy Physics - Theory ,Nuclear and High Energy Physics ,Phonon ,low energies ,FOS: Physical sciences ,Solid ,effective theory ,01 natural sciences ,Lattice (order) ,Quantum mechanics ,0103 physical sciences ,lcsh:Nuclear and particle physics. Atomic energy. Radioactivity ,Boundary value problem ,Quantum field theory ,010306 general physics ,Physics ,Bulk modulus ,010308 nuclear & particles physics ,Isotropy ,Space-Time Symmetries ,Effective Field Theories ,Invariant (physics) ,Condensed Matter - Other Condensed Matter ,Transverse plane ,High Energy Physics - Theory (hep-th) ,lcsh:QC770-798 ,Other Condensed Matter (cond-mat.other) - Abstract
Solid-like behavior at low energies and long distances is usually associated with the spontaneous breaking of spatial translations at microscopic scales, as in the case of a lattice of atoms. We exhibit three quantum field theories that are renormalizable, Poincar�� invariant, and weakly coupled, and that admit states that on the one hand are perfectly homogeneous down to arbitrarily short scales, and on the other hand have the same infrared dynamics as isotropic solids. All three examples presented here lead to the same peculiar solid at low energies, featuring very constrained interactions and transverse phonons that always propagate at the speed of light. In particular, they violate the well known $c_L^2 > \frac{4}{3} c_T^2$ bound, thus showing that it is possible to have a healthy renormalizable theory that at low energies exhibits a negative bulk modulus (we discuss how the associated instabilities are absent in the presence of suitable boundary conditions). We do not know whether such peculiarities are unavoidable features of large scale solid-like behavior in the absence of short scale inhomogeneities, or whether they simply reflect the limits of our imagination., 23 pages
- Published
- 2020
7. Stopping of protons – Improved accuracy of the UCA model
- Author
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Schiwietz, G. and Grande, P.L.
- Subjects
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STOPPING power (Nuclear physics) , *PROTON beams , *MATHEMATICAL convolutions , *APPROXIMATION theory , *ENERGY dissipation , *ELECTRON capture , *NUCLEAR energy - Abstract
Abstract: Recent theoretical developments in the unitary convolution approximation (UCA) for electronic energy losses of bare and screened ions are presented. Examples are given for proton beams and rare-gas targets. For gas targets there exists a sufficient amount of experimental data on charge exchange, for pinpointing the largely unknown stopping-power contribution of electron-capture processes at low and intermediate energies. [Copyright &y& Elsevier]
- Published
- 2012
- Full Text
- View/download PDF
8. Measurement of the antiproton–nucleus annihilation cross section at 5.3 MeV
- Author
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Bianconi, A., Corradini, M., Hori, M., Leali, M., Lodi Rizzini, E., Mascagna, V., Mozzanica, A., Prest, M., Vallazza, E., Venturelli, L., and Zurlo, N.
- Subjects
- *
PROTON & antiproton annihilation , *NUCLEAR cross sections , *HEAVY nuclei , *TARGETING (Nuclear strategy) , *NUCLEAR reactions , *NUCLEAR models , *MEASUREMENT - Abstract
Abstract: Antiproton annihilation cross sections on medium-heavy and heavy nuclear targets are measured for the first time at 5.3 MeV kinetic energy at the Antiprotons Decelerator facility of CERN. The results agree with the expected behavior from the black-disk model with the Coulomb corrections. [Copyright &y& Elsevier]
- Published
- 2011
- Full Text
- View/download PDF
9. Astrophysical S-factor of radiative pLi capture at low energies.
- Author
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Dubovichenko, S. B., Burtebaev, N., Zazulin, D. M., and Amar, A. A.
- Subjects
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ASTROPHYSICS , *CLUSTER analysis (Statistics) , *DATA analysis , *ENERGY levels (Quantum mechanics) , *QUANTUM theory - Abstract
possibility of describing experimental data for the astrophysical S-factor of pLi capture at low energies is discussed within the potential cluster model with forbidden states. [ABSTRACT FROM AUTHOR]
- Published
- 2010
- Full Text
- View/download PDF
10. Phase analysis of elastic pLi scattering at astrophysical energies.
- Author
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Dubovichenko, S. B. and Zazulin, D. M.
- Subjects
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LITHIUM , *ASTROPHYSICS , *SCATTERING (Physics) , *GAUSSIAN processes , *NUCLEAR physics - Abstract
Based on new experimental investigations of elastic pLi scattering at energies 500-1150 keV and angles 30-170°, a phase analysis is performed and interaction potentials for pLi-system in S- and P-states are constructed. [ABSTRACT FROM AUTHOR]
- Published
- 2010
- Full Text
- View/download PDF
11. Elastic cross sections of 1s-muonic atoms at low energies in non-adiabatic approach.
- Author
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Gheisari, R.
- Subjects
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ATOMS , *HYDROGEN isotopes , *WAVE functions , *WAVE mechanics , *NUCLEAR cross sections - Abstract
The low-energy elastic cross-section in collisions of a muonic atom with the hydrogen isotope is investigated, employing a new wave function (trial) and using the coordinate-space Faddeev-Hahn model. The wave function includes non-adiabatic terms. Our results of s-wave cross-sections are given, at the tμ(1s) + d scattering. Calculated cross-sections are in good accord with the results published by Chiccoli et al., while having no good agreement with other recent reports. [ABSTRACT FROM AUTHOR]
- Published
- 2009
- Full Text
- View/download PDF
12. Phase anlysis of elastic р12С scattering for astrophysical energies.
- Author
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Dubovichenko, S. B.
- Subjects
- *
ASTROPHYSICS , *FORCE & energy , *MASS spectrometry , *MANAGEMENT science - Abstract
Based on experimental research of elastic р12С scattering for energies of 200–1110 keV (in the center-of-mass system) and angles of 10–170°, the phase analysis of the р12С system in the S-state is performed and the interaction potential is constructed. [ABSTRACT FROM AUTHOR]
- Published
- 2008
- Full Text
- View/download PDF
13. Electron screening in reactions between light nuclei
- Author
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Barker, F.C.
- Subjects
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NUCLEAR reactions , *ELECTRONS - Abstract
Values of the electron-screening potential derived from previous fits to measurements of low-energy cross sections of nuclear reactions have generally been much larger than the values estimated from model calculations. Here we refit the data using somewhat different procedures and show that better agreement is possible in some cases. [Copyright &y& Elsevier]
- Published
- 2002
- Full Text
- View/download PDF
14. Limits on antiproton-nuclei annihilation cross sections at ∼125 keV.
- Author
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Aghai-Khozani, H., Barna, D., Corradini, M., De Salvador, D., Hayano, R.S., Hori, M., Leali, M., Lodi-Rizzini, E., Mascagna, V., Prest, M., Seiler, D., Sótér, A., Todoroki, K., Vallazza, E., and Venturelli, L.
- Subjects
- *
ANNIHILATION reactions , *KINETIC energy , *ANTIMATTER , *NUCLEAR reactions , *ANTIPROTONS , *PALLADIUM - Abstract
Some experimental limits on the annihilation cross sections σ ann of antiprotons on carbon, palladium, and platinum targets were determined at the previously unexplored kinetic energy region E ≈ 125 keV. Information on σ ann at such low antiproton energies is important in understanding the dynamics of the annihilation process, and provides useful data for models that attempt to describe the matter-antimatter asymmetry in the universe by assuming the existence of islands of antimatter concentration. [ABSTRACT FROM AUTHOR]
- Published
- 2021
- Full Text
- View/download PDF
15. Measurement of the antiproton–nucleus annihilation cross-section at low energy
- Author
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L. Venturelli, Y. Murakami, M. Prest, E. Lodi Rizzini, M. Corradini, Hiroyuki Yamada, Valerio Mascagna, M. Leali, Andrea Bianconi, Ryugo S. Hayano, Hossein Aghai-Khozani, Masaki Hori, and E. Vallazza
- Subjects
Nuclear reaction ,Physics ,Nuclear and High Energy Physics ,Large Hadron Collider ,Annihilation ,010308 nuclear & particles physics ,Low energies ,Antiproton annihilations ,Nuclear reactions ,Antineutron ,01 natural sciences ,Nuclear physics ,Cross section (physics) ,medicine.anatomical_structure ,Low energy ,Antiproton ,0103 physical sciences ,medicine ,Physics::Accelerator Physics ,High Energy Physics::Experiment ,Nuclear Experiment ,010306 general physics ,Nucleus - Abstract
Systematic measurements of the annihilation cross sections of low energy antinucleons were performed at CERN in the 80's and 90's. However the antiproton data on medium-heavy and heavy nuclear targets are scarce. The ASACUSA Collaboration at CERN has measured the antiproton annihilation cross section on carbon at 5.3 MeV: the value is (1.73 ± 0.25) barn. The result is compared with the antineutron experimental data and with the theoretical previsions.
