147 results on '"D. Deleanu"'
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2. Separation of the 1+/1− parity doublet in 20Ne
- Author
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J. Beller, C. Stumpf, M. Scheck, N. Pietralla, D. Deleanu, D.M. Filipescu, T. Glodariu, W. Haxton, A. Idini, J.H. Kelley, E. Kwan, G. Martinez-Pinedo, R. Raut, C. Romig, R. Roth, G. Rusev, D. Savran, A.P. Tonchev, W. Tornow, J. Wagner, H.R. Weller, N.-V. Zamfir, and M. Zweidinger
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Physics ,QC1-999 - Abstract
The (J,T)=(1,1) parity doublet in 20Ne at 11.26 MeV is a good candidate to study parity violation in nuclei. However, its energy splitting is known with insufficient accuracy for quantitative estimates of parity violating effects. To improve on this unsatisfactory situation, nuclear resonance fluorescence experiments using linearly and circularly polarized γ-ray beams were used to determine the energy difference of the parity doublet ΔE=E(1−)−E(1+)=−3.2(±0.7)stat(−1.2+0.6)sys keV and the ratio of their integrated cross sections Is,0(+)/Is,0(−)=29(±3)stat(−7+14)sys. Shell-model calculations predict a parity-violating matrix element having a value in the range 0.46–0.83 eV for the parity doublet. The small energy difference of the parity doublet makes 20Ne an excellent candidate to study parity violation in nuclear excitations. Keywords: Parity doublet, Parity violation
- Published
- 2015
- Full Text
- View/download PDF
3. Cardiac rupture after ST elevation myocardial infarction – a decade's experience of a tertiary cardiology centre
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C Margineanu, E L Antohi, S Bubenek, A Carp, D Deleanu, D Filipescu, R Filipescu, O D Geavlete, V Iliescu, B Radulescu, O Stiru, E Stoica, and O Chioncel
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Cardiology and Cardiovascular Medicine - Abstract
Mechanical complications post ST elevation myocardial infarction (STEMI) are life-threating events, that require rapid recognition and appropriate management. Clinical diagnosis, considering high index of suspicion and bedside echocardiography should be considered in all STEMI patients Despite the overall decrease of the incidence of cardiac rupture (CR) secondary to STEMI in context of early revascularization and the wide availability of primary PCI, CR has still an unacceptable high mortality. Purpose To provide demographic, clinical, management and prognostic data associated to cardiac rupture from a tertiary centre of cardiology in Romania and to better describe in-hospital trajectory. The primary endpoint was defined as the incidence of CR and secondary endpoints were rate of surgical interventions, in-hospital mortality rate at 24 hours and after 24 hours during index hospitalization. Methods The analysis of the electronic medical records retrospectively identified 7703 patients admitted for STEMI between 01 Jan 2011 and 31 Dec 2020. A database consisting of demographic data, medical history, cv and non-cv comorbidities, in-hospital management were recorded using an UiPath robotic process automation (RPA) technology. Characteristics of the patients +/− CR were compared, and data analysis was performed using SPSS 26 Ed. Results Of a total number of 7703 consecutive STEMI patients, CR has been identified in 185 patients (mean incidence of 2.4%). The annual rates for CR incidence remained stable during the past decade (Figure 1). Patients with CR were older compared with non-CR (71.6±10.2 vs 61.47±12.8 years; p The CR patients had more comorbidities and CV risk factors – HTN, smoker status, DLP, more AF, CKD, obesity and chronic cognitive deficit (p Among the CR group patients, anterior MI was the frequent localisation (52%), followed by inferior MI (17%), infero-lateral (23%) and RV involvement MI (6.4%). According to the type of the mechanical complication, patients developed free wall rupture (50% of cases), 39% IVS rupture and 11% papillary muscle was involved; A number of 50 patients (27%), benefited from emergent cardiac surgery and 31.3% of CR patients received mechanical circulatory support. The overall STEMI mortality in the first 24-hours was 1.84% and in most of these patients the main cause of death was related to CR (31%). Overall total in-hospital mortality was 8.08% (6.5% non-CR group vs. 70.8% the CR group – Figure 1). Conclusions The study presents the epidemiological characteristics of CR complicating STEMI in the largest tertiary cardiovascular hospital in Romania. We have identified a stable trend for the incidence of CR incidence among patients with STEMI. In spite of the high rate of cardiac surgery and MCS, in-hospital mortality remains very high, particularly in the first 24 h since admission Funding Acknowledgement Type of funding sources: None.
- Published
- 2022
4. Structure of the low-lying states in Pd99,101,103,105
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D. Ivanova, S. Lalkovski, C. Costache, S. Kisyov, C. Mihai, N. Mǎrginean, P. Petkov, L. Atanasova, D. Bucurescu, R. B. Cakirli, M. P. Carpenter, R. F. Casten, Gh. Cǎta-Danil, I. Cǎta-Danil, D. Deleanu, D. Filipescu, N. Florea, I. Gheorghe, D. Ghiţǎ, T. Glodariu, F. G. Kondev, R. Lica, R. Mǎrginean, A. Negret, S. Pascu, T. Sava, E. A. Stefanova, L. Stroe, G. Suliman, R. Suvaila, O. Yordanov, and N. V. Zamfir
- Published
- 2022
5. On a method of estimating chaos control parameters from time series
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D Deleanu
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lcsh:V ,Series (mathematics) ,Computer science ,Mechanical Engineering ,Ocean Engineering ,Management Science and Operations Research ,Computer Science Applications ,CHAOS (operating system) ,Modeling and Simulation ,Applied mathematics ,Electrical and Electronic Engineering ,Control parameters ,lcsh:Naval Science ,Instrumentation - Abstract
The algorithm of Ott, Grebogi and Yorke (OGY) is recognized for its efficiency in controlling chaotic dynamical systems, even if the system’s equations are not known and the input data are provided by measured time series in experimental settings. Recently, Santos and Graves (SG) proposed a simple method for estimating the chaos control parameters required by OGY algorithm and applied it to the logistic map. Using only two time series of 100 values, they obtained approximate results for the fixed point case within 2 % of the analytical ones. Although the outputs refer only to a particular case, their conclusion seems to be that the method works as well as in general. To check this statement, we performed a large amount of numerical simulations on different one – dimensional maps. With slight different nuances, our findings were the same so we only presented in the paper the logistic map case. We have noticed that the use of only two short time series implies high risks in a reasonable estimate of the location of the fixed points and of the two control parameters (especially of the second). For large enough number of time series (three or five sets of 400 values each, in the paper) the results provided by numerical simulation approximated the theoretical ones within the limit of a few percent at most. The role played by each method parameter, as the radius for a close encounter of the fixed point or the number of the series and their lengths, is also investigated.
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- 2018
6. Exhaust Gas Recirculation (EGR) valve, design and computational fluid dynamic analysis
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C L Dumitrache, D Deleanu, and B Hnatiuc
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business.industry ,Environmental science ,Exhaust gas recirculation ,Mechanics ,business - Abstract
All EGR systems used on contemporary cars operate on the principle of “external” exhaust gas recirculation. A certain proportion of the engine exhaust gases is extracted and transmitted back into the fresh air-gasoline mixture by means of a control valve. Exhaust gas recirculation valve is generally controlled by a pneumatic or mechanical system designed to dose the exhaust gases in accordance with certain factors such as: engine speed; intake manifold pressure; engine temperature. This paper presents the design steps of the EGR valve using NX SIEMENS. After making the 3D model, it was imported into ANSYS where a study of the flow of fluids (flue gases CO2 and liquid coolant) was made. In this study it was considered that the valve was actuated and the exhaust gases enter the engine while they are also cooled by the liquid coolant. From the fluid flow modeling process it can be seen that the coolant does not take much of the flue gas temperature, its role being more to maintain a proper temperature of the body valve.
- Published
- 2021
7. Computational NX Fluid Structure Interaction (FSI) analysis on naval three way ball valve
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D Deleanu and C L Dumitrache
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Discretization ,Computer science ,Ball valve ,Component (UML) ,Fluid–structure interaction ,Work (physics) ,Mechanical engineering ,Computer Aided Design ,Boundary value problem ,computer.software_genre ,computer ,Domain (software engineering) - Abstract
This article represents the continuation of a study that was presented in another paper using the NX Siemens CAD program and FSI (fluid structure interaction analysis) for a complex valve encountered in the naval domain, a ball valve known as (three way ball valve -TWB). In designing of this valve presented in the previous work, some drawings (sketches) of the component parts presented in engineering guidelines were used, all dimensions being determined by the author. In the FSI analysis the same NX Siemens program was used to discretize the solid bodies of the valve coming into contact with the fluid, materials were chosen for these bodies, boundary conditions were set and the pressure field exerted by the fluid on the solid bodies was imported. Finally a series of conclusions were drawn about the speeds, pressures of the fluid and how they are distributed on the walls of the valve, determining the so-called structural analysis “fluid structure interaction”.
- Published
- 2021
8. The nonlinear ship rolling and safe basin erosion in stochastic beam seas
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D Deleanu and C L Dumitrache
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Nonlinear system ,Beam (nautical) ,Erosion ,Geotechnical engineering ,Structural basin ,Geology - Abstract
A short number of steep breaking waves hitting a ship from the side may affect its dynamic behaviour and determine extreme roll angles and, eventually, capsizing. Even the capsize is a rare event, its consequences for the ship and crew are often fatal. Generally, the ship rolling in regular or stochastic beam seas could be described by a second-order non-linear differential equation with the roll angle as dependent variable. Non-linearity comes from the restoring and damping moments, which are usually represented by polynomials of roll angle or of its time derivative. In the paper, we used such a model equation to estimate the ship rolling and capsizing in a stochastic beam sea. The sea action was simulated by a harmonic function with random frequency and phase. The roll equation was solved using a simple, fast and accurate iterative scheme based on Taylor expansion which proved to be very competitive in terms of accuracy with more elaborate methods and which allowed a substantial reduction of the CPU time. Due to these properties of the scheme, we were able to conduct an extensive investigation on fractal erosion of safe basins and to represent the boundaries between capsizing and non-capsizing regions in wave frequency – wave amplitude plane and normalized integrity curves for different combinations of random wave parameters. The restoring and damping coefficients corresponded to a vehicle ferry model, considered to be either with or without bilge keels.
- Published
- 2021
9. Nanosecond lifetime measurements of Iπ=9/2- intrinsic excited states and low-lying B(E1) strengths in 183Re using combined HPGe-LaBr3 coincidence spectroscopy
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R. Britton, D. Ghita, D. Deleanu, T. Sava, R. T. Wood, A. Olacel, Alison Bruce, Ioana Gheorghe, I. Cǎta-Danil, V. Werner, T. Glodariu, N. Florea, R. Mǎrginean, K.F. Mulholland, N. Alkhomashi, L. Stroe, P. J. R. Mason, Raymond J. Carroll, D. Bucurescu, Zs. Podolyák, T. Alharbi, P. A. Söderström, T. Daniel, C. Mihai, N. Mǎrginean, P. H. Regan, L. A. Gurgi, R. Lice, S. Toma, A. Negret, Oliver J. Roberts, A.D. Bajoga, R. Suvaila, and E. Wilson
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Physics ,Radiation ,010308 nuclear & particles physics ,Gamma ray ,01 natural sciences ,Electromagnetic radiation ,Semiconductor detector ,Nuclear physics ,Excited state ,0103 physical sciences ,Gamma spectroscopy ,Atomic physics ,Electric dipole transition ,Nuclear Experiment ,010306 general physics ,Spectroscopy ,Excitation - Abstract
This paper presents precision measurements of electromagnetic decay probabilities associated with electric dipole transitions in the prolate-deformed nucleus 183Re. The nucleus of interest was formed using the fusion evaporation reaction 180Hf(7Li,4n)183Re at a beam energy of 30 MeV at the tandem accelerator at the HH-IFIN Institute, Bucharest Romania. Coincident decay gamma rays from near-yrast cascades were detected using the combined HPGe-LaBr3 detector array ROSPHERE. The time differences between cascade gamma rays were measured using the LaBr3 detectors to determine the half-lives of the two lowest lying spin-parity 9/2- states at excitation energies of 496 and 617 keV to be 5.65(5) and 2.08(3) ns respectively. The deduced E1 transition rates from these two states are discussed in terms of the K-hindrance between the low-lying structures in this prolate-deformed nucleus.