- Published
- 2018
16. Précession du Spin électronique dans un transistor tunel magnétique tout solide
- Author
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Vautrin, Christopher, Institut Jean Lamour (IJL), Institut de Chimie du CNRS (INC)-Université de Lorraine (UL)-Centre National de la Recherche Scientifique (CNRS), Université de Lorraine, Michel Hehn, Daniel Lacour, STAR, ABES, and Université de Lorraine (UL)-Institut de Chimie du CNRS (INC)-Centre National de la Recherche Scientifique (CNRS)
- Subjects
[PHYS.PHYS]Physics [physics]/Physics [physics] ,Low energies ,Transistor ,Basses énergies ,Precession ,[PHYS.PHYS] Physics [physics]/Physics [physics] ,Électronique de spin ,Electronic spin - Abstract
This work is about polarised hot electrons spin precession. This phenomenon is induced by the exchange field of a ferromagnetic thin film in a multilayer structure. The electronic spin precession has already been measured in ferromagnetic materials, but only for electrons whose energy is more than 4eV over the Fermi level. The initial aim of this PhD work is to measure the electron spin precession for weak energies, between 0.7 eV and 2eV over the Fermi level. In order to achieve that, a magnetic tunnel transistor composed of three magnetic layers with their magnetisations directions perpendicular to each other has to be elaborated. The electrons are injected at low energy by means of a tunnel junction. A Schottky diode (interface between Cu and Si) filters the incident electrons by their energies, which enables only ballistic electrons to contribute to the measured current in the semi-conductor. The first task consisted in obtaining a magnetic layer showing perpendicular magnetic anisotropy. We succeeded in growing cobalt nickel multilayers exhibiting a perpendicular magnetic anisotropy up to five repetitions. The second part of the job carried out during this PhD was to optimise the magneto-current of a spin valve. Indeed, it determines the magnetic tunnel transistor sensitivity. We have demonstrated that the magneto-current increases with the number of repetitions of the [Co/Ni] multilayer up to a maximum of nearly a hundred percent, which is the maximum theoretically predicted in a spin valve with crossed magnetisations. Eventually, the third task of this PhD was the study of the electron spin precession in various ferromagnetic materials. This effect has been evidenced here for thin layers with in-plane magnetisations composed of Co, CoFeB, and also for a CoAl alloy depending on the thickness of the layers, Ce travail porte sur la précession du spin d’électrons chauds polarisés en spin. Celle-ci est induite par le champ d’échange d’une couche mince ferromagnétique dans une structure multicouche. La précession du spin électronique a déjà été mesurée dans des matériaux ferromagnétiques mais uniquement pour des électrons qui possèdent une énergie supérieure à 4eV au-dessus du niveau de Fermi. L’objectif premier de cette thèse est de mesurer la précession du spin de l’électron pour des faibles énergies, comprises entre 0.7eV et 2eV au-dessus du niveau de Fermi. Pour ce faire, un transistor tunnel magnétique comportant trois couches magnétiques avec les aimantations qui pointent dans les trois directions de l’espace doit être construit. Les électrons sont injectés à basse énergie grâce à une jonction tunnel. Une diode Schottky (interface entre du Cu et du Si) filtre en énergie les électrons incidents, permettant uniquement aux électrons balistiques de contribuer au courant mesuré dans le semi-conducteur. Le premier travail a consisté à obtenir une couche magnétique exhibant une anisotropie perpendiculaire. Ainsi, nous avons réussi à faire croître une multicouche de Co et Ni sur une diode Schottky qui possède une anisotropie perpendiculaire jusqu’à 5 répétitions. Le deuxième travail réalisé dans cette thèse était d’optimiser le magnéto-courant d’une la vanne de spin. En effet, le magnéto-courant détermine la sensibilité de notre transistor tunnel magnétique. Nous avons notamment démontré ici que le magnéto-courant augmente avec le nombre de répétitions de la multicouche [Co/Ni], pour atteindre quasiment le maximum de 100% théoriquement prédit dans une vanne de spin à aimantations croisées. Enfin, le troisième travail de cette thèse résidait dans l’étude de la précession du spin de l’électron dans différents matériaux ferromagnétiques. Cet effet a été mis en évidence ici pour des couches à aimantation planaire composée de Co, de CoFeB, ainsi que pour un alliage de CoAl et ceci en fonction de leur épaisseur
- Published
- 2017
17. Systèmes quantiques multi-particulaires et localisation à basses énergies ou à faible interaction
- Author
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Ekanga, Trésor, Institut de Mathématiques de Jussieu - Paris Rive Gauche (IMJ-PRG), Université Pierre et Marie Curie - Paris 6 (UPMC)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Université Sorbonne Paris Cité, Anne Boutet de Monvel, Viktor Anatolʹevič Čulaevskij, and STAR, ABES
- Subjects
Faibles interactions ,Low energies ,[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph] ,Weak interaction ,Basses énergies ,[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph] ,Multi-particle systems ,Systèmes multi-particulaires - Abstract
In this thesis, we study for the N-particles Schrodinger operators the Anderson localization phenomenon which consists of both exponential localization of eigenfunctions and dynamical localization. We rst consider the discrete multi-particle Anderson model with a short range interaction and a random potential whose values are independent and identically distributed i.i.d. with a log-Hölder continuous common probability distribution function. For such model, we show that the bottom of its spectrum is non-random and prove the Anderson localization for energies suciently close to the spectral edge. On the other hand, we establish that the complete localization from singleparticle systems extends to multi-particle systems with suciently weak interaction at arbitrary disorder and for absolute continuous probability distribution function of the i.i.d random variables. The results are proved by an adaptation to multi-particle systems of the vari- able energy multi-scale analysis which allows singular distributions instead of the fractional moments method. Wegner bounds, useful for the multi-scale analysis are proved for separable cubes using the Stollmann's Lemma. We also prove the Combes-Thomas estimate which plays an important role in the analysis of extreme energies., Dans cette thèse, on étudie le phénomène de localisation d'Anderson des opérateurs de Schrödinger à N particules qui englobe aussi bien la localisation exponentielle des fonctions propres que la localisation dynamique. Dans un premier temps, on considère le modèle d'Anderson discret multi- particulaire avec un potentiel aléatoire à valeurs indépendantes et identiquement distribuées i.i.d. dont la distribution commune est au moins log-Höldérienne et une interaction de courte portée. On établit pour ce modèle la localisation d'Anderson pour les énergies susamment proches du bas du spectre après avoir montré qu'il est non-aléatoire. D'autre part, on montre que la localisation complète des systèmes mono- particulaires s'étend aux systèmes multi-particulaires ayant une interaction globale susamment faible et pour un désordre arbitraire. Pour ce résultat, l'existence d'une densité bornée de la distribution commune des variables aléatoires i.i.d. est nécessaire et on le montre pour des interactions ayant une forme très générale mais bornées. Les résultats sont démontrés à l'aide de l'adaptation aux systèmes multi- particulaires de l'analyse multi-échelle à énergie variable qui permet de traiter des distributions singulières contrairement à la méthode des moments fractionnaires. Les estimées de Wegner intervenant notamment dans l'analyse multi-échelle sont établies pour des cubes vériant une propriété de séparabilité en utilisant le Lemme de Stollmann. On démontre également l'estimée de Combes-Thomas qui joue un rôle important dans l'analyse des énergies extrêmes.
- Published
- 2017
18. Compton scattering on a target with degeneracy states.
- Author
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Inozemtseva, N., Sysoev, P., and Inozemtsev, V.