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- 2017
10. The ROSPHERE γ-ray spectroscopy array
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M. Ivascu, A. Olacel, C. Mihai, S. Toma, I. Căta-Danil, D. Ghiţă, G. Suliman, G. Ciocan, C. R. Niţă, Andreea Iren Serban, C. Costache, Gh. Căta-Danil, Alexandru Negret, R. Mărginean, Zs. Podolyák, A. Dewald, N. Florea, Thomas Braunroth, S. Pascu, L. Stroe, R. Dima, C. A. Ur, D. Deleanu, C. Fransen, Ioana Gheorghe, R. Suvaila, Oliver J. Roberts, P. H. Regan, N. Marginean, D. Bucurescu, R. Lica, D. M. Filipescu, I. O. Mitu, T. Sava, Alison Bruce, N. V. Zamfir, and T. Glodariu
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Physics ,Nuclear and High Energy Physics ,Scintillation ,Physics::Instrumentation and Detectors ,010308 nuclear & particles physics ,business.industry ,Detector ,Scintillator ,01 natural sciences ,Particle detector ,Semiconductor detector ,Optics ,Nuclear magnetic resonance ,0103 physical sciences ,Scintillation counter ,Gamma spectroscopy ,010306 general physics ,business ,Spectroscopy ,Instrumentation - Abstract
The ROmanian array for SPectroscopy in HEavy ion REactions (ROSPHERE) has been designed as a multi-detector setup dedicated to γ-ray spectroscopy studies at the Bucharest 9 MV Tandem accelerator. Consisting of up to 25 detectors (either Compton suppressed HPGe detectors or fast LaBr3(Ce) scintillator detectors) together with a state of the art plunger device, ROSPHERE is a powerful tool for lifetime measurements using the Recoil Distance Doppler Shift (RDDS) and the in-beam Fast Electronic Scintillation Timing (FEST) methods. The array's geometry, detectors, electronics and data acquisition system are described. Selected results from the first experimental campaigns are also presented.
- Published
- 2016
11. Naval U-tube Heat Exchanger, design and CFX analysis
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C L Dumitrache and D Deleanu
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Engineering ,business.industry ,Component (UML) ,Heat transfer ,Heat exchanger ,Fluid dynamics ,Mechanical engineering ,Tube (fluid conveyance) ,CAD ,Engineering design process ,business ,Domain (software engineering) - Abstract
Heat exchangers are common devices on board' ships, but also in the oil-chemical industry. In this paper is presented an U-tube heat-exchanger that was designed with NX Siemens. The component parts of this heat exchanger, the CAD models and their assembly mode in the final part are presented. It is known that the design of a heat exchanger is a real challenge, and the dimensions of the component parts are established according to some standards, engineering design guidelines and to the industrial domain where they are used. The dimensions of our device were established by the author by consulting specialized works. The details of how the component parts were designed, the CAD instructions used and the constraints applied to the component parts in the final assembly are presented in details. Subsequently, the final assembly is taken over in ANSYS where a CFX analysis of fluid flow is performed and a study of the heat transfer between the two fluids.
- Published
- 2020
12. Sloshing effect, Fluid Structure Interaction analysis
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D. Deleanu and C. L. Dumitrache
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Materials science ,Slosh dynamics ,Fluid–structure interaction ,Mechanics - Published
- 2020
13. Controlling the parametric roll of a container ship model by changing the forward velocity
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D. Deleanu and C. L. Dumitrache
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Container (abstract data type) ,Forward velocity ,Geology ,Marine engineering ,Parametric statistics - Abstract
Parametric roll on ships is a resonance phenomenon whose onset causes heavy roll oscillations leading to dangerous situations for the ship, the cargo and the crew. It affects both small vessels with marginal stability and large container ships if four conditions are met simultaneously: the wave length and ship length are approximately equal, the frequency of encounter wave is twice the roll natural frequency, the ship’s roll damping is low enough and the wave height exceeds a limit value characteristic to each vessel. A good start to capture the basic features of the parametric roll is to cancel the couplings between roll and the other motions of the ship and to analyse the influence of parameters on the ship stability and the appearance of large roll amplitudes by using one-degree-of-freedom model. By doing this, one realizes that, besides increasing the damping, the roll motion can be stabilized by changing the wave encounter frequency in such a way that the resonance condition is no longer fulfilled. Two parameters mainly affect the encounter frequency: the ship forward velocity and the heading angle. In the paper, we have numerically investigated the effect of increasing or decreasing the forward speed on the roll amplitudes. We followed two strategies. In the first, we allowed the speed to change with a constant acceleration (positive or negative) so that the encounter frequency has left the dangerous region of the resonance. In the second strategy, we changed the forward speed up and down around a value that generates large roll amplitudes, by using different periodic profiles such as sinusoidal, saw tooth or trapezoidal. We noticed that both control techniques generally managed to significantly reduce the roll amplitudes (with a few exceptions). At the same time, we found that very important in how the amplitudes diminish are parameters like the moment of time when the control is activated, the speed rate of change or the period and amplitude of the speed change around the average value (in the second strategy). The data used in the paper have been obtained from experiments with a container ship model in a towing tank followed by expansion to a full scale ship.
- Published
- 2020
14. An accurate and fast iterative scheme for estimating the ship rolling and capsizing in regular waves
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F V Panaitescu, M Panaitescu, and D Deleanu
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Scheme (programming language) ,Computer science ,Control theory ,Regular wave ,Capsizing ,computer ,computer.programming_language - Abstract
A short number of steep breaking waves hitting a ship from the side may affect its dynamic behaviour and to determine extreme roll angles and, eventually, capsizing. This last phenomenon is a challenging task for naval engineers because it is responsible not only for a lot of material damages, but also for human lives. It is therefore not surprising that there have been published many relevant theoretical and experimental studies on heavy rolling and capsizing but the problem is not yet fully resolved. Generally, the ship rolling in beam regular seas could be described by a second-order non-linear differential equation with the roll angle as dependent variable. Non-linearity comes from the restoring and damping moments, which are usually represented by (odd) polynomials of roll angle or of its time derivative. Numerical integrators incorporated in modern software packages (e.g. ode45 in Matlab) encounter efficiency problems for the unbounded solutions associated with capsizing, the running time being extremely high. The alternative is to write a computer software, appropriate to the topic to be solved. In the paper, the roll equation was solved using a simple, fast and accurate iterative scheme based on Taylor expansion. Compared with Runge-Kutta 4th order numerical technique, the used scheme demonstrated not only an excellent agreement of the results, but also a significant reduction of the CPU time. The rapidity of the scheme allowed us to conduct a comprehensive investigation on fractal erosion of safe basins and to represent the normalized integrity curves and the amplitude-frequency response curves for different combinations of wave parameters. The restoring and damping coefficients corresponded to a vehicle ferry model, considered to be either intact or damaged, on the one hand, and with or without bilge keels, on the other.
- Published
- 2020
15. Separation of the 1+/1− parity doublet in 20Ne
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Jacob Beller, Andrea Idini, Norbert Pietralla, E. Kwan, Marcus Scheck, D. Deleanu, Anton Tonchev, Robert Roth, Wick Haxton, Markus Zweidinger, T. Glodariu, Werner Tornow, R. Raut, Deniz Savran, H. R. Weller, D. M. Filipescu, Christina Stumpf, J. H. Kelley, Gabriel Martínez-Pinedo, Gencho Rusev, Christopher Romig, N. V. Zamfir, and J. Wagner
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Physics ,Nuclear and High Energy Physics ,High Energy Physics::Phenomenology ,Nuclear resonance fluorescence ,High Energy Physics::Experiment ,Parity (physics) ,Matrix element ,Atomic physics ,Nuclear Experiment - Abstract
The ( J , T ) = ( 1 , 1 ) parity doublet in 20 Ne at 11.26 MeV is a good candidate to study parity violation in nuclei. However, its energy splitting is known with insufficient accuracy for quantitative estimates of parity violating effects. To improve on this unsatisfactory situation, nuclear resonance fluorescence experiments using linearly and circularly polarized γ -ray beams were used to determine the energy difference of the parity doublet Δ E = E ( 1 − ) − E ( 1 + ) = − 3.2 ( ± 0.7 ) stat ( − 1.2 + 0.6 ) sys keV and the ratio of their integrated cross sections I s , 0 ( + ) / I s , 0 ( − ) = 29 ( ± 3 ) stat ( − 7 + 14 ) sys . Shell-model calculations predict a parity-violating matrix element having a value in the range 0.46–0.83 eV for the parity doublet. The small energy difference of the parity doublet makes 20 Ne an excellent candidate to study parity violation in nuclear excitations.
- Published
- 2015
16. Absolute Cross Sections for Proton Induced Reactions on 147,149Sm Below the Coulomb Barrier
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D. Bucurescu, N. Marginean, Ioana Gheorghe, I. Căta-Danil, C. Mihai, A. Negret, R. Mărginean, G. Cata-Danil, M. Ivascu, T. Glodariu, D. Deleanu, D. M. Filipescu, R. Lica, O. Sima, L. Stroe, S. Toma, M. Sin, D. Ghita, and T. Sava
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Physics ,Nuclear physics ,Nuclear and High Energy Physics ,education.field_of_study ,Isotope ,Nucleosynthesis ,Population ,Nuclear data ,Coulomb barrier ,Model parameters ,Atomic physics ,Activation method ,education - Abstract
Cross sections for 147,149 Sm(p,n) 147,149 Eu and 147,149 Sm(p, γ ) 148,150 Eu were measured using the activation method. The results are compared to the predictions of the Hauser-Feshbach statistical model. Different γ -ray strength functions have been tested against the experimental values. In the case of 150 Eu, in order to reproduce the experimental isomeric population cross sections, various scenarios for unknown branching ratios of certain discrete states have been discussed. The results provide constraints for the optical model parameters dedicated to this insufficiently known area of isotopes. Such cross sections for (p, γ ) reactions at energies below the Coulomb barrier are valuable for p -process nucleosynthesis calculations.
- Published
- 2014
17. Explicit finite difference schemes for solving the one – dimensional tsunami wave propagation equations
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C. L. Dumitrache and D. Deleanu
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Algebra ,History ,Thesaurus (information retrieval) ,Tsunami wave ,Computer science ,Explicit finite difference ,Physics::Geophysics ,Computer Science Applications ,Education - Abstract
Because the tsunami wavelength is much longer than the sea depth, the propagation of this powerful destructive wave can be modelled by the non-linear shallow water equations (SWEs). To solve accurately these hyperbolic partial differential equations, one can resort to a variety of numerical techniques, including finite difference method (FDM) or finite volume method (FVM). In this paper, we have selected FDM, as a well verified instrument on other fluid flow problems, to estimate the tsunami wave propagation in one dimension. The ability of four explicit scheme (Forward Euler, Lax Friedrichs, Mac Cormack and Richtmyer) to solve SWEs was tested on three different test problems. Starting from the idea that a tsunami may begin as a sudden rise of a column of water, the first test represents a square or a sinusoidal pulse which breaks up into two identical waves moving in opposing directions on a constant depth seabed. In the other two test problems we simulate a tsunami wave approaching the shore on a variable seabed depth having either o steady or a highly variable slope. The numerical results allow us to assert that, in general, the used explicit schemes lead to a correct description of a tsunami wave propagation, both offshore and near the coastline. The exception is represented by the Forward Euler scheme that, due to its instability, was only used in the first test.