- Abstract
n additional pole term and the contributions to it from intermediate states with the same mass but with different spins is calculated for the Compton scattering amplitude on a two-particle system with zero total angular momentum. It is shown that the decomposition of invariant amplitudes on the generalized polarizabilities of the system does not take place if this term is taken into account. [ABSTRACT FROM AUTHOR]
- Published
- 2011
- Full Text
- View/download PDF
19. Core–shell structure in copper ferrite–polyaniline nanocomposite: Confirmation by laser Raman spectra
- Author
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M. Balaji, P. Chithra lekha, and D. Pathinettam Padiyan
- Subjects
Raman frequencies ,Raman scattering ,Materials science ,Laser beam effects ,Polyaniline ,Scanning electron microscope ,High-resolution scanning electron microscopes ,Analytical chemistry ,Core shell structure ,chemistry.chemical_element ,Nanocomposites ,law.invention ,Copper alloys ,chemistry.chemical_compound ,symbols.namesake ,law ,Shell thickness ,Shells (structures) ,In situ polymerization ,Magnetic materials ,Spectroscopy ,Laser Raman spectroscopy ,Laser Raman spectra ,Nanocomposite ,Excitation power ,Low energies ,Laser excitation ,Ferrite ,In-situ polymerization ,Laser ,Higher energy beams ,Copper ,Scanning Electron Microscope ,Induced heating ,chemistry ,Laser-induced heating ,Core particles ,Raman spectroscopy ,symbols ,Ferrite (magnet) ,Average particle size ,Incident energy ,Scanning electron microscopy - Abstract
Laser Raman spectroscopy was used to investigate the presence of core-shell structure in copper ferrite-polyaniline nanocomposites prepared by in situ polymerization method. Laser beams with two excitation powers, 0.3 mW and 3 mW, were employed to study the ferrite-polyaniline interaction and its changes by the laser induced heating effects. Low energy Raman spectra distinctly displayed polyaniline bands only without bands for CuFe 2O 4 in all the nanocomposites. This observation attributes polyaniline shell over the CuFe 2O 4 core particle, since the low energy was not sufficient for the beam to penetrate the polyaniline shell. However, with higher incident energy due to the induced heating effect, there was disturbance of polyaniline shell and the Raman frequencies were shifted depending on the shell thickness. Raman spectra of copper ferrite-polyaniline nanocomposites recorded using higher energy beam were consistent with the low energy Raman spectra of polyaniline samples annealed at three different temperatures of 200, 300 and 400 �C respectively for 2 h. High-resolution scanning electron microscope study also supports the formation of core-shell structure. It revealed that the average particle size increases with increase of shell thicknesses. � 2012 Elsevier B.V.
- Published
- 2012
- Full Text
- View/download PDF
20. An Efficient Ferrocene Derivative as a Chromogenic, Optical, and Electrochemical Receptor for Selective Recognition of Mercury(II) in an Aqueous Environment
- Author
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Sundargopal Ghosh and Arunabha Thakur
- Subjects
Absorption spectroscopy ,Selective recognition ,Inorganic chemistry ,Color ,chemistry.chemical_element ,Iron compounds ,Electrochemistry ,Redox ,Inorganic Chemistry ,Ferrocenyl ,Presence of water ,Visual outputs ,Ferrocene derivative ,Qualitative inorganic analysis ,Physical and Theoretical Chemistry ,Benzylacetate ,Receptor ,Aqueous environment ,Aqueous solution ,Low energies ,Chromogenic ,Binding events ,Organic Chemistry ,Organometallics ,Mercury (element) ,chemistry ,Positive ions ,Mercury compounds ,Colorimetry ,Colorimetric detection - Abstract
The synthesis, electrochemical, optical, and cation-sensing properties of two triazole-tethered ferrocenyl benzylacetate derivatives, C 36H 36O 6N 6Fe (2) and C 23H 23O 3N 3Fe (3), are presented. The binding event of both the receptors can be inferred either from a redox shift (2, ?E 1/2 = 106 mV for Hg 2+ and ?E 1/2 = 187 mV for Ni 2+, 3, ?E 1/2 = 167 mV for Hg 2+ and ?E 1/2 = 136 mV for Ni 2+) or a highly visual output response (colorimetric) for Hg 2+, Ni 2+, and Cu 2+ cations. Remarkably, the redox and colorimetric responses toward Hg 2+ are preserved in the presence of water (CH 3CN/H 2O, 2/8), which can be used for the selective colorimetric detection of Hg 2+ in an aqueous environment over Ni 2+ and Cu 2+ cations. The changes in the absorption spectra are accompanied by the appearance of a new low-energy (LE) peak at 625 nm for both compounds 2 and 3 (2, ? = 2500 M -1 cm -1, 3, ? = 1370 M -1 cm -1), due to a change in color from yellow to purple for Hg 2+ cations in CH 3CN/H 2O (2/8). � 2012 American Chemical Society.
- Published
- 2012
- Full Text
- View/download PDF
21. Assessing the potentiality of the 250kV-SSAMS for stopping power measurements at low energies.
- Author
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Linares, R., Fonseca, L.M., Santos, H.C., Added, N., Seabra, C.C., and Xing, Y.T.
- Subjects
- *
NUCLEAR energy , *ENERGY dissipation , *STOPPING power (Nuclear physics) , *ION energy , *NUCLEAR research - Abstract
Since 2012, a compact 250 kV Single Stage accelerator (250 kV-SSAMS) has been installed at Instituto de Física, Universidade Federal Fluminense, for radiocarbon analysis of natural samples. The system presents two magnets, for mass selection prior and post the gas stripper, and an electrostatic spherical analyzer (ESA). The overall performance of the machine makes it suitable for experimental researches in atomic collisions, in particular for studies of the stopping power of atomic projectiles at energies below 25 keV/u. Here we report on the energy loss measurements of 12C + and 16O + ions in a thin carbon foil at energies in the range of 10 to 25 keV/u. Energies of the ions after the foil are determined from the high-voltage applied to the ESA in order to recover the maximum intensity reading in a Faraday Cup (FC) after the ESA. Energies of the ions after the foil are determined from the high-voltage applied to the ESA. With this technique, experimental data for the stopping power within a precision of about 0.5%. [ABSTRACT FROM AUTHOR]
- Published
- 2019
- Full Text
- View/download PDF
22. New determination of the C-12(alpha, gamma)O-16 reaction rate from gamma-ray angular distribution measurements
- Subjects
NUCLEOSYNTHESIS ,DELAYED ALPHA-SPECTRUM ,THERMONUCLEAR REACTION-RATES ,CONSTRAINTS ,NUCLEAR ,LOW ENERGIES ,N-16 ,C-12(ALPHA ,MASSIVE STARS ,GAMMA)O-16 CROSS-SECTION - Published
- 2005
- Full Text
- View/download PDF
23. S-17(0) determined from the Coulomb breakup of 83 MeV/nucleon B-8
- Subjects
S-FACTOR ,ASTROPHYSICAL INTEREST ,FLUX ,GAMMA)B-8 ,BE-7(P ,DISSOCIATION ,NUCLEAR ,LOW ENERGIES ,GAMMA)B-8 CROSS-SECTION ,E2 TRANSITIONS - Abstract
A kinematically complete measurement was made of the Coulomb dissociation of SE nuclei on a Pb target at 83 MeV/nucleon. The cross section was measured at low relative energies in order to infer the astrophysical S factor for the Be-7(p, gamma)B-8 reaction. A first-order perturbation theory analysis including El, E2, and M1 transitions was employed to extract the El strength relevant to neutrino-producing reactions in the solar interior. By fitting the measured cross section from E-rel = 130 to 400 keV, we find S-17(0)= 17.8(-1.2)(+1.4) eV b.
- Published
- 2001
- Full Text
- View/download PDF
24. Interactions of Strange Mesons at Low Energies
- Author
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Avakyan, E. Z., Avakyan, S. L., Avakyan, E. Z., and Avakyan, S. L.
- Published
- 2015
25. Precision experiments and fundamental physics at low energies - Part II
- Author
-
Blaum, Klaus, Mueller, Holger, and Severijns, Nathal
- Subjects
low energies ,fundamental physics - Abstract
Co-editor of journal volume ispartof: Annalen der Physik vol:525 issue:8 pages:A127-A128 status: published
- Published
- 2013
26. Universal Energy Distribution of Quasiparticles Emitted in a Local Time-Dependent Quench
- Author
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Pietro Smacchia and Alessandro Silva
- Subjects
Energy distributions ,FOS: Physical sciences ,General Physics and Astronomy ,Perturbation (astronomy) ,Critical points ,Power law ,Settore FIS/03 - Fisica della Materia ,Quantum mechanics ,Ising chains ,Time-dependent ,Quantum statistical mechanics ,Quantum ,Condensed Matter - Statistical Mechanics ,Quasiparticles ,Transverse field ,Physics ,Statistical Mechanics (cond-mat.stat-mech) ,Low energies ,Scaling limits ,Time dependence ,Transverse magnetization ,Average values ,Correlation function ,Scaling limit ,Quantum electrodynamics ,Quasiparticle ,Exponent ,Probability distribution - Abstract
We study the emission of quasi-particles in the scaling limit of the 1d Quantum Ising chain at the critical point perturbed by a time dependent local transverse field. We compute \it exactly \rm and for a \it generic \rm time dependence the average value of the transverse magnetization, its correlation functions, as well as the statistic of both the inclusive and exclusive work. We show that, except for a cyclic perturbation, the probability distribution of the work at low energies is a power law whose exponent is universal, i.e. does not depend on the specific time dependent protocol, but only on the final value attained by the perturbation., 5 pages, 1 figure, Published Version
- Published
- 2012
- Full Text
- View/download PDF
27. Backstepping based approach for the combined longitudinal-lateral vehicle control
- Author
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Lamri Nehaoua, Lydie Nouveliere, Informatique, Biologie Intégrative et Systèmes Complexes (IBISC), and Université d'Évry-Val-d'Essonne (UEVE)
- Subjects
Vehicle Control ,Collision avoidance (spacecraft) ,Engineering ,Backstepping procedure ,Low speed ,business.industry ,Low energies ,Control engineering ,Collision avoidance maneuver ,Tracking (particle physics) ,Vehicle driving ,Control module ,Road vehicles ,Vehicle dynamics ,Lateral control ,Control theory ,Trajectory tracking ,Backstepping ,Trajectory ,Lane change ,Vehicle control ,business ,Control methods - Abstract
International audience; This paper presents an integrated control method of a light road vehicle driving on a known and high secured itinerary at low speed. A planning module sends a safe and low energy reference trajectory to a control module that permits to manage the trajectory tracking under 50 km/h. A backstepping procedure is presented and formulated to realize a coupled longitudinal and lateral control in lane change or collision avoidance maneuvers.