- Published
- 2019
18. Sloshing effect, design and optimisation of water ballast tank
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C. L. Dumitrache, C. Scurtu, and D. Deleanu
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Physics ,History ,Slosh dynamics ,Ballast tank ,Computer Science Applications ,Education ,Marine engineering - Published
- 2019
19. Numerical study of a container ship model for the uncoupled parametric rolling
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D. Deleanu and C. L. Dumitrache
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Container (abstract data type) ,Geology ,Parametric statistics ,Marine engineering - Abstract
Parametric roll on ships is a resonance phenomenon whose onset causes heavy roll oscillations leading to dangerous situations for the ship, the cargo and the crew. It affects both small vessels with marginal stability and large container ships if four conditions are met simultaneously: the wave length and ship length are approximately equal, the frequency of encounter wave is twice the roll natural frequency, the ship’s roll damping is low enough and the wave height exceeds a limit value characteristic to each vessel. For a container ship, the first two conditions result in a time-varying geometry of the submerged hull and thus to a periodic variation of the transverse stability. In the last two decades, several mathematical models for parametric rolling have been proposed by scientists. In the paper, we cancelled the couplings terms between heave, pitch and roll in a 3 DOF model proposed by Neves and Rodriguez to obtain an uncoupled 1 DOF model for the parametric roll. Even if it seems too simplistic, such a model based on Mathieu type equation is a good start to capture the basic features of the analysed phenomenon. There are no less than seven parameters that can influence the ship stability and the appearance of large roll amplitudes. By modifying two of these parameters one by one and keeping the others constant, a series of colour plots have been drown that capture the role played by the ship’s parameters in obtaining dangerous roll amplitudes or too short times to take countermeasures. Analysing the instability regions suggested by these colour plots, one can imagine control measures to reduce the roll amplitudes, such as changing the forward velocity or the heading angle. The data used in the paper have been obtained from experiments with a container ship model in a towing tank followed by expansion to a full scale ship.
- Published
- 2019
20. Fluid Structure Interaction (FSI) analysis on ballast tank in-line ejector
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D Deleanu and C L Dumitrache
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Ballast ,Work (thermodynamics) ,business.industry ,Ballast tank ,Mechanical engineering ,Injector ,Static analysis ,Computational fluid dynamics ,Finite element method ,law.invention ,law ,Fluid–structure interaction ,business ,Geology - Abstract
Ejectors are common devices on board liquid carrier vessels and meet on both cargo and ballast tanks. The “in-line” ejector presented in this paper is an original model that was designed with NX Siemens, using information and technical data from a worldwide supplier of high quality marine products. This paper presents a static analysis of fluid’ influence which passing through an ejector on its metal structure using Ansys. From a previous work we took into account the data obtained with CFD (computer fluid dynamic) analysis. The pressure and fluid temperature fields were imported and applied to the meshed ejector model with finite elements, obtaining data on deformations and equivalent stresses and elastic strain.
- Published
- 2019
21. E3andM2transition strengths inBi83209
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M. Smolen, A. Negret, C. Townsley, F. Browne, B. A. Brown, L. Stroe, P. H. Regan, R. Mărginean, D. Deleanu, D. M. Filipescu, D. Ghiţă, D. Bucurescu, Ioana Gheorghe, K. Mulholland, S. Toma, T. Alexander, T. Sava, R. Lica, Alison Bruce, Raymond J. Carroll, Zs. Podolyák, C. Mihai, J. F. Smith, C. R. Niţă, Thamer Alharbi, N. Florea, T. Glodariu, R. Suvaila, N. Marginean, S. Aydin, and Oliver J. Roberts
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Physics ,Crystallography ,Angular distribution ,010308 nuclear & particles physics ,0103 physical sciences ,Heavy ion ,010306 general physics ,7. Clean energy ,01 natural sciences - Abstract
The $1{i}_{\frac{13}{2}}\ensuremath{\rightarrow}1{h}_{\frac{9}{2}}\phantom{\rule{0.16em}{0ex}}(M2)$ and $3{s}_{\frac{1}{2}}\ensuremath{\rightarrow}2{f}_{\frac{7}{2}}\phantom{\rule{0.16em}{0ex}}(E3)$ reduced proton transition probabilities in $_{83}^{209}\mathrm{Bi}$ have been determined from the direct half-life measurements of the ${\frac{13}{2}}_{1}^{+}$ and ${\frac{1}{2}}_{1}^{+}$ states using the Romanian array for $\ensuremath{\gamma}$-ray SPectroscopy in HEavy ion REactions (RoSPHERE). The ${\frac{13}{2}}_{1}^{+}$ and ${\frac{1}{2}}_{1}^{+}$ states were found to have ${T}_{\frac{1}{2}}=0.120(15)$ ns and ${T}_{\frac{1}{2}}=9.02(24)$ ns respectively. Angular distribution measurements were used to determine an $E3/M2$ mixing ratio of $\ensuremath{\delta}=\ensuremath{-}0.184(13)$ for the 1609 keV $\ensuremath{\gamma}$-ray transition deexciting the ${\frac{13}{2}}_{1}^{+}$ state. This value for $\ensuremath{\delta}$ was combined with the measured half-life to give reduced transition probabilities of $B(E3,{\frac{13}{2}}_{1}^{+}\ensuremath{\rightarrow}{\frac{9}{2}}_{1}^{\ensuremath{-}})=12(2)\ifmmode\times\else\texttimes\fi{}{10}^{3}\phantom{\rule{4.pt}{0ex}}{e}^{2}\phantom{\rule{0.16em}{0ex}}{\mathrm{fm}}^{6}$ and $B(M2,{\frac{13}{2}}_{1}^{+}\ensuremath{\rightarrow}{\frac{9}{2}}_{1}^{\ensuremath{-}})=38(5){\ensuremath{\mu}}_{N}^{2}\phantom{\rule{0.16em}{0ex}}{\mathrm{fm}}^{2}$. These values are in good agreement with calculations within the finite Fermi system. The extracted value of $B(E3,{\frac{1}{2}}_{1}^{+}\ensuremath{\rightarrow}{\frac{7}{2}}_{1}^{\ensuremath{-}})=6.3(2)\ifmmode\times\else\texttimes\fi{}{10}^{3}\phantom{\rule{4.pt}{0ex}}{e}^{2}\phantom{\rule{0.16em}{0ex}}{\mathrm{fm}}^{6}$ can be explained by a small ($\ensuremath{\sim}6%$) admixture in the wave function of the ${\frac{1}{2}}_{1}^{+}$ state.
- Published
- 2016
22. MOESM1 of Scaling up strategies of the chronic respiratory disease programme of the European Innovation Partnership on Active and Healthy Ageing (Action Plan B3: Area 5)
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J. Bousquet, J. Farrell, G. Crooks, P. Hellings, E. Bel, M. Bewick, N. Chavannes, J. Sousa, A. Cruz, T. Haahtela, G. Joos, N. Khaltaev, J. Malva, A. Muraro, M. Nogues, S. Palkonen, S. Pedersen, C. Robalo-Cordeiro, B. Samolinski, T. Strandberg, A. Valiulis, A. Yorgancioglu, T. Zuberbier, A. Bedbrook, W. Aberer, M. Adachi, A. Agusti, C. Akdis, M. Akdis, J. Ankri, A. Alonso, I. Annesi-Maesano, I. Ansotegui, J. Anto, S. Arnavielhe, H. Arshad, C. Bai, I. Baiardini, C. Bachert, A. Baigenzhin, C. Barbara, E. Bateman, B. Beghé, A. Kheder, K. Bennoor, M. Benson, K. Bergmann, T. Bieber, C. Bindslev-Jensen, L. Bjermer, H. Blain, F. Blasi, A. Boner, M. Bonini, S. Bonini, S. Bosnic-Anticevitch, L. Boulet, R. Bourret, P. Bousquet, F. Braido, A. Briggs, C. Brightling, J. Brozek, R. Buhl, P. Burney, A. Bush, F. Caballero-Fonseca, D. Caimmi, M. Calderon, P. Calverley, P. Camargos, G. Canonica, T. Camuzat, K. Carlsen, W. Carr, A. Carriazo, T. Casale, A. Cepeda Sarabia, L. Chatzi, Y. Chen, R. Chiron, E. Chkhartishvili, A. Chuchalin, K. Chung, G. Ciprandi, I. Cirule, L. Cox, D. Costa, A. Custovic, R. Dahl, S. Dahlen, U. Darsow, G. Carlo, F. Blay, T. Dedeu, D. Deleanu, E. Manuel Keenoy, P. Demoly, J. Denburg, P. Devillier, A. Didier, A. Dinh-Xuan, R. Djukanovic, D. Dokic, H. Douagui, G. Dray, R. Dubakiene, S. Durham, M. Dykewicz, Y. El-Gamal, R. Emuzyte, L. Fabbri, M. Fletcher, A. Fiocchi, A. Fink Wagner, J. Fonseca, W. Fokkens, F. Forastiere, P. Frith, M. Gaga, A. Gamkrelidze, J. Garces, J. Garcia-Aymerich, B. Gemicioğlu, J. Gereda, S. González Diaz, M. Gotua, I. Grisle, L. Grouse, Z. Gutter, M. Guzmán, L. Heaney, B. Hellquist-Dahl, D. Henderson, A. Hendry, J. Heinrich, D. Heve, F. Horak, J. Hourihane, P. Howarth, M. Humbert, M. Hyland, M. Illario, J. Ivancevich, J. Jardim, E. Jares, C. Jeandel, C. Jenkins, S. Johnston, O. Jonquet, K. Julge, K. Jung, J. Just, I. Kaidashev, M. Kaitov, O. Kalayci, A. Kalyoncu, T. Keil, P. Keith, L. Klimek, B. Koffi N’Goran, V. Kolek, G. Koppelman, M. Kowalski, I. Kull, P. Kuna, V. Kvedariene, B. Lambrecht, S. Lau, D. Larenas-Linnemann, D. Laune, L. Le, P. Lieberman, B. Lipworth, J. Li, K. Lodrup Carlsen, R. Louis, W. MacNee, Y. Magard, A. Magnan, B. Mahboub, A. Mair, I. Majer, M. Makela, P. Manning, S. Mara, G. Marshall, M. Masjedi, P. Matignon, M. Maurer, S. Mavale-Manuel, E. Melén, E. Melo-Gomes, E. Meltzer, A. Menzies-Gow, H. Merk, J. Michel, N. Miculinic, F. Mihaltan, B. Milenkovic, G. Mohammad, M. Molimard, I. Momas, A. Montilla-Santana, M. Morais-Almeida, M. Morgan, R. Mösges, J. Mullol, S. Nafti, L. Namazova-Baranova, R. Naclerio, A. Neou, H. Neffen, K. Nekam, B. Niggemann, G. Ninot, T. Nyembue, R. O’Hehir, K. Ohta, Y. Okamoto, K. Okubo, S. Ouedraogo, P. Paggiaro, I. Pali-Schöll, P. Panzner, N. Papadopoulos, A. Papi, H. Park, G. Passalacqua, I. Pavord, R. Pawankar, R. Pengelly, O. Pfaar, R. Picard, B. Pigearias, I. Pin, D. Plavec, D. Poethig, W. Pohl, T. Popov, F. Portejoie, P. Potter, D. Postma, D. Price, K. Rabe, F. Raciborski, F. Radier Pontal, S. Repka-Ramirez, S. Reitamo, S. Rennard, F. Rodenas, J. Roberts, J. Roca, L. Rodriguez Mañas, C. Rolland, M. Roman Rodriguez, A. Romano, J. Rosado-Pinto, N. Rosario, L. Rosenwasser, M. Rottem, D. Ryan, M. Sanchez-Borges, G. Scadding, H. Schunemann, E. Serrano, P. Schmid-Grendelmeier, H. Schulz, A. Sheikh, M. Shields, N. Siafakas, Y. Sibille, T. Similowski, F. Simons, J. Sisul, I. Skrindo, H. Smit, D. Solé, T. Sooronbaev, O. Spranger, R. Stelmach, P. Sterk, J. Sunyer, C. Thijs, T. To, A. Todo-Bom, M. Triggiani, R. Valenta, A. Valero, E. Valia, E. Valovirta, E. Ganse, M. Hage, O. Vandenplas, T. Vasankari, B. Vellas, J. Vestbo, G. Vezzani, P. Vichyanond, G. Viegi, C. Vogelmeier, T. Vontetsianos, M. Wagenmann, B. Wallaert, S. Walker, D. Wang, U. Wahn, M. Wickman, D. Williams, S. Williams, J. Wright, B. Yawn, P. Yiallouros, O. Yusuf, A. Zaidi, H. Zar, M. Zernotti, L. Zhang, N. Zhong, M. Zidarn, and J. Mercier
- Abstract
Additional file 1. IPCRG scaling up activities.
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- 2016
- Full Text
- View/download PDF
23. SIMULTANEOUS RESONANCE CASES IN A PITCH – ROLL SHIP MODEL. PART 1: FIRST – ORDER APPROXIMATE SOLUTIONS
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D Deleanu
- Published
- 2016
- Full Text
- View/download PDF
24. SIMULTANEOUS RESONANCE CASES IN A PITCH – ROLL SHIP MODEL. PART 2: NUMERICAL ANALYSIS
- Author
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D Deleanu
- Published
- 2016
- Full Text
- View/download PDF
25. Poster session 2
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J. M. Perez-Pomares, A. Ruiz-Villalba, A. Ziogas, J. C. Segovia, M. Ehrbar, R. Munoz-Chapuli, A. De La Rosa, J. N. Dominguez, L. Hove-Madsen, B. Sankova, D. Sedmera, D. Franco, A. Aranega Jimenez, G. Babaeva, N. Chizh, S. Galchenko, B. Sandomirsky, M. Schwarzl, S. Seiler, P. Steendijk, S. Huber, H. Maechler, M. Truschnig-Wilders, B. Pieske, H. Post, S. Simrick, R. Kreutzer, C. Rao, C. M. Terracciano, P. Kirchhof, L. Fabritz, T. Brand, M. Theveniau-Ruissy, P. Parisot, A. Francou, E. Saint-Michel, K. Mesbah, R. G. Kelly, H.-T. Wu, S.-S. Sie, C.-Y. Chen, T.-C. Kuan, C. S. Lin, Z. Ismailoglu, M. Guven, A. Yakici, Y. Ata, S. Ozcan, E. Yildirim, Z. Ongen, V. Miroshnikova, E. Demina, T. Rodygina, P. Kurjanov, A. Denisenko, A. Schwarzman, A. Rubanenko, Y. Shchukin, A. Germanov, M. Goldbergova, J. Parenica, J. Lipkova, N. Pavek, P. Kala, M. Poloczek, A. Vasku, I. Parenicova, J. Spinar, C. Gambacciani, E. Chiavacci, M. Evangelista, N. Vesentini, C. Kusmic, L. Pitto, A. Chernova, S. U. Y. Nikulina, D. A. Arvanitis, I. Mourouzis, C. Pantos, E. G. Kranias, D. V. Cokkinos, D. Sanoudou, T. E. Vladimirskaya, I. A. Shved, S. G. Kryvorot, I. M. Schirmer, A. Appukuttan, L. Pott, K. Jaquet, Y. Ladilov, C. R. Archer, M. D. Bootman, H. L. Roderick, A. Fusco, D. Sorriento, G. Santulli, B. Trimarco, G. Iaccarino, M. Hagenmueller, J. Riffel, E. Bernhold, H. A. Katus, S. E. Hardt, A. Maqsood, M. Zi, S. Prehar, L. Neyses, S. Ray, D. Oceandy, N. Khatami, P. Wadowski, V. Wagh, J. Hescheler, A. Sachinidis, W. Mohl, B. Chaudhry, D. Burns, D. J. Henderson, N. A. M. Bax, M. H. Van Marion, B. Shah, M. J. Goumans, C. V. C. Bouten, D. W. J. Van Der Schaft, A. A. M. Van Oorschot, S. Maas, J. Braun, J. Van Tuyn, A. A. F. De Vries, A. C. Gittenberger-De Groot, S. Bageghni, M. J. Drinkhill, T. F. C. Batten, J. F. X. Ainscough, B. Onate, G. Vilahur, R. Ferrer-Lorente, J. Ybarra, A. Diez-Caballero, C. Ballesta-Lopez, F. Moscatiello, J. Herrero, L. Badimon, E. Martin-Rendon, D. M. Clifford, S. A. Fisher, S. J. Brusnkill, C. Doree, A. Mathur, M. Clarke, S. M. Watt, R. Hernandez-Vera, D. Kavanagh, A. I. Yemm, J. Frampton, N. Kalia, Y. Terajima, T. Shimizu, S. Tsuruyama, H. Ishii, H. Sekine, N. Hagiwara, T. Okano, K. R. Vrijsen, S. A. J. Chamuleau, J. P. G. Sluijter, P. F. M. Doevendans, R. Madonna, S. Delli Pizzi, L. Di Donato, A. Mariotti, L. Di Carlo, E. D'ugo, M. A. Teberino, A. Merla, A. T, R. De Caterina, L. Kolker, N. N. Ali, K. Maclellan, M. Moore, J. Wheeler, S. E. Harding, R. A. Fleck, J. M. Rowlinson, N. Kraenkel, R. Ascione, P. Madeddu, J. F. O'sullivan, A. L. Leblond, G. Kelly, A. H. S. Kumar, P. Metharom, C. K. Buneker, N. Alizadeh-Vikali, B. G. Hynes, R. O'connor, N. M. Caplice, M. Noseda, A. J. De Smith, T. Leja, P. H. Rao, F. Al-Beidh, M. S. Abreu Pavia, A. I. Blakemore, M. D. Schneider, K. Stathopoulou, F. Cuello, E. Ehler, R. S. Haworth, M. Avkiran, H. Morawietz, C. Eickholt, H. Langbein, M. Brux, C. Goettsch, W. Goettsch, A. Arsov, C. Brunssen, L. Mazilu, I. R. Parepa, A. I. Suceveanu, A. P. Suceveanu, F. S. De Man, C. Guignabert, L. Tu, M. L. Handoko, I. Schalij, E. Fadel, P. E. Postmus, A. Vonk-Noordegraaf, M. Humbert, S. Eddahibi, C. Del Giudice, A. Anastasio, L. Fazal, F. Azibani, N. Bihry, R. Merval, E. Polidano, J.-L. Samuel, C. Delcayre, Y. Zhang, Y. M. Mi, L. L. Ren, Y. P. Cheng, R. Guo, Y. Liu, Y. N. Jiang, A. D. Kokkinos, P. Tretjakovs, A. Jurka, I. Bormane, I. Mikelsone, D. Reihmane, K. Elksne, G. Krievina, J. Verbovenko, G. Bahs, N. Lopez-Andres, A. Rousseau, L. Calvier, R. Akhtar, C. Labat, K. Cruickshank, J. Diez, F. Zannad, P. Lacolley, P. Rossignol, K. Hamesch, P. Subramanian, X. Li, A. Thiemann, K. Heyll, K. Dembowsky, E. Chevalier, C. Weber, A. Schober, L. Yang, G. Kim, B. Gardner, J. Earley, M. Hofmann-Bowman, C.-F. Cheng, W.-S. Lian, H. Lin, N. J. Jinjolia, G. A. Abuladze, S. H. T. Tvalchrelidze, I. Khamnagadaev, M. Shkolnikova, L. Kokov, I. Miklashevich, I. Drozdov, I. Ilyich, B. O. Bingen, S. F. A. Askar, D. L. Ypey, A. Van Der Laarse, M. J. Schalij, D. A. Pijnappels, C. H. Roney, F. S. Ng, R. A. Chowdhury, E. T. Y. Chang, P. M. Patel, A. R. Lyon, J. H. Siggers, N. S. Peters, A. Obergrussberger, S. Stoelzle, A. Bruggemann, C. Haarmann, M. George, N. Fertig, D. Moreira, A. Souza, P. Valente, J. Kornej, C. Reihardt, J. Kosiuk, A. Arya, G. Hindricks, V. Adams, D. Husser, A. Bollmann, P. Camelliti, J. Dudhia, P. Dias, J. Cartledge, D. J. Connolly, M. Nobles, S. Sebastian, A. Tinker, A. Opel, H. Daimi, A. Haj Khelil, J. Be Chibani, A. Barana, I. Amoros, M. Gonzalez De La Fuente, R. Caballero, A. Aranega, A. Kelly, O. Bernus, O. J. Kemi, R. C. Myles, I. A. Ghouri, F. L. Burton, G. L. Smith, M. Del Lungo, L. Sartiani, V. Spinelli, M. Baruscotti, D. Difrancesco, A. Mugelli, E. Cerbai, A. M. Thomas, Q. Aziz, T. Khambra, J. M. A. Addlestone, E. J. Cartwright, R. Wilkinson, W. Song, S. Marston, A. Jacquet, N. M. Mougenot, A. J. Lipskaia, E. R. Paalberends, K. Stam, S. J. Van Dijk, M. Van Slegtenhorst, C. Dos Remedios, F. J. Ten Cate, M. Michels, H. W. M. Niessen, G. J. M. Stienen, J. Van Der Velden, M. I. Read, A. A. Andreianova, J. C. Harrison, C. S. Goulton, D. S. Kerr, I. A. Sammut, M. Wallner, D. Von Lewinski, D. Kindsvater, M. Saes, I. Morano, A. Muegge, B. Buyandelger, S. Kostin, S. Gunkel, J. Vouffo, K. Ng, J. Chen, M. Eilers, R. Isaacson, H. Milting, R. Knoell, M.-E. Cattin, C. Crocini, S. Schlossarek, S. Maron, A. Hansen, T. Eschenhagen, L. Carrier, G. Bonne, R. Coppini, C. Ferrantini, I. Olivotto, L. Belardinelli, C. Poggesi, M. C. Leung, A. E. Messer, O. Copeland, S. B. Marston, A. M. Mills, T. Collins, P. O'gara, T. Thum, K. Regalla, K. T. Macleod, T. Prodromakis, U. Chaudhry, A. Darzi, M. H. Yacoub, T. Athanasiou, A. Bogdanova, A. Makhro, M. Hoydal, T. O. Stolen, A. B. Johnssen, M. Alves, D. Catalucci, G. Condorelli, L. G. Koch, S. L. Britton, U. Wisloff, V. Bito, P. Claus, K. Vermeulen, C. Huysmans, R. Ventura-Clapier, K. R. Sipido, M. N. Seliuk, A. P. Burlaka, E. P. Sidorik, N. V. Khaitovych, M. M. Kozachok, V. S. Potaskalova, R. B. Driesen, D. T. Galan, D. De Paulis, T. Arnoux, S. Schaller, R. M. Pruss, D. M. Poitz, A. Augstein, R. C. Braun-Dullaeus, A. Schmeisser, R. H. Strasser, P. Micova, P. Balkova, M. Hlavackova, J. Zurmanova, D. Kasparova, F. Kolar, J. Neckar, F. Novak, O. Novakova, S. Pollard, M. Babba, A. Hussain, R. James, H. Maddock, A. S. Alshehri, G. F. Baxter, B. Dietel, R. Altendorf, W. G. Daniel, R. Kollmar, C. D. Garlichs, R. Sirohi, N. Roberts, D. Lawrence, A. Sheikh, S. Kolvekar, J. Yap, M. Arend, G. Walkinshaw, D. J. Hausenloy, D. M. Yellon, A. Posa, R. Szabo, Z. Szalai, P. Szablics, M. A. Berko, K. Orban, Z. S. Murlasits, L. Balogh, C. Varga, H. C. Ku, M. J. Su, R.-M. Chreih, C. Ginghina, D. Deleanu, A. L. B. J. Ferreira, A. Belal, M. A. Ali, X. Fan, A. Holt, R. Campbell, R. Schulz, C. Bonanad, V. Bodi, J. Sanchis, J. M. Morales, V. Marrachelli, J. Nunez, M. J. Forteza, F. Chaustre, C. Gomez, F. J. Chorro, T. Csont, V. Fekete, Z. Murlasits, E. Aypar, P. Bencsik, M. Sarkozy, Z. V. Varga, P. Ferdinandy, G. D. Duerr, M. Zoerlein, D. Dewald, B. Mesenholl, P. Schneider, A. Ghanem, S. Rittling, A. Welz, O. Dewald, E. Becker, C. Peigney, C. Bouleti, A. Galaup, C. Monnot, B. Ghaleh, S. Germain, A. Timmermans, A. Ginion, C. De Meester, K. Sakamoto, J.-L. Vanoverschelde, S. Horman, C. Beauloye, L. Bertrand, N. Maroz-Vadalazhskaya, E. Drozd, L. Kukharenko, I. Russkich, D. Krachak, Y. Seljun, Y. Ostrovski, A.-C. Martin, B. Le Bonniec, T. Lecompte, B. Dizier, J. Emmerich, A.-M. Fischer, C.