- Published
- 2012
- Full Text
- View/download PDF
28. Low-energy rotational inelastic collisions of H(+) + CO system
- Author
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T. J. Dhilip Kumar and Sanjay Kumar
- Subjects
Energy ranges ,Interaction potentials ,Ab initio ,Inelastic collision ,General Physics and Astronomy ,Collision energies ,Ground electronic state ,Rigid rotors ,Molecular polarizabilities ,Polarizability ,Ab initio quantum chemistry methods ,Close coupling ,Infinite-order sudden approximation ,Low collision energy ,Vibrational ground ,Low temperatures ,Physical and Theoretical Chemistry ,Rotational partition function ,Integral cross-sections ,Cross section ,Chemistry ,Low energies ,Excited states ,Quantum mechanical ,Rotational excitation ,Close coupling calculation ,Dipole ,Quantum theory ,Quadrupole ,Potential energy surface ,Quadrupole moments ,Basis sets ,Atomic physics ,Multipolar expansion ,Calculations ,Quantum chemistry ,Coupled-cluster singles - Abstract
The quantum mechanical state-to-state rotational excitation cross sections have been computed using the ab initio ground electronic state potential energy surface of the system [M. Mladenovic and S. Schmatz, J. Chem. Phys. 109, 4456 (1998)] computed at coupled-cluster single and double and triple perturbative excitations method using correlation-consistent polarized valence quadruple zeta basis set where the asymptotic potential have been computed using the dipole moment, quadrupole moment, and the molecular polarizability components and fitted to this interaction potential. The anisotropy of the surface has been analyzed in terms of the multipolar expansion coefficients for the rigid-rotor surface. The integral cross sections for rotational excitations have been computed by solving close-coupled equations at very low collision energies (5-200 cm -1) and the corresponding rates have been obtained for a range of low temperatures (5-175 K). The j = 0 ? j ? 1 rotational excitation cross section (and rate) is found to be the dominant followed by the j 0 ? j ? 2 in these collision energies. The close-coupling, coupled-state, and infinite-order sudden approximations coupling calculations have been performed in the energy range of 0.1-1.0 eV using vibrational ground potential. The rotational cross sections have been obtained by performing computationally accurate close-coupling calculations at 0.1 eV using vibrationally averaged potential (v 1) and compared with the results of vibrational ground potential. � 2012 American Institute of Physics.
- Published
- 2012
29. Powder processing and coating heat treatment on cold sprayed Ti-6Al-4V alloy
- Author
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Wilson Wong, Steve Yue, Eric Irissou, Phuong Vo, and Jean Gabriel Legoux
- Subjects
Sintering ,Micro tensile tests ,Mechanical properties ,Heat treatment temperature ,Tensile strength ,Powder flowability ,Coating ,General Materials Science ,Powder coatings ,Vanadium alloys ,Coating porosity ,Recrystallization (metallurgy) ,Coating deposition ,Cold spray ,Condensed Matter Physics ,Propellant gas ,Particle impact velocities ,Cohesion strength ,Mechanics of Materials ,Tensile testing ,Materials science ,Feedstock powders ,Nitrogen ,Alloy ,Gas dynamic cold spray ,Raw material ,engineering.material ,Heat treatment ,Ball-milled ,Ti-6al-4v ,Sprayed coatings ,Titanium alloys ,Argon ,Ti-6Al-4V alloy ,Propellant ,Nitrogen gas ,Cerium alloys ,Powder processing ,Low energies ,Mechanical Engineering ,Metallurgy ,Titanium alloy ,Static recovery ,Vanadium ,Coating hardness ,engineering ,Aluminum coatings ,Argon atmospheres ,Aluminum - Abstract
This study investigates the effect of powder processing on powder flowability, compact ability, and the heat treatment of the resulting coatings on the mechanical properties of cold gas dynamic sprayed Ti-6Al-4V alloy. Nitrogen gas was used throughout the coating deposition process. Propellant gas temperature and pressure were attuned to maximize particle impact velocity. Three powder processing conditions were used in this study: as received (AR), low-energy ball milled (BM), and argon atmosphere heat treated (HT). Results showed coating porosities of around 6 to 7%, regardless of the feedstock powder used or the heat treatment performed. It was observed at 600 and 800°C anneals that a coating hardness reduction occurred, possibly due to static recovery and recrystallization, with minor sintering possibly occurring at the 800°C anneals. In addition, micro tensile tests showed an increase in cohesion strength at higher heat treatment temperatures. © 2012 Trans Tech Publications, Switzerland., 7th International Conference on Processing and Manufacturing of Advanced Materials, THERMEC'2011, 1 August 2011 through 5 August 2011, Quebec City, QC
- Published
- 2012
30. Reconstruction of the X-ray tube spectrum from a scattering measurement
- Author
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Sergio Gallardo, Viviana Scot, Pier Luca Rossi, François Tondeur, Jonathan Bare, José Ródenas, Jorge Eduardo Fernandez, Fernandez Jorge Eduardo, Scot Viviana, Bare Jonathan, Tondeur Francois, Gallardo Sergio, Rodenas Jose, and Rossi PierLuca
- Subjects
X ray beam ,Photon ,X ray spectrum ,Mathematical parameters ,X ray spectrometry ,Rayleigh scattering ,Light scattering ,Adjoints ,law.invention ,Boltzmann equation ,Mathematical model ,law ,Unfolding techniques ,Accuracy ,Priority journal ,Physics ,Radiation ,Detector ,X-ray spectrum ,Calculation ,X-ray tube ,X-ray tube spectrum ,symbols ,Compton scattering ,Operational units ,Radiation detector ,Intensity distribution ,Radiation beam ,INGENIERIA NUCLEAR ,Particle detector ,Article ,symbols.namesake ,Optics ,Analytic method ,Artifact reduction ,Validation process ,X ray tubes ,Ill-conditioning ,Experimentation ,Quality control procedures ,business.industry ,Low energies ,Intermethod comparison ,Low energy radiation ,Scattering measurements ,Boltzmann transport equation ,Adjoint transport ,X ray tube ,Radiation measurement ,Radiation dose distribution ,business ,Inverse techniques ,Beam (structure) ,Process optimization - Abstract
An inverse technique has been designed to unfold the x-ray tube spectrum from the measurement of the photons scattered by a target interposed in the path of the beam. A special strategy is necessary to circumvent the ill-conditioning of the forward transport algebraic problem. The proposed method is based on the calculation of both, the forward and adjoint analytical solutions of the Boltzmann transport equation. After testing the method with numerical simulations, a simple prototype built at the Operational Unit of Health Physics of the University of Bologna was used to test the method experimentally. The reconstructed spectrum was validated by comparison with a straightforward measurement of the X-ray beam. The influence of the detector was corrected in both cases using standard unfolding techniques. The method is capable to accurately characterize the intensity distribution of an X-ray tube spectrum, even at low energies where other methods fail.
- Published
- 2011
31. RVC-based time-predictable faulty caches for safety-critical systems
- Author
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Abella, J., Quiñones, E., Cazorla, F. J., Valero, M., and Sazeides, Yiannakis
- Subjects
Bit rates ,Probability of failure ,Low energies ,Computer science ,business.industry ,CPU cache ,Reliability (computer networking) ,Safety critical systems ,Worst-case execution time ,Area overhead ,Life-critical system ,Safety testing ,Victim cache ,Embedded system ,Software fault tolerance ,Fraction (mathematics) ,Cache ,business - Abstract
Technology and Vcc scaling lead to significant faulty bit rates in caches. Mechanisms based on disabling faulty parts show to be effective for average performance but are unacceptable in safety critical systems where worst-case execution time (WCET) estimations must be safe and tight. The Reliable Victim Cache (RVC) deals with this issue for a large fraction of the cache bits. However, replacement bits are not protected, thus keeping the probability of failure still high. This paper proposes two mechanisms to tolerate faulty bits in replacement bits and keep time-predictability by extending the RVC. Our solutions offer different tradeoffs between cost and complexity. In particular, the Extended RVC (ERVC) has low energy and area overheads while keeping complexity at a minimum. The Reliable Replacement Bits (RRB) solution has even lower overheads at the expense of some more wiring complexity. © 2011 IEEE. 25 30 Sponsors: IEEE IEEE Computer Society tttc Conference code: 86459 Cited By :6
- Published
- 2011
- Full Text
- View/download PDF
32. Ethanol enhances collective dynamics of lipid membranes
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Mounir Tarek, Karin Schmalzl, Martin D. Kaye, Valeria Conti Nibali, and Maikel C. Rheinstädter
- Subjects
Neutron Spectroscopy ,Materials science ,Phonon ,Lipid Bilayers ,molecular motions ,transverse properties ,Molecular Conformation ,fluid-phase ,low energies ,Molecular Dynamics Simulation ,Inelastic scattering ,01 natural sciences ,03 medical and health sciences ,Molecular dynamics ,dispersions ,0103 physical sciences ,Atom ,ddc:530 ,010306 general physics ,collective dynamics ,030304 developmental biology ,0303 health sciences ,Ethanol ,Scattering ,Bilayer ,Cell Membrane ,bi-layer ,molecular dynamics simulations ,molecular dynamics ,Neutron Diffraction ,Membrane ,Chemical physics ,lipid membranes ,Atomic physics ,Dimyristoylphosphatidylcholine ,Dispersion (chemistry) ,additional mode - Abstract
From inelastic neutron-scattering experiments and all atom molecular dynamics simulations we present evidence for a low-energy dynamical mode in the fluid phase of a 1,2-dimyristoyl-sn-glycero-3-phoshatidylcholine (DMPC) bilayer immersed in a 5% water/ethanol solution. In addition to the well-known phonon that shows a liquidlike dispersion with energies up to 4.5 meV, we observe an additional mode at smaller energies of 0.8 meV, which shows little or no dispersion. Both modes show transverse properties and might be related to molecular motion perpendicular to the bilayer. © 2011 American Physical Society.
- Published
- 2011
- Full Text
- View/download PDF
33. Low Energy Electron Point Projection Microscopy of Suspended Graphene, the Ultimate 'Microscope Slide'
- Author
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Radovan Urban, Jeremy T. Robinson, Mark Salomons, Martin Cloutier, Robert A. Wolkow, L. Livadaru, Josh Mutus, and Paul E. Sheehan
- Subjects
Diffraction ,electron holography ,virtual sources ,FOS: Physical sciences ,low energies ,General Physics and Astronomy ,02 engineering and technology ,Electron ,01 natural sciences ,Electron holography ,electron beams ,law.invention ,point projection ,nano-scale objects ,strong field ,law ,Mesoscale and Nanoscale Physics (cond-mat.mes-hall) ,low energy electrons ,0103 physical sciences ,Microscopy ,knife edge ,Electron gun ,010302 applied physics ,Physics ,Condensed Matter - Mesoscale and Nanoscale Physics ,electron transmission ,business.industry ,Graphene ,graphene ,electrons ,image objects ,021001 nanoscience & nanotechnology ,electron emitters ,Anode ,microscope slide ,Cathode ray ,Optoelectronics ,covalent radii ,0210 nano-technology ,business - Abstract
Point projection microscopy (PPM) is used to image suspended graphene by using low-energy electrons (100-205 eV). Because of the low energies used, the graphene is neither damaged nor contaminated by the electron beam for doses of the order of 107 electrons per nm2. The transparency of graphene is measured to be 74%, equivalent to electron transmission through a sheet twice as thick as the covalent radius of sp2-bonded carbon. Also observed is rippling in the structure of the suspended graphene, with a wavelength of approximately 26 nm. The interference of the electron beam due to diffraction off the edge of a graphene knife edge is observed and is used to calculate a virtual source size of 4.7 ± 0.6 Å for the electron emitter. It is demonstrated that graphene can serve as both the anode and the substrate in PPM, thereby avoiding distortions due to strong field gradients around nanoscale objects. Graphene can be used to image objects suspended on the sheet using PPM and, in the future, electron holography. © IOP Publishing Ltd and Deutsche Physikalische Gesellschaft.
- Published
- 2011
34. Transmittance and optical constants of Ho films in the 3-1340 eV spectral range
- Author
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M. Fernández-Perea (1), J. Larruquert (1), J. Aznárez (1), J. Méndez (1), L. Poletto (2), F. Frassetto (2), M. Malvezzi (3), D. Bajoni (3), A. Giglia (4), N. Mahne (4), and S. Nannarone (4
- Subjects
Materials science ,Analytical chemistry ,General Physics and Astronomy ,chemistry.chemical_element ,Molar absorptivity ,Evaporation (deposition) ,Energy ranges ,Extinction coefficients ,Film substrates ,High transmittance ,In-situ ,K-values ,Lanthanides ,Low energies ,Multi-layer-coating ,Promising materials ,Room temperature ,Spectral range ,Sum rule ,Transmittance measurements ,chemistry ,Vacuum deposition ,Transmittance ,Thin film ,Holmium ,Absorption (electromagnetic radiation) ,Refractive index - Abstract
The optical constants n and k of holmium (Ho) films were obtained in the 3-1340-eV range from transmittance measurements performed at room temperature. Thin films of Ho with various thicknesses were deposited by evaporation in ultra high vacuum conditions and their transmittance was measured in situ. Ho films were deposited onto thin C-film substrates supported on high transmittance grids. Transmittance measurements were used to obtain the extinction coefficient k of Ho films. The refractive index n of Ho was calculated with Kramers-Krönig analysis; in order to do this, k data were extrapolated both on the high and on the low energy parts of the spectrum by using experimental and calculated k values available in the literature. Ho, similar to other lanthanides, has a low-absorption band below the O2,3 edge onset; the lowest absorption was measured at ∼22 eV. Therefore, Ho is a promising material for filters and multilayer coatings in the energy range below the O2,3 edge in which most materials have a large absorption. Good consistency of the data resulted from the application of f and inertial sum rules. © 2011 American Institute of Physics., This work was also supported by the National Programme for Space Research, Subdireccio´n General de Proyectos de Investigacio´n, Ministerio de Ciencia y Tecnologı´a, project numbers AYA2008-06423- C03-02/ESP, AYA2009-14070, and AYA2010-22032.
- Published
- 2011
- Full Text
- View/download PDF
35. The effects of ozone treatment on polylactic acid (PLA) fibres
- Author
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Pinar Uysal, Mike Wilding, Ozan Avinc, Hüseyin Aksel Eren, Uludağ Üniversitesi/Mühendislik Fakültesi/Tekstil Mühendisliği Bölümü., Eren, Hüseyin Aksel, and Uysal, Pınar
- Subjects
Surface damages ,Polymers and Plastics ,Disperse Dyes ,Dyeing ,Colour Fastness ,Peroxide ,Peroxide treatment ,chemistry.chemical_compound ,SEM imaging ,Polylactic acid ,Ozonation ,Fabric strength ,Chemical Engineering (miscellaneous) ,Fiber ,Composite material ,Hydrogen peroxide ,Microstructure ,Internal microstructure ,Ozone water treatment ,acid) (PLA) ,strength ,whiteness ,Whiteness ,Lactic acid ,Fiber surface ,Fibers ,Body fluids ,Rigidity ,Raman spectroscopy ,Bleaching ,Wetting ,Strength ,Polylactic acids ,bleaching ,flexural rigidity ,hydrogen peroxide ,ozone ,poly(lactic ,Materials science ,Polyester ,Flexural rigidity ,Poly(lactic acid) (PLA) ,Ozone ,poly(lactic acid) (PLA) ,Poly(lactic acid) ,Oxidation ,Treatment time ,Room temperature ,Low energies ,Poly lactic acid ,Ozonization ,chemistry ,Ozone treatment ,Flexural rigidities ,Materials science, textiles ,Higher temperatures ,Burst strength - Abstract
A set of knitted poly(lactic acid) (PLA) fabrics was ozonated at room temperature for periods ranging from one to 60 minutes in order to identify any accompanying effects on physical properties (specifically whiteness, water-absorbency, flexural rigidity and burst strength), fiber surface integrity or internal microstructure. A significant (ca. 6% after 10 minutes of treatment) initial increase in whiteness was observed, with longer treatment times producing little further change. The fabric’s absorbency and flexibility both increased, the time of wetting having fallen by ca. 20% and the flexural rigidity by ca. 16%, respectively, after 10 minutes of treatment. Fabric strength remained virtually unaffected for short times (up to 10 minutes) of ozonation, although longer treatments caused a measurable drop (ca. 10% after 60 minutes). SEM imaging showed virtually no evidence for surface damage, even after 60 minutes of treatment, whereas peroxide treatment caused massive pitting of the fiber surface. Raman spectroscopy of the ozonated PLA fabrics indicated that the treatment had not affected the internal microstructure of the fibers. Our conclusion is that brief (no more than 10 minutes) room-temperature ozonation is potentially an effective, safe and low-energy alternative to conventional higher temperature peroxide treatment. © 2011, SAGE Publications. All rights reserved.