-M. Samama, A. Godier, S. Mogensen, E. M. Furchtbauer, C. Aalkjaer, W. L. Choong, A. Jovanovic, F. Khan, J. M. Daniel, J. M. Dutzmann, R. Widmer-Teske, D. Guenduez, D. Sedding, M. M. Castro, J. J. C. Cena, W. J. C. Cho, G. G. Goobie, M. P. W. Walsh, R. S. Schulz, J. Dutzmann, K. T. Preissner, W. Sones, M. Kotlikoff, K. Serizawa, K. Yogo, K. Aizawa, M. Hirata, Y. Tashiro, N. Ishizuka, A. Varela, M. Katsiboulas, D. Tousoulis, T. G. Papaioannou, S. Vaina, C. H. Davos, C. Piperi, C. Stefanadis, E. K. Basdra, A. G. Papavassiliou, C. Hermenegildo, M. Lazaro-Franco, A. Sobrino, C. Bueno-Beti, N. Martinez-Gil, T. Walther, C. Peiro, C. F. Sanchez-Ferrer, S. Novella, M. Ciccarelli, A. Franco, G. W. Dorn, P. Cseplo, O. Torok, Z. S. Springo, Z. Vamos, D. Kosa, J. Hamar, A. Koller, K. J. Bubb, A. Ahluwalia, E. L. Stepien, A. Gruca, J. Grzybowska, J. Goralska, A. Dembinska-Kiec, J. Stolinski, L. Partyka, H. Zhang, D. Sweeney, G. N. Thomas, P. V. Fish, D. P. Taggart, S. Cioffi, M. Bilio, S. Martucciello, E. Illingworth, A. Caporali, S. Shantikumar, M. Marchetti, F. Martelli, C. Emanueli, M. Meloni, A. Al Haj Zen, G. Sala-Newby, S. Del Turco, C. Saponaro, B. Dario, S. Sartini, A. Menciassi, P. Dario, C. La Motta, G. Basta, V. Santiemma, C. Bertone, F. Rossi, E. Michelon, M. J. Bianco, A. Castelli, D. I. Shin, K. B. Seung, S. M. Seo, H. J. Park, P. J. Kim, S. H. Baek, Y. S. Choi, S. H. Her, D. B. Kim, J. M. Lee, C. S. Park, S. Rocchiccioli, A. Cecchettini, G. Pelosi, L. Citti, O. Parodi, M. G. Trivella, D. Michel-Monigadon, F. Burger, S. Dunoyer-Geindre, G. Pelli, B. Cravatt, S. Steffens, A. Didangelos, U. Mayr, X. Yin, C. Stegemann, J. Shalhoub, A. H. Davies, C. Monaco, M. Mayr, S. Lypovetska, S. Grytsenko, I. U. Njerve, A. A. Pettersen, T. B. Opstad, V. Bratseth, H. Arnesen, I. Seljeflot, I. E. Dumitriu, P. Baruah, R. F. Antunes, J. C. Kaski, I. Trapero, I. Benet, C. Alguero, F. J. Chaustre, A. Mangold, S. Puthenkalam, K. Distelmaier, C. Adlbrecht, I. M. Lang, T. Koizumi, I. Inoue, N. Komiyama, S. Nishimura, O. N. Korneeva, O. M. Drapkina, L. Fornai, A. Angelini, A. Kiss, F. Giskes, G. Eijkel, M. Fedrigo, M. L. Valente, G. Thiene, R. M. A. Heeren, T. Padro, L. Casani, R. Suades, B. Bertoni, R. Carminati, V. Carlini, L. Pettinari, C. Martinelli, N. Gagliano, G. Noppe, P. Buchlin, N. Marquet, N. Baeyens, N. Morel, A. Baysa, J. Sagave, C. P. Dahl, L. Gullestad, A. Carpi, F. Di Lisa, M. Giorgio, J. Vaage, G. Valen, E. Vafiadaki, V. Papalouka, G. Terzis, K. Spengos, P. Manta, C. Gales, G. Genet, E. Dague, O. Cazorla, B. Payre, C. Mias, A. Ouille, A. Lacampagne, A. Pathak, J. M. Senard, M. Abonnenc, P. Da Costa Martins, S. Srivastava, M. Gautel, L. De Windt, L. Comelli, C. Lande, N. Ucciferri, L. Ikonen, H. Vuorenpaa, K. Kujala, J.-R. Sarkanen, T. Heinonen, T. Ylikomi, K. Aalto-Setala, H. Capros, N. Sprincean, N. Usurelu, V. Egorov, N. Stratu, V. Matchkov, E. Bouzinova, N. Moeller-Nielsen, O. Wiborg, P. S. Gutierrez, R. Aparecida-Silva, L. F. Borges, L. F. P. Moreira, R. R. Dias, J. Kalil, N. A. G. Stolf, W. Zhou, K. Suntharalingam, N. Brand, R. Vilar Compte, L. Ying, K. Bicknell, A. Dannoura, P. Dash, G. Brooks, I. Tsimafeyeu, Y. Tishova, N. Wynn, I. P. Oyeyipo, L. A. Olatunji, L. Maegdefessel, J. Azuma, R. Toh, U. Raaz, D. R. Merk, A. Deng, J. M. Spin, P. S. Tsao, L. Tedeschi, M. Taranta, I. Naldi, S. Grimaldi, C. Cinti, M. Bousquenaud, F. Maskali, S. Poussier, P. Y. Marie, H. Boutley, G. Karcher, D. R. Wagner, Y. Devaux, I. Torre, S. Psilodimitrakopoulos, I. Iruretagoiena, A. Gonzalez-Tendero, D. Artigas, P. Loza-Alvarez, E. Gratacos, I. Amat-Roldan, L. Murray, D. M. Carberry, P. Dunton, M. J. Miles, M.-S. Suleiman, K. Kanesalingam, R. Taylor, C. N. Mc Collum, A. Parniczky, M. Solymar, A. Porpaczy, A. Miseta, Z. S. Lenkey, S. Szabados, A. Cziraki, J. Garai, I. Myloslavska, S. M. Menazza, M. C. Canton, F. D. L. Di Lisa, S. H. V. Oliveira, C. A. S. Morais, M. R. Miranda, T. T. Oliveira, M. R. A. Lamego, L. M. Lima, N. S. Goncharova, A. V. Naymushin, A. V. Kazimli, O. M. Moiseeva, M. G. Carvalho, A. P. Sabino, A. P. L. Mota, M. O. Sousa, A. Niessner, B. Richter, P. J. Hohensinner, K. Rychli, G. Zorn, R. Berger, D. Moertl, R. Pacher, J. Wojta, M. Huelsmann, G. Kukharchik, N. Nesterova, A. Pavlova, L. Gaykovaya, N. Krapivka, I. Konstantinova, L. Sichinava, S. Prapa, K. P. Mccarthy, P. J. Kilner, X. Y. Xu, M. R. Johnson, S. Y. Ho, M. A. Gatzoulis, E. G. Stoupel, R. Garcia, D. Merino, C. Montalvo, M. A. Hurle, J. F. Nistal, A. V. Villar, A. Perez-Moreno, R. Gilabert, and E. Ros
- Subjects
medicine.medical_specialty ,Endocrinology ,Physiology ,Activator (genetics) ,Chemistry ,Physiology (medical) ,Internal medicine ,medicine ,AMPK ,Myocyte ,Long-term potentiation ,Metabolism ,Cardiology and Cardiovascular Medicine - Published
- 2012
26. Method Developing and Testing for Inelastic Scattering Measurements at the GELINA Facility
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A. J. M. Plompen, C. Rouki, N. Nankov, P. Dessagne, M. Stanoiu, G. Rudolf, M. Mosconi, C. Borcea, Alexandru Negret, Ralf Nolte, J. C. Thiry, D. Deleanu, and M. Kerveno
- Subjects
Physics ,Fission ,Detector ,General Physics and Astronomy ,Nuclear data ,chemistry.chemical_element ,Germanium ,Actinide ,Inelastic scattering ,Inelastic neutron scattering ,Neutron temperature ,Nuclear physics ,chemistry ,Nuclear Experiment - Abstract
Accurate inelastic scattering measurements are of interest to improving modelling and simulation of advanced reactor systems through better nuclear data (OECD-NEA, High priority request list for nuclear data http://www.nea.fr/html/dbdata/hprl/). Two setups are available at IRMM for measurements of inelastic scattering with the (n, n′γ)-technique. The first the GAINS gammaarray for inelastic neutron scattering at a 200 m station consists of eight high purity germanium detectors, has high incident neutron energy resolution and is therefore tailored for inelastic scattering measurements. The second, at a 30 m station was developed by IPHC with the purpose of studying actinides for the Th/U cycle and emphasizing besides (n, n′γ) also (n, 2nγ) reactions. In the recent past a number of efforts were started to investigate the uncertainties and corrections required to obtain reliable results and to investigate the limits of accuracy of this technique. A joint effort is described that has led to an improved understanding of the fission chambers used. In particular, the important corrections to the efficiency for fission fragment loss were investigated.
- Published
- 2011
27. Sub-nanosecond Half-life Measurement of the Yrast Iπ=5− State in the N=78 Nucleus Ce58136 using Fast-timing Coincident Gamma-ray Spectroscopy
- Author
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D. Bucurescu, K. Mulholland, R. Mărginean, T. Glodariu, D. Ghita, Zs. Podolyák, T. Sava, L. Stroe, Oliver J. Roberts, A. Negret, R. Britton, T. Alharbi, N. V. Zamfir, C. R. Nita, D. Deleanu, D. M. Filipescu, C. Mihai, Zena Patel, P. H. Regan, N. Marginean, C. Townsley, and A.D. Bajoga
- Subjects
Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Yrast ,Quadrupole ,Half-life ,Gamma spectroscopy ,Atomic physics ,Nanosecond ,Scintillator ,Nuclear Experiment ,Spectroscopy ,Radioactive decay - Abstract
We report on the measurement of the half-life of the yrast I π = 5 − state in the transitional nucleus 136 Ce using a combined HPGe-LaBr3(Ce) scintillator gamma-ray detection array. The measured value for the E 1 decay is approximately half a nanosecond, which corresponds to an E 1 decay strength of approximately 2 × 10 − 6 Wu. This value is in line with single-particle type E 1 decays in this mass region and suggests no sign of additional K-hindrance associated with axially symmetric quadrupole deformations observed for lighter cerium isotopes.
- Published
- 2014
28. The gamma efficiency of the GAINS spectrometer
- Author
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Ph. Dessagne, C. Borcea, A. J. M. Plompen, M. Kerveno, D. Deleanu, Alexandru Negret, and J. C. Thiry
- Subjects
Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Spectrometer ,Monte Carlo method ,Neutron source ,Neutron ,Neutron scattering ,Inelastic scattering ,Instrumentation ,Neutron time-of-flight scattering ,Semiconductor detector - Abstract
The GAINS (Germanium Array for Inelastic Neutron Scattering) setup was recently installed at the GELINA (Geel Linear Accelerator) neutron source of EC-JRC-IRMM. In order to produce reliable neutron inelastic cross-section data the setup requires a precise efficiency calibration for each sample under investigation. These samples represent extended sources in non-standard orientations and with significant self-attenuation of gamma rays. We present in detail the efficiency calibration procedure performed with two Monte Carlo simulations using MCNP and GEANT4. A good agreement is found between the two independent approaches. The general features of the simulations are discussed together with an in-depth description of the various factors influencing the efficiency.