- Published
- 2011
36. The two-photon exchange contribution to muonic hydrogen from chiral perturbation theory
- Author
-
Peset Martín, Clara María, Pineda, Antonio, Peset Martín, Clara María, and Pineda, Antonio
- Abstract
We compute the spin-dependent and spin-independent structure functions of the forward virtual-photon Compton tensor of the proton at using heavy baryon effective theory including the Delta particle. We compare with previous results when existing. Using these results we obtain the leading hadronic contributions, associated to the pion and Delta particles, to the Wilson coefficients of the lepton–proton four fermion operators in NRQED. The spin-independent coefficient yields a pure prediction for the two-photon exchange contribution to the muonic hydrogen Lamb shift, . We also compute the charge, , and Zemach, , moments for . Finally, we discuss the spin-dependent case, for which we compute the difference between the four-fermion Wilson coefficients relevant for hydrogen and muonic hydrogen., Ministerio de Ciencia e Innovación (España), Depto. de Física Teórica, Fac. de Ciencias Físicas, TRUE, pub
- Published
- 2014
37. Electron capture in highly charged ion-atom collisions
- Subjects
SELECTIVE DOUBLE CAPTURE ,HELIUM-ATOMS ,BARE IONS ,LOW ENERGIES ,CROSS-SECTIONS ,AR - Abstract
An attempt is made to identify the most important mechanisms responsible for the rearrangement of electrons during collisions between multiply charged ions and atoms at keV energies. It is discussed to which extent the influence of binding energy, angular momentum of heavy particles and electrons, and electron-electron correlation on the dynamic processes can be understood by means of simple models. Collision systems comprising only one, two, or many active electrons are distinguished, since rigorous theoretical treatments for such systems are well established, just being developed or not yet available respectively.
- Published
- 1993
38. Magneto-photoluminescence spectroscopy of single InAs/AlAs quantum dots
- Author
-
Sarkar, D., Van Der Meulen, H.P., Calleja, J.M., Meyer, J.M., Haug, Rolf J., and Pierz, K.
- Subjects
Nonresonant ,Photoluminescence spectroscopy ,Condensed Matter::Other ,Low energies ,Magnetophotoluminescence ,Quantum Dot ,Physics::Optics ,Condensed Matter::Mesoscopic Systems and Quantum Hall Effect ,Condensed Matter::Materials Science ,Semiconductor quantum dots ,ddc:530 ,Exciton localization ,Excitons ,Dewey Decimal Classification::500 | Naturwissenschaften::530 | Physik ,Acoustic phonons ,G factors ,Photoluminescence ,Magnetos ,Konferenzschrift ,Diamagnetic shifts - Abstract
We present non-resonant, polarization-resolved magneto-photoluminescence measurements up to 12 T on single InAs/AlAs quantum dots. We observe typical g-factors between 1 and 2, very low diamagnetic shifts due to strong exciton localization and low-energy sidebands, which are attributed to the piezoelectric exciton-acoustic phonon interaction. Spanish Ministry of Education/MAT2008- 01555/NAN Spanish Ministry of Education/Consolider CSD 2006-19 Community of Madrid CAMS-0505-ESP-0200 Spanish Ministry of Science and Innovation/Nanoinpho-QD TEC2008-06756-C03-01
- Published
- 2010
- Full Text
- View/download PDF
39. Design of an aberration corrected low-voltage SEM
- Subjects
electron beam ,Low energy ,Spherical aberrations ,Spheres ,Low energies ,Foil ,low voltage scanning electron microscope ,article ,Chromatic aberration ,static electricity ,scanning electron microscope ,Aberration correction ,Low voltages ,Low voltage ,Aberrations ,equipment design ,SEM ,Probes ,computer analysis ,Electronics ,Spherical aberration ,Scanning electron microscopy - Abstract
The low-voltage foil corrector is a novel type of foil aberration corrector that can correct for both the spherical and chromatic aberration simultaneously. In order to give a realistic example of the capabilities of this corrector, a design for a low-voltage scanning electron microscope with the low-voltage foil corrector is presented. A fully electrostatic column has been designed and characterised by using aberration integrals and ray tracing calculations. The amount of aberration correction can be adjusted relatively easy. The third order spherical and the first order chromatic aberration can be completely cancelled. In the zero current limit, a FW50 probe size of 1.0. nm at 1. kV can be obtained. This probe size is mainly limited by diffraction and by the fifth order spherical aberration. © 2010 Elsevier B.V.
- Published
- 2010
40. Methods for probing charging properties of polymeric materials using XPS
- Author
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Gulay Ertas, Sefik Suzer, Hikmet Sezen, and Süzer, Şefik
- Subjects
Artificial systems ,Semiconducting silicon compounds ,Photoemission spectroscopy ,Polymers ,X ray photoelectron spectroscopy ,Analytical chemistry ,Dynamics of charging ,Spectral line ,law.invention ,chemistry.chemical_compound ,Square-wave ,law ,Electrical circuit models ,Spectroscopy ,Radiation ,Series capacitors ,Esters ,Reseistance ,Condensed Matter Physics ,Atomic and Molecular Physics, and Optics ,Electronic, Optical and Magnetic Materials ,Capacitor ,Dielectric properties ,XPS spectra ,Charging ,Capacitance ,Experimental data ,Dielectric ,Capacitors ,Molecular physics ,Silicon wafers ,Dielectric materials ,Frequency dependence ,X-ray photoelectron spectroscopy ,High frequency ,X ray photoelectron spectra ,Charging property ,Blend films ,XPS ,Physical and Theoretical Chemistry ,Si wafer ,Low energies ,Resistors ,Artificial dielectric ,chemistry ,Polystyrenes ,Polystyrene ,Polymeric matreials ,Materials properties - Abstract
Various thin polystyrene, PS, and poly(methyl methacrylate), PMMA and PS + PMMA blend films have been examined using the technique of recording X-ray photoelectron spectrum while the sample is subjected to +/- 10 V d.c, bias, and three different forms of (square-wave (SQW), sinusoidal (SIN) and triangular (TRG)), a.c. pulses. All films exhibit charging shifts as observed in the position of the corresponding C1s peak under d.c. bias. The a.c. pulses convert the single C1s peak to twinned peaks in the case of the square-wave form, and distort severely in the cases of the SIN, and TRG forms, and all three of them exhibit strong frequency dependence. In order to mimic and better understand the behavior of these polymeric materials, an artificial dielectric system consisting of a clean Si-wafer coupled to an external 1 M Omega resistor and 56 nF capacitor is created, and its response to different forms of voltage stimuli, is examined in detail. A simple electrical circuit model is also developed treating the system as consisting of a parallel resistor and a series capacitor. With the help of the model, the response of the artificial system is successfully calculated as judged by comparison with the experimental data. Using one high frequency SQW measurements, the off-set in the charging shift clue to the extra low-energy neutralizing electrons is estimated. After correcting the corresponding off-set shifts, the XPS spectra of the three different PS films, one PMMA, and one PS + PMMA blend film are re-examined. As a result of these detailed analysis, there emerges a clear relationship between the thicknesses of the PS films with their charging abilities. In the blend film, PS and PMMA domains are electrically separated, and exhibit different charging shifts, however, the presence of one is felt by the other. Hence, the PS component shifts are larger in the blend, due to the presence of PMMA domains, which has intrinsically a larger R-eff, and conversely the PMMA component shifts are smaller due to the presence of PS domains. (C) 2009 Elsevier B.V. All rights reserved.
- Published
- 2010
41. Design of an aberration corrected low-voltage SEM
- Author
-
Diederik Maas, J.E. Barth, R.H. van Aken, Cornelis W. Hagen, Pieter Kruit, and TNO Industrie en Techniek
- Subjects
Diffraction ,electron beam ,Low energy ,Spheres ,Chromatic aberration ,Aberration correction ,Low voltage ,Optics ,equipment design ,Spherical aberration ,Instrumentation ,FOIL method ,Physics ,Contrast transfer function ,Spherical aberrations ,business.industry ,Low energies ,Foil ,low voltage scanning electron microscope ,article ,static electricity ,scanning electron microscope ,Atomic and Molecular Physics, and Optics ,Low voltages ,Electronic, Optical and Magnetic Materials ,Ray tracing (physics) ,Third order ,Aberrations ,SEM ,Cathode ray ,Probes ,computer analysis ,Electronics ,business ,Scanning electron microscopy - Abstract
The low-voltage foil corrector is a novel type of foil aberration corrector that can correct for both the spherical and chromatic aberration simultaneously. In order to give a realistic example of the capabilities of this corrector, a design for a low-voltage scanning electron microscope with the low-voltage foil corrector is presented. A fully electrostatic column has been designed and characterised by using aberration integrals and ray tracing calculations. The amount of aberration correction can be adjusted relatively easy. The third order spherical and the first order chromatic aberration can be completely cancelled. In the zero current limit, a FW50 probe size of 1.0. nm at 1. kV can be obtained. This probe size is mainly limited by diffraction and by the fifth order spherical aberration. © 2010 Elsevier B.V.
- Published
- 2010
42. Fabrication of ultrafine and nanocrystalline WC-Co mixtures by high energy milling
- Author
-
Bonache Bezares, Victoria, Salvador Moya, Mª Dolores, Busquets Mataix, David Jerónimo, and Segovia-López, Francisco
- Subjects
SEM and TEM ,Powder mixtures ,X ray diffraction ,Mechanical properties ,Planetary milling ,Crystallite size ,Ultrafine ,Ball milling ,Tungsten alloys ,WC-Co ,Sintering ,CIENCIA DE LOS MATERIALES E INGENIERIA METALURGICA ,Internal strains ,Processing condition ,Ball mills ,Nanocrystallines ,Nanocrystalline WC-Co ,Characterisation ,Low energies ,X ray diffraction analysis ,Nanocrystalline powders ,Wet milling ,Grain size ,Grain growth ,Microstrain ,Mixtures ,Planetary ball mill ,Diffraction ,Grain size and shape ,Milling (machining) ,Transmission electron microscopy ,Scanning and transmission electron microscopy - Abstract
[EN] In this work ultrafine and nanocrystalline WC-Co mixtures were obtained by low energy milling in planetary ball mill. The effect of the processing conditions on the reduction and distribution of the grain sizes and the internal strains level were studied. The characterisation of the powder mixtures was performed by means of scanning and transmission electron microscopy and X-ray diffraction analysis. Observations through SEM and TEM images showed a particle size below 100 nm, after milling. The X-ray diffraction profile analysis revealed a WC phase refined to a crystallite size of 19 nm. The mixtures obtained have been consolidated and mechanical and microstructurally characterised. The results show improvements in resistant behaviour of the material consolidated from nanocrystalline powders, in spite of the grain growth experienced during the sintering. The best results were found for the material obtained by wet milling during 100 h, which presents values of hardness higher than 1800 HV. © 2011 Institute of Materials, Minerals and Mining., This work has been supported by CICYT, Spain, through project no. MAT2006-12945-C03-02.
- Published
- 2009
- Full Text
- View/download PDF
43. Low energy ion scattering investigations of n-butanol-ice system in the temperature range of 110-150 K
- Author
-
Soumabha Bag, Jobin Cyriac, Thalappil Pradeep, and G. Naresh Kumar
- Subjects
Propanol ,Surface diffusion ,Diffusion ,Diffusive mixing ,Segregation (metallography) ,Analytical chemistry ,Liquid alcohols ,Ion ,chemistry.chemical_compound ,Temperature range ,Ice system ,Molecular levels ,Mass spectra ,Physical and Theoretical Chemistry ,Sputtered species ,N-butanol ,Surface energies ,Monolayers ,Ethanol ,Mass spectrometry ,Surface tension ,Low energies ,Methanol ,Ice ,Low energy ion scattering ,Atmospheric temperature range ,Thin layers ,Ultra high vacuum ,Amorphous solid water ,Surface chemistry ,Surface energy ,Surfaces, Coatings and Films ,Electronic, Optical and Magnetic Materials ,Amorphous solid ,General Energy ,chemistry ,Low-energy ion scattering ,Water ice ,Mass spectrum ,Isomeric alcohols ,Selective ionization ,Ionization of liquids ,Tert-butyl alcohols ,Mass spectrometers ,Surface segregation - Abstract
We have investigated the interaction of n-butanol (NBA) with thin layers of water ice prepared in ultra high vacuum in the temperature range of 110-150 K. From the mass spectra of the chemically sputtered species, created upon the collision of low energy (?30 eV) Ar + ions, we study the process of diffusive mixing of NBA with water ice, at the molecular level. The results show that NBA undergoes diffusive mixing with H 2O. Even after depositing 1000 monolayers (MLs) of amorphous solid water (ASW) over NBA, both the species are observed on the surface. However, when NBA is deposited over ASW, no water is seen on the surface above 3-5 MLs of NBA. This could be interpreted as the absence of diffusive mixing in this system or surface segregation of NBA, in view of its lower surface energy just as in the case of liquid alcohols. An isomeric alcohol, namely, tert-butyl alcohol (TBA), also behaves similarly. Although the presence of NBA and TBA is detected, in the presence of ASW, they undergo selective ionization, giving specific peaks in the mass spectrum. D 2O behaves in a manner similar to that of H 2O. Preliminary experiments with other alcohols; namely, methanol, ethanol, and propanol were also done, and the results suggest that incomplete diffusion or surface segregation begins with propanol. � 2009 American Chemical Society.
- Published
- 2009
44. Response of polyelectrolyte layers to the SiO2 substrate charging as probed by XPS
- Author
-
Sefik Suzer, Can Pinar Conger, and Süzer, Şefik
- Subjects
Semiconducting silicon compounds ,Counter-ions ,Polarity changes ,Polymers ,X ray photoelectron spectroscopy ,Binding energy ,Analytical chemistry ,Substrate (electronics) ,Cationic polyelectrolytes ,chemistry.chemical_compound ,Electrolytes ,Photoemission process ,External potentials ,Electrochemistry ,Silicon dioxide ,Silicon compounds ,General Materials Science ,Underlayer ,Spectroscopy ,Chemistry ,Bilayer ,Polyelectrolyte layers ,Bi layers ,Surfaces and Interfaces ,Condensed Matter Physics ,Silicon Dioxide ,Polyelectrolytes ,Polyelectrolyte ,Layer-by-layer techniques ,Layer (electronics) ,Electrical stimulus ,Second layers ,Hot electrons ,Atoms ,Binding sites ,Oxide ,Overlayer ,X-ray photoelectron spectroscopy ,Potential energy ,Xps ,Positively charged ,Substrate charging ,Substrates ,Low energies ,Spectrum Analysis ,Hot filaments ,Oxide layers ,Nuclear energy ,Silicon substrates ,Intensity alterations ,Single layers ,Spectrum analysis ,Molecular Probes ,Molecular probes - Abstract
A single layer of the Cationic polyelectrolyte poly(allyamine) hydrochloride (PAH) deposited, using the layer-by-layer technique, on a silicon substrate containing 5 nm oxide layer is investigated by XPS while applying an external potential bias to the sample to control and manipulate the charge built-up on the oxide layer. Under application of a -10 V bias, the oxide layer is positively charged due to Photoemission process, evidenced by the measured Si2p binding energy of 104.4 eV. Application of a +10 V bias attracts the low energy neutralizing electrons, stemming from a hot filament, and leads to a negatively charged oxide layer, also evidenced by the measured Si2p binding energy of 102.9 eV. The single polyelectrolyte overlayer also responds to this polarity change of the oxide layer underneath by displaying a somewhat larger shifts both in the C1s and Nls peaks. In addition to the shifts in the positions, the N1s peaks undergo a significant intensity depletion, mostly on the positively charged -N+ component. We interpret this intensity depletion to be the result of reorientation of some of the dangling positively charged groups by moving toward the negatively charged oxide underlayer. To our knowledge this is the first time that a chemically specific response to an electrical stimuli is reported using XPS. A bilayer LbL film consisting of PAH and PSS, exhibits even a larger charging shift, but this time no intensity alteration is observed, most probably due to locking of the -N+ groups by the -SO3 + counterions of the second layer. © 2009 American Chemical Society.
- Published
- 2009
45. Excitation functions of 6,7Li+7Li reactions at low energies.
- Author
-
Prepolec, L., Soic, N., Blagus, S., Miljanic, Đ., Siketic, Z., Skukan, N., Uroic, M., and Milin, M.