- Published
- 2010
29. Abstracts
- Author
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O. Barthelemy, J. Silvain, D. Brieger, A. Bellemain-Appaix, G. Cayla, F. Beygui, R. Lancar, J. P. Collet, A. Mercadier, G. Montalescot, K. S. Cha, Y. H. Nam, J. H. Kim, S. Y. Park, T. H. Park, M. H. Kim, Y. D. Kim, H. C. Lee, M. S. Ahn, T. J. Hong, R. Blanco, F. Blanco, J. Szarfer, A. Garcia Escudero, G. Gigena, J. Gagliardi, A. Rodriguez, R. Sarmiento, S. Affatatto, M. Riccitelli, A. Petris, M. D. Datcu, C. Pop, M. Radoi, C. Arsenescu-Georgescu, I. Petrescu, L. Petrescu, L. Serban, E. Nechita, G. Tatu-Chitoiu, M. Dorobantu, I. Benedek, E. Craiu, C. Sinescu, D. D. Ionescu, C. Ginghina, B. Minescu, A. Izzo, P. Mantovani, L. Tomasi, L. Dall'oglio, S. Bonatti, R. Rosiello, M. Romano, F. Agostini, R. Zanini, Z. Y. Zhao, Y. J. Wu, J. J. Li, Y. J. Yany, H. Y. Qian, Y. D. Tang, A. T. Timoteo, A. Toste, A. Lousinha, R. Ramos, J. A. Oliveira, M. L. Ferreira, R. C. Ferreira, C. Cabades, J. L. Diez Gil, P. Aguar, D. Sanmiguel, A. Lopez-March, R. Marmol, L. Guerra, V. Girbes, J. Ferrando, A. Rincon De Arellano, L. Patricio, M. Blondal, T. Ainla, T. Marandi, J. Eha, M. M. Oliveira, M. N. Silva, P. S. Cunha, J. Feliciano, S. Silva, J. Kanovsky, P. Kala, J. Parenica, M. Poloczek, K. Prymusova, L. Kubkova, J. Spinar, D. Olinic, C. Homorodean, M. Ober, M. Olinic, C. Andrioaia, A. Condac, M. Masmoudi, B. Berdaoui, S. Labidi, C. Tapia Ballesteros, C. Hernandez Luis, M. G. Sandin, J. M. Vegas, R. Andion, N. Martinez, I. A. Gonzalez, M. Alvarado, I. J. Amat, J. A. San Roman, M. J. Garcia Gonzalez, E. Arroyo Ucar, C. Hernandez Garcia, M. Dorta Martin, F. Marrero Rodriguez, R. Dragu, M. Kapeliovich, H. Hammerman, D. Silva, N. Cortez-Dias, C. Jorge, J. Silva Marques, P. Carilho Ferreira, S. Robalo Martins, M. Almeida Ribeiro, C. Calisto, M. Fiuza, M. G. Lopes, P. Milicevic, M. Panic, I. Stankovic, D. Milicevic, T. Kalezic, S. Kafedzic, I. Ilic, M. Cerovic, B. Putnikovic, A. Neskovic, D. Rott, D. Leibowitz, Z. Monhart, J. Reissigova, H. Grunfeldova, P. Jansky, B. Valente, I. Villanueva Benito, I. Solla, E. Paredes, O. Diaz Castro, F. Calvo, J. A. Baz, A. Iniguez, A. Aleksova, R. Gerloni, R. Belfiore, C. Carriere, G. Barbati, E. Fabris, F. Possa, D. Nait, M. Milo, G. Sinagra, N. Marques, J. Mimoso, V. Gomes, R. M. Agra Bermejo, E. A. A. Emad Abu Assi, S. R. R. Sergio Raposeiras Roubin, P. C. G. Pilar Cabanas Grandio, C. P. G. Carlos Pena Gil, J. M. G. A. Jose Maria Garcia Acuna, J. R. G. J. Jose Ramon Gonzalez Juanatey, M. J. Daly, P. Scott, C. G. Owens, A. Tomlin, B. Smith, A. A. J. Adgey, L. R. Alvarez-Contreras, U. Juarez, A. Altamirano, A. Arias, A. Alvarez-San Gabriel, H. Gonzalez-Pacheco, C. Martinez-Sanchez, M. Rahnavardi, M. Keshtkar-Jahromi, H. Vakili, S. Gholamin, S. M. Razavi, T. Gilis-Januszewski, K.- P. Mellwig, M. Wiemer, J. Gilis-Januszewski, A. Peterschroeder, J. Koerfer, D. Horstkotte, M. Vrsalovic, B. Getaldic, N. Vrkic, H. Pintaric, S. Khan, B. Wasan, L. Moretti, P. Grossi, S. Silenzi, M. Testa, L. Candelori, L. N. Clementi, M. Forlini, L. Lando, M. L. Pezzuoli, P. Corradetti, G. Leurent, P. Y. Pennec, E. Filippi, B. Moquet, J. P. Hacot, P. Druelles, A. Rialan, G. Rouault, I. Coudert, H. Le Breton, S. Gevaert, F. Tromp, E. Vandecasteele, F. De Somer, Y. Van Belleghem, S. Bouchez, F. Martens, I. Herck, M. De Pauw, O. Ludka, M. Sepsi, R. Miklik, L. Dusek, D. Tomcikova, J. M. Garcia-Acuna, P. Aguiar-Souto, S. Raposeiras Roubin, R. Agra-Bermejo, M. Jacquet, E. Abu-Assi, J. R. Gonzalez-Juanatey, A. Ibatov, R. Labrova, R. Karlik, P. Lokaj, Q. She, S. B. Deng, S. H. Huang, L. J. Gu, J. I. A. N. Rong, Z. K. Wu, Y. Li, J. Zhang, L. Parascan, A. Campanile, L. Spinelli, G. Santulli, M. Ciccarelli, S. De Gennaro, E. Assante Di Panzillo, B. Trimarco, G. Iaccarino, E. Bobescu, G. Datcu, D. Dobreanu, B. Doka, J.- C. Charniot, C. Cosson, J. P. Albertini, R. Bittar, P. Giral, C. Cherfils, E. Guillerm, D. Bonnefont-Rousselot, A. Rusali, L. Cojocaru, I. Parepa, T. Koizumi, S. Iida, J. Sato, T. Kikutani, T. Muramatsu, S. Nishimura, N. Komiyama, W. P. Lee, B. B. Ong, K. Haralambos, D. Townsend, J. A. E. Rees, E. J. Williams, J. P. Halcox, I. Mcdowell, M. Damjanovic, G. Koracevic, D. Djordjevic-Radojkovic, M. Pavlovic, N. Krstic, S. Ciric-Zdravkovic, A. Stojkovic, Z. Perisic, S. Apostolovic, A. Faustino, L. Seca, S. Barra, F. Caetano, R. Providencia, J. Silva, P. Gomes, G. Costa, M. Costa, A. Leitao-Marques, A. L. Volkova, G. P. Arutyunov, N. A. Bylova, I. I. Dayter, Y. T. F. N. Jao, C. C. Fang, Y. Chen, C. L. Yu, S. P. Wang, J. Valencia, P. Perez-Berbel, J. M. Ruiz-Nodar, J. Pineda, P. Bordes, M. Quintanilla, V. Mainar, F. Sogorb, N. Santos, M. Serrao, H. Cafe, B. Silva, R. Oliveira, G. Caires, A. Drumond, J. Araujo, R. A. Providencia, P. L. Gomes, J. R. Pais, P. Mota, A. M. Leitao-Marques, S. Farhan, R. Jarai, I. Tentzeris, B. Vogel, M. K. Freynhofer, J. Wojta, K. Huber, M. Poli, P. Trambaiolo, F. Corsi, M. De Luca, M. Mustilli, V. Lukic, M. Simonetti, G. Ferraiuolo, M. Lettino, G. Casella, M. R. Conte, L. De Luca, G. Geraci, R. Ceravolo, A. Pani, G. Fradella, A. Schratter, H. Thiele, T. Klemm, K. Demmin, D. Lehmann, M. Mende, G. Schuler, U. Pittl, A. Chernova, S. U. Nikulina, T. Naruke, T. Inomata, T. Yanagisawa, E. Maekawa, T. Mizutani, H. Shinagawa, M. Nishii, I. Takeuchi, H. Takehana, T. Izumi, C. Paulo, J. Mascarenhas, M. Patacho, J. Pimenta, P. Bettencourt, S. Nardai, G. Y. Szabo, B. Berta, I. Edes, B. Merkely, J. Delgado Silva, R. Baptista, R. Faria, J. Trigo, P. Gago, G. Gheorghe, I. T. Nanea, A. Cristea, S. Almarichi, H. Martins, F. Saraiva, E. Jorge, P. L. Mendes, P. Monteiro, S. Costa, F. Franco, L. A. Providencia, T. Nanea, G. S. Gheorghe, S. Visan, N. Paun, R. Gaber, R. Delewi, R. Nijveldt, H. A. De Bruin, A. Hirsch, A. Van Der Laan, B. J. Bouma, J. P. G. Tijssen, A. C. Van Rossum, F. Zijlstra, J. J. Piek, H. Rus, M. Donea, C. Ciurea, G. Ifteni, G. Casolo, M. Chioccioli, M. Magnacca, J. Del Meglio, A. Comella, M. Baratto, J. Lera, L. Salvadori, C. Tessa, C. Vignali, Z. Keca, T. Momcilov Popin, G. Panic, R. White, F. Mateen, A. Weaver, Y. Agmon, E. Okisheva, D. Tsaregorodtsev, V. Sulimov, I. J. Amat Santos, C. Hernandez, C. Tapia, A. Campo, D. Fredman, L. Svensson, M. Rosenqvist, S. Tadel-Kocjancic, P. Radsel, R. Knafelj, V. Gorjup, M. Noc, E. Zima, Z. S. Jenei, E. Kovacs, I. Osztheimer, L. Molnar, A. Horvath, D. Becker, L. Geller, R. Maggi, T. Furukawa, V. Viscardi, M. Brignole, S. R. N. Leal, H. Dores, I. Rosario, J. Monge, M. J. Carvalho, I. Arroja, A. Leitao, C. Fonseca, A. Aleixo, A. Silva, S. Keuleers, P. Herijgers, M. C. Herregods, W. Budts, C. Dubois, B. Meuris, P. Verhamme, W. Flameng, F. Van De Werf, T. Adriaenssens, H. Badran, M. Elnoamany, T. Lolah, C. Olariu, C. Macarie, M. A. H. Mollik, A. I. Hassan, T. K. Paul, M. Z. Haque, R. Jahan, M. Rahmatullah, M. A. Khatun, M. T. Rahman, M. H. Chowdhury, J. Bustamante Munguira, E. Tamayo, I. Garcia-Cuenca, E. Bustamante, J. Gualis, M. L. Gomez-Martinez, S. Florez, J. I. Gomez-Herreras, R. Ramirez Rodriguez, A. M. Ramirez Rodriguez, M. A. Garcia-Bello, E. Hernadez Ortega, E. Caballero Dorta, A. Garcia Quintana, V. Piro Mastraccio, A. Medina Fernandez Aceytuno, E. Assanelli, M. De Metrio, M. Rubino, G. Lauri, A. Cabiati, J. Campodonico, M. Grazi, M. Moltrasio, I. Marana, G. Marenzi, M. Lovlien, B. Schei, R. Picon-Heras, C. Acebal, J. C. Garcia Rubira, D. Vivas Balcones, I. Nunez-Gil, B. Ruiz-Mateos, B. Ibanez, A. Fernandez-Ortiz, V. D. Vintila, O. A. Enescu, C. I. Stoicescu, C. Udroiu, M. Cinteza, G. Tatu - Chitoiu, D. Vinereanu, C. Fresco, M. De Biasio, D. Muser, R. Sappa, G. Morocutti, G. Bernardi, A. Proclemer, B. Fontanella, A. Affatato, C. Ciccarese, M. Sacchini, M. Volpini, F. Bianchetti, G. Verzura, L. Dei Cas, R. Pudil, V. Blaha, J. Vojacek, I. Paraskevaidis, I. Ikonomidis, J. Parissis, C. Papadopoulos, V. Stasinos, V. Bistola, M. Anastasiou-Nana, M. Shochat, A. Shotan, M. Kazatsker, V. Gurovich, A. Asif, E. Noiman, Y. Levy, D. Blondhaim, P. Rabinovich, S. Meisel, S. Petrovic, J. Glasnovic, M. Tomasevic, D. Sakac, S. Obradovic, O. Londono Sanchez, S. Pacreu, L. Torres, G. Mihaylov, G. M. Shaban, E. Trendafilova, V. Krasteva, T. S. Mudrov, J. P. Didon, V. Panageas, N. Vlachos, A. Pernat, I. Radan, H. Mozina, P. Pepi, F. Cionini, N. Baccaglioni, A. Viertel, J. Havers, G. Ballard, G. Groenefeld, L. M. Branco, L. Ferreira, A. Fiarresga, L. Lettieri, A. Reggiani, R. Juarez Prera, G. Blanco Palacios, A.