- Subjects
- *
NUCLEAR excitation , *NUCLEAR reactions , *PARTICLES (Nuclear physics) , *TELESCOPES , *NUCLEAR physics - Abstract
Differential cross sections of 6,7Li+7Li nuclear reactions have been measured at forward angles (10°and 20°), using particle identification detector telescopes, over the energy range 2.75–10.00 MeV. Excitation functions have been obtained for low-lying residual-nucleus states. The well pronounced peak in the excitation function of 7Li(7Li,4He)10Be(3.37 MeV,2+) at beam energy about 8 MeV, first observed by Wyborny and Carlson in 1971 at 0°, has been observed at 10°, but is less evident at 20°. The cross section obtained for the 7Li(7Li,4He)10Be(g.s,0+) reaction is about ten times smaller. The well pronounced peak in the excitation function of 7Li(7Li,4He)10Be(3.37 MeV,2+) reaction could correspond to excited states in 14C, at excitation energies around 30 MeV. [ABSTRACT FROM AUTHOR]
- Published
- 2009
- Full Text
- View/download PDF
46. Stopping Power of Au for Ti Using Elastic Recoil Technique.
- Author
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Linares, R., Freire, J. A., Ribas, R. V., Medina, N. H., Oliveira, J. R. B., Seale, W. A., Cybulska, E. W., Wiedemann, K. T., Allegro, P. R., and Toufen, D. L.
- Subjects
- *
HEAVY ions , *ELASTIC scattering , *ATOMS , *RADIOACTIVE nuclear beams , *NUCLEAR reactions , *NUCLEAR physics - Abstract
The slowing down of heavy ions in matter is still not well understood especially at low energies (<0.5 MeV/u). In this contribution we present new experimental data for the stopping power of Au for Ti ions using an elastic recoil technique where a heavy-ion beam at low energies is produced by elastic scattering of an energetic primary beam imping on a thin target. Atoms from the target recoil at low energies. We compare our experimental data with previous data and with semi-empirical and theoretical models. [ABSTRACT FROM AUTHOR]
- Published
- 2009
- Full Text
- View/download PDF
47. On the accuracy of density-functional theory exchange-correlation functionals for H bonds in small water clusters. II. The water hexamer and van der Waals interactions
- Author
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Matthias Scheffler, Martin Fuchs, Angelos Michaelides, Claudia Filippi, Biswajit Santra, and Alexandre Tkatchenko
- Subjects
Materials science ,Hexamers ,Perturbation techniques ,Correlation functionals ,Quantum Monte Carlo ,Total energies ,Physics [G04] [Physical, chemical, mathematical & earth Sciences] ,General Physics and Astronomy ,Thermodynamics ,Functional theories ,H bonds ,Random hexamer ,Dissociation (chemistry) ,Total interaction energies ,Dissociation energies ,Isomers ,symbols.namesake ,Van der Waals forces ,Second orders ,Physics::Atomic and Molecular Clusters ,Reference datums ,Van der Waals ,Limit (mathematics) ,Physics::Chemical Physics ,Physical and Theoretical Chemistry ,Perturbation theory ,Diffusion (business) ,Water hexamer ,Functionals ,Wave functions ,Basis set ,Complete basis sets ,Time varying systems ,Low energies ,Van der Waals interactions ,Liquid waters ,Plesset perturbation theories ,Functional simulations ,Xc functionals ,Water clusters ,Diffusion quantum monte carlo ,Physique [G04] [Physique, chimie, mathématiques & sciences de la terre] ,Energy isomers ,symbols ,Density functional theory ,van der Waals force ,Flow interactions ,Dissociation - Abstract
Second order Møller–Plesset perturbation theory at the complete basis set limit and diffusion quantum Monte Carlo are used to examine several low energy isomers of the water hexamer. Both approaches predict the so-called prism to be the lowest energy isomer, followed by cage, book, and cyclic isomers. The energies of the four isomers are very similar, all being within 10–15 meV/H2O. These reference data are then used to evaluate the performance of several density-functional theory exchange-correlation (xc) functionals. A subset of the xc functionals tested for smaller water clusters [I. Santra et al., J. Chem. Phys. 127, 184104 (2007)] has been considered. While certain functionals do a reasonable job at predicting the absolute dissociation energies of the various isomers (coming within 10–20 meV/H2O), none predict the correct energetic ordering of the four isomers nor does any predict the correct low total energy isomer. All xc functionals tested either predict the book or cyclic isomers to have the largest dissociation energies. A many-body decomposition of the total interaction energies within the hexamers leads to the conclusion that the failure lies in the poor description of van der Waals (dispersion) forces in the xc functionals considered. It is shown that the addition of an empirical pairwise (attractive) C6R−6 correction to certain functionals allows for an improved energetic ordering of the hexamers. The relevance of these results to density-functional simulations of liquid water is also briefly discussed.
- Published
- 2008
48. Phase shift analysis of the 12C (P,P)12C process differential cross sections at low energies
- Author
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Burtebayev, N., Chechin, L. M., Dubovichenko, S. B., Zazulin, D. M., and Bölüm Yok
- Subjects
Faz kayması analizi ,Low energies ,12C (P, P) 12C proses diferansiyel kesitleri ,Phase shift analysis ,Düşük enerjiler ,12C (P,P)12C process differential cross sections - Abstract
Turkish International Cooperation Agency.
- Published
- 2008
49. Resonance raman spectra of TNT and RDX using vibronic theory, excited-state gradient, and complex polarizability approximations
- Author
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Al-Saidi, W. A., Asher, S. A., Norman, Patrick, Al-Saidi, W. A., Asher, S. A., and Norman, Patrick
- Abstract
Geometries, UV absorption bands, and resonance Raman (RR) cross sections of TNT and RDX are investigated using density functional theory (DFT) in conjunction with the Coulomb attenuated B3LYP exchange-correlation functional. The absorption and RR spectra are determined with use of vibronic (VB) theory, excited-state gradient, and complex polarizability (CPP) approximations. We examined low-energy isomers (two for TNT and four for RDX) whose energies differ by less than 1 kcal/mol, such that they would appreciably be populated at room temperature. The two TNT isomers differ by an internal rotation of the methyl group, while the four conformers of RDX differ by the arrangements of the nitro group relative to the ring. Our theoretical optical properties of the TNT and RDX isomers are in excellent agreement with experimental and recent CCSD-EOM results, respectively. For the two TNT isomers, the ultraviolet RR (UVRR) spectra are similar and in good agreement with recently measured experimental results. Additionally, the UVRR spectra computed using the excited-state and CPP approaches compare favorably with the VB theory results. On the other hand, the RR spectra of the RDX conformers differ from one another, reflecting the importance of the positioning of the NO 2 groups with respect to the ring. In the gas phase or in solution, RDX would give a spectrum associated with a conformationally averaged structure. It is encouraging that the computed spectra of the conformers show similarities to recent measured RDX spectra in acetonitrile solution, and reproduce the 10-fold decrease in the absolute Raman cross sections of RDX compared to TNT for the observed 229 nm excitation. We show that in TNT and RDX vibrational bands that couple to NO 2 or the ring are particularly resonance enhanced. Finally, the computed RDX spectra of the conformers present a benchmark for understanding the RR spectra of the solid-phase polymorphs of RDX., QC 20240110
- Published
- 2012
- Full Text
- View/download PDF
50. Reconstruction of the X-ray tube spectrum from a scattering measurement
- Author
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Universitat Politècnica de València. Departamento de Ingeniería Química y Nuclear - Departament d'Enginyeria Química i Nuclear, Fernandez, Jorge E., Scot, Viviana, Bare, Jonathan, Tondeur, François, Gallardo Bermell, Sergio, Ródenas Diago, José, Luca Rossi, Pier, Universitat Politècnica de València. Departamento de Ingeniería Química y Nuclear - Departament d'Enginyeria Química i Nuclear, Fernandez, Jorge E., Scot, Viviana, Bare, Jonathan, Tondeur, François, Gallardo Bermell, Sergio, Ródenas Diago, José, and Luca Rossi, Pier
- Abstract
An inverse technique has been designed to unfold the x-ray tube spectrum from the measurement of the photons scattered by a target interposed in the path of the beam. A special strategy is necessary to circumvent the ill-conditioning of the forward transport algebraic problem. The proposed method is based on the calculation of both, the forward and adjoint analytical solutions of the Boltzmann transport equation. After testing the method with numerical simulations, a simple prototype built at the Operational Unit of Health Physics of the University of Bologna was used to test the method experimentally. The reconstructed spectrum was validated by comparison with a straightforward measurement of the X-ray beam. The influence of the detector was corrected in both cases using standard unfolding techniques. The method is capable to accurately characterize the intensity distribution of an X-ray tube spectrum, even at low energies where other methods fail.
- Published
- 2012
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