- C. Martin, S. Manzo Silberman, A. Chaib, O. Varenne, P. Allouch, E. Salengro, A. Jegou, O. Margot, C. Spaulding, A. Diego, A. De Miguel, C. Cuellas, E. Fraile, J. Martin, B. Vega, R. Bangueses, F. Fernandez-Vazquez, A. Perez De Prado, S. Leal, M. J. Correia, J. C. Monge, J. Abecasis, C. Garcia-Garcia, I. Subirana, J. Sala, J. Bruguera, V. Valle, G. Sanz, M. Fiol, F. Aros, J. Marrugat, R. Elosua, S. N. C. Barra, A. Leitao Marques, Y. J. Yang, B. Xu, G. Y. Song, R. L. G, A. Aleksic, P. Serpytis, K. Rucinskas, A. Kalinauskas, N. Karvelyte, C. I. Santos De Sousa, S. Ferreira, J. Calaca, N. Lousada, R. Palma Reis, D. M. Gualandro, L. F. B. C. Seguro, F. G. M. Braga, O. M. Silvestre, R. L. Lage, J. Fabri, M. T. Oliveira, J. A. Urbano Moral, J. Torres Llergo, R. Solanilla Rodriguez, A. Sanchez Gonzalez, A. Martinez Martinez, C. A. Den Uil, W. K. Lagrand, M. Van Der Ent, L. S. D. Jewbali, J. M. Cheng, P. E. Spronk, M. L. Simoons, C. Mornos, D. Dragulescu, A. Ionac, J. Guardado, O. Azevedo, M. Fernandes, F. Canario-Almeida, V. Sanfins, A. Pereira, J. Almeida, V. U. Kaplunova, Y. N. Belenkov, E. V. Privalova, A. A. Fomin, A. Y. Suvorov, A. Goodkova, M. G. Rubakova, I. A. Kuznetsova, E. N. Semernin, F. Keshavarzi, J. Kojuri, V. M. Mikhailov, I. V. Vezhenkova, A. Y. A. Goodkova, I. Pavlovic, M. Schwarz, G. Jakl, P. Smetana, T. Perkmann, A. Mayr, J. Mair, G. Klug, M. Schocke, T. Trieb, W. Jaschke, O. Pachinger, B. Metzler, L. Bronze Carvalho, J. Azevedo, M. L. Andrade, M. J. Relvas, J. Coucello, G. Morais, M. Seabra, F. Afamefule, M. Luaces Mendez, R. Teijeiro-Mestre, I. J. Nunez-Gil, N. Leco-Gil, E. Madronal-Cerezo, I. Zannin, J. Ruiz, M. A. Orynchak, I. I. Vakalyuk, I. P. Vakalyuk, A. Berezin, T. Panasenko, Y. Cavusoglu, A. Cavusoglu, I. Unluoglu, M. Tek, C. Demirustu, B. Gorenek, M. Unalacak, A. Birdane, F. Yuksel, N. Ata, J. P. J. Halcox, A. Beyaztas, E. Entok, I. Uslu, A. Schaefer, U. Flierl, N. Seydelmann, J. Bauersachs, L. Calmac, S. Marinescu, G. Tatu Chitoiu, A. G. Fruntelata, S. Hamdi, Y. Maazoun, A. Neji, O. Farhat, M. Majdoub, K. Ben Hamda, F. Maatouk, S. M. Balanescu, I. Nedelciuc, D. Deleanu, F. Ortan, S. Mot, P. R. Sinnaeve, S. Moreels, M. Coosemans, T. Vydt, W. Desmet, D. Tobing, R. Rifnaldi, D. Juzar, I. Firdaus, S. Dharma, I. Irmalita, H. Kalim, R. Bejiqi, R. Retkoceri, H. Bejiqi, L. Kryeziu, M. Kelmendi, S. H. Borovci, S. M. Victor, A. Gnanaraj, R. Deshmukh, A. S. Mullasari, M. Yahalom, R. S. Kaiyal, N. Roguin, J. Bornstein, S. Atar, R. Farah, L. F. Seca, A. M. Leitao Marques, R. Margato, P. Sousa, H. Ribeiro, L. Rocha, A. Correia, J. I. Moreira, H. C. Carvalho, M. Afifi, N. Abed, A. Suarez-Barrientos, D. Vivas, F. Castro-Ferreira, E. Franco, J. C. Garcia-Rubira, V. Fuster, C. Macaya, B. Ibanez Cabeza, S. Salinger, D. Milic, T. Stanojlovic, T. Kostic, M. A. Khan, F. Vrapi, K. Naeem, J. Davar, K. Hristova, G. Pencheva, R. Radeva, S. Milanov, A. Fareed, M. Oraby, G. M. Nasr, F. Maklady, P. Dupouy, J. T. Sorensen, C. J. Terkelsen, J. F. Lassen, S. Trautner, E. F. Christensen, T. T. Nielsen, H. E. Botker, H. R. Andersen, K. A. Thygesen, L. Checco, T. Usmiani, P. L. Sbarra, M. Boffini, R. Saviolo, C. Grasso, F. Conrotto, M. Marchetti, M. Rinaldi, S. Marra, F. Moscoso Costa, J. Ferreira, L. Raposo, C. Aguiar, M. Trabulo, J. A. Silva, V. Marques, A. Swiatkowski, J. Kowalczyk, R. Lenarczyk, P. Chodor, G. Honisz, T. Was, M. Swierad, B. Sredniawa, L. Polonski, Z. Kalarus, A. S. Postadzhiyan, H. Velinov, V. Velchev, D. Hazarbasanov, M. Apostolova, B. Finkov, M. Petrovic, A. Jovelic, T. Canji, I. Srdanovic, T. Popov, M. Golubovic, K. Pavlovic, N. Cemerlic-Adjic, J. Bro-Jeppesen, J. Kjaergaard, M. C. Wanscher, S. L. Nielsen, L. S. Rasmussen, C. Hassager, M. Khan, E. Crolla, H. Morley, L. Akeroyd, Y. Beaini, C. Morley, R. H. Bekeredjian, U. Krumsdorf, W. Rottbauer, H. A. Katus, S. Pleger, A. Botelho, N. Quintal, P. Faria, S. Gomes, J. C. Roussel, T. Senage, C. Perigaud, O. Habash, M. Michel, M. Treilhaud, P. Despins, J. N. Trochu, O. Baron, D. Duveau, A. N. Kitsiou, K. Giannakopoulos, G. Papadimitriou, S. Karas, Z. Babic, V. Nikolic Heitzler, D. Milicic, M. Bergovec, M. Raguz, J. Mirat, M. Strozzi, Z. Plazonic, L. Giunio, R. Steiner, M. Freynhofer, I. Brozovic, V. Bruno, L. Leherbauer, M. Djurkovic, M. Willheim, W. Huebl, S. Hahne, I. Kozanli, K. Kalla, A. Geppert, G. Unger, A. F. Simoes Marques Assuncao Caetano, C. Faustino, A. Ariza Sole, J. C. Sanchez Salado, V. Lorente Tordera, V. Martinez Garcia, J. Salazar Mendiguchia Y Garcia, J. A. Gomez Hospital, J. Maristany Daunert, F. J. Berdejo Gago, E. Esplugas Oliveras, A. Brzozowska-Czarnek, A. Urbanik, N. Kakouros, S. Kakouros, J. Lekakis, J. Rizos, D. Kokkinos, J. Venevtseva, A. Melnikov, M. Valiahmetov, T. Gomova, I. Perelomova, J. J. Ferrer Hita, F. Bosa-Ojeda, A. Sanchez-Grande-Flecha, G. Yanes-Bowden, M. J. Vargas-Torres, A. Rodriguez-Gonzalez, C. Rubio-Iglesias-Garcia, A. Dominguez-Rodriguez, C. Enjuanes-Grau, F. Marrero-Rodriguez, A. I. Suceveanu, A. Suceveanu, L. Mazilu, L. Alexandrescu, E. Dumitru, V. Miu, V. Jitari, F. L. Voinea, K. P. Balachandran, R. Schofield, R. Sankaranarayanan, K. Helm, C. Crowe, R. Singh, J. Mcdonald, M. J. Chuen, M. Kobusiak-Prokopowicz, M. Preglowska, A. Mysiak, T. Doi, T. Sakoda, T. Akagami, T. Naka, T. Tsujino, T. Masuyama, M. Ohyanagi, N. Kume, H. Mitsuoka, K. Hayashida, M. Tanaka, L. M. Biasucci, R. Della Bona, G. Biasillo, M. Leo, M. Zaninotto, M. Plebani, F. Crea, R. Dellabona, B. Gok, A. Unalir, B. Timuralp, N. Nikulina, S. S. Yakushin, G. I. Furmenko, S. A. Akinina, R. Ingrid, L. Bronze, S. Djambazov, A. Zhivkov, I. Maznev, M. Ingeliev, R. Slavov, N. Cvetkova, V. Patarinski, L. Groch, J. Horak, N. Dimitrov, H. G. Hayrapetyan, P. Cabanas-Grandio, C. Pena-Gil, N. A. Mc Keag, C. J. Mc Cann, C. Cardwell, I. S. Young, N. Mikhalchikova, N. Burova, M. Zaccaria, P. Palmisano, V. Palumbo, M. M. Ciccone, S. Favale, K. C. Chen, W. H. Yin, J. H. Liu, S. Goncalves, J. F. Santos, P. Amador, L. N. Soares, K. Zahidova, F. Guliyev, N. Zahidov, P. Carrilho-Ferreira, J. S. Marques, J. Carvalho De Sousa, H. Uthoff, C. Thalhammer, M. Potocki, T. Reichlin, M. Noveanu, M. Aschwanden, D. Staub, N. Arenja, T. Socrates, C. Mueller, Y. Zhao, X. Wu, Q. Xue, L. Gao, H. Lin, S. Wang, K. Watanabe, A. Kawamura, T. Seko, A. Omura, S. Sakabe, A. Kasai, A. V. Starodubova, G. Storozhakov, O. Kisliak, F. Hautieva, M. Tursheva, N. Fedotova, R. C. Di Maio, J. Mclaughlin, J. D. Allen, J. M. C. Anderson, H. Khaled Nagi, O. Tayeh, W. Farok, A. Mousa, P. Neuzil, J. Skoda, J. Petru, L. Sediva, S. Kralovec, F. Holy, K. Holdova, P. Jehlicka, P. Plasil, V. Y. Reddy, S. Alabakovska, D. Labudovic, S. Jovanova, K. Tosheska, M. Alabakovski, K. Jeevaratnam, S. P. Tee, Y. Zhang, L. Guzadhur, I. S. Gurung, R. Duehmke, A. A. Grace, M. Lei, C. L. Huang, Y. Ishibashi, M. Yamauchi, Y. Akashi, H. Musha, F. Miyake, T. Hnatek, L. Kamenik, P. Sedlon, J. Luxova, B. Steuerova, J. Skvaril, M. Cernohous, M. Zavoral, N. Ratkovic, N. R. Nemanja Djenic, A. J. Aleksandra Jovelic, S. O. Slobodan Obradovic, B. G. Branko Gligic, E. Kletsiou, M. Giannakopoulou, E. Bozas, E. K. Iliodromitis, E. D. E. Papathanassoglou, M. Anton, G. Anton, M. Muraru, S. Salinger Martinovic, M. Radosavljevic, D. Stanojevic, M. Zivkovic, T. Pessoa, N. Aspromonte, C. Ronco, M. Tubaro, M. Santini, F. Colivicchi, A. Aiello, D. Cruz, A. Anzoletti Boscolo, G. Vianello, R. Valle, A. Parspour, S. Watkins, D. Datta, A. G. Nikishin, M. M. Pirnazarov, T. A. Nurbaev, Z. Motovska, M. Fischerova, P. Osmancik, M. Maly, P. Widimsky, E. Pavli, A. Dibra, J. Mehilli, L. Dibra, A. Schoemig, A. Kastrati, P. Carmo, M. Almeida, R. Teles, P. Goncalves, J. Brito, F. D'ascenzo, A. Gonella, G. Longo, A. Pullara, C. Moretti, F. Sciuto, P. Omede', G. Biondi Zoccai, G. P. Trevi, I. Sheiban, H. M. Cafe, D. Pereira, D. Freitas, D. Ortiz Berbel, J. M. Rabasa Baraibar, A. M. Leone, A. De Caterina, A. Aurelio, A. Sciahbasi, E. Lioy, C. Trani, F. Burzotta, I. Porto, A. G. Rebuzzi, K. Trusinskis, D. Juhnevica, K. Strenge, D. Sondore, I. Kumsars, S. Jegere, I. Narbute, A. Grave, I. Zakke, A. Erglis, C. Ferrari, A. L. Bartorelli, M. Saeed, D. Cozma, S. Pescariu, S. I. Dragulescu, H. S. Kamal, A. Abdelfattah, A. M. Abdelbary, H. Elassar, A. Naggar, M. Khaled, A. M. Fareed, J. M. Pernes, J. C. Gaux, M. W. Prull, B. Sasko, H. Wirdemann, A. Bittlinsky, T. Butz, H. J. Trappe, M. Perazzolo Marra, L. Cacciavillani, A. Marzari, M. De Lazzari, R. Turri, P. China, F. Corbetti, S. Iliceto, L. L. Stazhadze, E. A. Spiridonova, N. A. Bulanova, A. A. Ermolaev, L. Savic, I. Mrdovic, G. Krljanac, J. Perunicic, M. Asanin, R. Lasica, M. Matic, Z. Vasiljevic, M. Ostojic, M. Tichy, C. Andrys, A. Conti, C. Poggioni, G. Viviani, F. Bulletti, V. Boni, M. Luzzi, S. Vicidomini, M. Donati, B. Del Taglia, R. Pini, O. Sousa, R. Fontes-Carvalho, D. Caeiro, N. Dias Ferreira, G. Silva, E. Pereira, J. Ribeiro, A. Albuquerque, V. Gama Ribeiro, M. Murai, Y. Takeda, T. Shinmyo, J. Tanigawa, H. Hazui, T. Nakakohji, Y. Ohishi, M. Hoshiga, T. Ishihara, T. Hanafusa, J. Belohlavek, V. Rohn, J. Kunstyr, M. Lips, M. Semrad, F. Mlejnsky, J. Tosovsky, A. Linhart, J. Lindner, Z. Sablik, A. Samborska-Sablik, J. Drozdz, W. Gaszynski, M. M. Izquierdo-Gomez, R. Juarez-Prera, G. Blanco-Palacios, R. Lakhdar, M. Drissa, B. Jedaida, H. Drissa, F. Sampaio, H.- T. Hsin, J.- H. Huang, K.- M. Chiu, Z.- S. Chen, P.- C. Lin, L.- Y. Chen, S.- H. Chu, I. Efthimiadis, P. Skendros, A. Sarantopoulos, P. Boura, A. M. Van Der Laan, P. A. Van Der Vleuten, M. Klees, J. G. P. Tijssen, B. E. Backus, A. J. Six, J. H. Kelder, A. Mosterd, E. G. Mast, T. P. Mast, R. Braam, R. Tio, R. Veldkamp, P. A. Doevendans, N. Paarup Dridi, L. Holmvang, T. Engstroem, S. Rekik, J. Brunet, F. X. Hager, G. Bayet, L. Meille, J. M. Quatre, J. Sainsous, P.- H. Chu, C.- H. Tang, N. Pogosova, I. E. Koltunov, I. D. Sapunova, V. A. Vigodin, R. Uhliar, A. Schmidt, B. Brockmeyer, A. Suzuki, Y. Eki, H. Higuchi, A. Yukawa, R. Yamauchi, Y. Sato, Y. Endo, J. Salazar Mendigucha Garcia, S. Homs Vila, A. Cequier Fillat, R. Andion Ogando, M. Sandin Fuentes, J. M. Vegas Valle, I. A. Gonzalez Garcia, I. A. Duro Aguado, A. J. Palomino Doza, I. Gomez Salvador, J. A. San Roman Calvar, T. M. Mamarasulov, L. Todorovic, Z. C. H. Cherneva, S. D. Denchev, K. Heltai, A. Boytsov, N. N. Nikulina, D. Zanna, V. Marangelli, C. Caiati, R. Picon Heras, M. J. Loureiro, I. Urazovskaya, D. Vinogradova, E. Vasilieva, A. Shpektor, E. Conti, M. B. Musumeci, F. M. Lauri, E. Dito, M. De Giusti, A. Lallo, D. Fusco, M. Davoli, M. Volpe, C. Autore, H. Gamra, Z. Dridi, M. Hassine, F. Addad, I. Gherissi, A. Reda, M. Mahjoub, S. Bouraoui, M. Abdennadher, F. Betbout, P. M. F. P. Mota, J. D. Silva, R. Jankovic Tomasevic, V. Djordjevic, D. Djordjevic Radojkovic, A. Scafa Udriste, A. Fruntelata, E. Gainoiu, S. Bogdan, D. Zamfir, C. Teodorescu, M. Guran, D. Constantinescu, A. Konopka, M. Banaszewski, I. Wojtkowska, J. Stepinska, J. V. Vidergold, I. V. Osipova, T. V. Tavrovskaya, J. V. Galkina, A. V. Timofeev, R. I. Vorobyov, E. N. Vorobyova, L. Matos, A. C. C. Carvalho, W. Oliveira, F. Cintra, D. Poyares, M. Andersen, R. Martins, S. Tufik, P. Ostadal, J. Brada, S. Horakova, M. Mlcek, V. Hrachovina, O. Kittnar, I. V. Gorudko, I. V. Buko, S. N. Cherenkevich, L. Z. Polonetsky, V. Y. Plotkin, M. A. Timoshina, S. V. Azanchevskaya, N. N. Chromov-Borisov, A. Vorlat, L. Snoep, M. J. Claeys, C. J. Vrints, A. Palazzuoli, M. Caputo, I. Quatrini, A. Calabro, G. Antonelli, M. S. Campagna, B. Franci, R. Nuti, A. Maisel, M. Negrini, T. Minora, P. Marino, R. Seregni, E. Tavlueva, O. Barbarash, L. Barbarash, T. Janota, J. Kudlicka, K. Malik, D. Wichterle, J. Hradec, R. Body, S. D. Carley, G. Mcdowell, M. Nuttall, C. Wibberley, M. France, J. K. Cruickshank, K. Mackway-Jones, M. Leon, C. Cozma, F. Mitu, D. R. Almeida, C. B. Dias, I. Burazor, M. Burazor, M. Krstic, M. Lazovic, M. Vukmanovic, J. Djordjevic, Z. Radovanovic, D. Ilic, P. Bosnjakovic, A. C. Ferreira, P. S. Mateus, P. Fontes, T. Teixeira, G. Conte, A. Menozzi, E. Solinas, M. G. Bolognesi, I. Tadonio, F. Mantovani, A. Cattabiani, L. Vignali, D. Ardissino, O. Tautu, A. Alexandrescu, R. Niculescu, R. Jankovic, N. Bozinovic, C. Santos, F. Costa, G. Cardoso, I. Correia, K. Fountoulaki, S. Kastellanos, E. Voltirakis, A. Kokotos, C. Michalakeas, K. Kontsas, K. Hasioti, E. T. Iliodromitis, M. G. Sandin Fuentes, E. Zatarain Nicolas, N. Martinez Uruena, M. Alvarado Montes De Oca, V. Dytrych, T. Kovarnik, O. Smid, A. Kral, A. G. Aroutunov, S. Intwala, I. Jegere, H. S. H. Shaalan, Z. Pagava, R. Agladze, R. Shakarishvili, N. Sharashidze, L. Gujejiani, G. Saatashvili, T. Z. Katova, V. Kostova, Y. Simova, S. Vukotic, S. Rafajlovski, R. Romanovic, N. Antonijevic, B. Gligic, M. Hutyra, T. Skala, D. Horak, D. Vindis, M. Taborsky, A. Contine, M. Del Pinto, F. Angeli, P. Verdecchia, F. Borgognoni, E. Grikstaite, P. Pantano, G. Ambrosio, C. Cavallini, C. Bonanad, J. Sanchis, V. Bodi, J. Nunez, X. Bosch, M. Heras, M. Pellicer, A. Llacer, L. Adao, M. Oliveira, H. Goncalves, J. Primo, V. Gama, C. Lombardi, M. Metra, S. Bugatti, E. Pasotti, F. Quinzani, M. Adamo, C. Villa, R. Rovetta, A. Manerba, M. Mariani, A. Dushpanova, M. Baroni, E. Cerone, A. Nardelli, J. Gianetti, S. Berti, F. Feliciano, R. Soares, S. Santos, A. Kruger, D. Vondrakova, J. Herget, C. Navarro, N. A. Cromie, J. A. A. Adgey, D. Caeiro Pereira, P. Braga, R. Fontes Carvalho, A. Rodrigues, M. Goncalves, L. Simoes, and K. V. Borisov
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Cardiology and Cardiovascular Medicine - Published
- 2010
30. Isomerism of low-lying states in 86Y
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C. Rusu, R. Mărginean, G. Cata-Danil, N. Marginean, T. Sava, I. Căta-Danil, A. Iordachescu, D. M. Filipescu, S. Pascu, D. Deleanu, G. Suliman, T. Glodariu, L. Stroe, D. Ghiţă, M. Ivascu, D. Bucurescu, N. V. Zamfir, M. Ionescu-Bujor, and C. Mihai
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Spherical model ,Physics ,Nuclear and High Energy Physics ,Valence (chemistry) ,Atomic orbital ,Proton ,Hadron ,Nuclear fusion ,Neutron ,Configuration space ,Atomic physics - Abstract
Low-energy isomeric states of 86Y were populated in the reaction 73Ge + 16O at 57MeV and were investigated by means of delayed n $ \gamma$ and $ \gamma$ $ \gamma$ coincidences. A half-life of 70(7)ns was measured for the 5- state at 208keV, yielding an exceptionally small B(M1) value of 2.0(7)×10-5 W.u. and a B(E2) value of 0.34(+24 -13) W.u. For the other three known isomeric states at 218, 243, and 302keV, the half-lives extracted from the present experimental data are in very good agreement with previous measurements. Given the newly observed isomeric character of the 5- 208keV state, the re-analysis of earlier experimental data on the 302keV isomer led to a new spin-parity assignment, 6+, for this state. In addition, this re-evaluation provided two g -factors, -0.083(3) and +0.63(2) , for the 208 and 302keV states, respectively. The results are discussed in terms of spherical-shell model calculations performed with a truncated space of configurations built on the f 5/2 , p 3/2 , p 1/2 , and g 9/2 valence orbitals. Effective spin, orbital, and “tensor” g -factors were determined empirically for protons and neutrons in the considered configuration space.
- Published
- 2010
31. Measurement of the 90Sr absolute activity using the autocorrelation single-crystal scintillation method
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N. A. Lebedev, N. V. Morozova, D. V. Filosovof, S. Pascu, Gh. Căta-Danil, D. Ghiţă, T. Badica, D. Deleanu, I. V. Popescu, and V.A. Morozov
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Radionuclide ,Scintillation ,Isotope ,business.industry ,Chemistry ,Health, Toxicology and Mutagenesis ,Autocorrelation ,Public Health, Environmental and Occupational Health ,Pollution ,Analytical Chemistry ,Computational physics ,Optics ,Nuclear Energy and Engineering ,Range (statistics) ,Radiology, Nuclear Medicine and imaging ,business ,Single crystal ,Spectroscopy - Abstract
It is shown for the first time that the ASCSTS technique we have introduced several years ago for lifetime measurements can be also used for measuring low level activities. A good example with practical relevance in this respect is 90Sr isotope. In order to apply this technique the radioactive isotope must have an isomeric state with a lifetime spanning the ns–μs range. This method is adequate for measuring weak activities with high detection efficiency in a geometry close to 4π. It is experimentally demonstrated that ASCSTS method is a reliable, high efficiency technique for measuring absolute radioactivity in the long radioactive chains.
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- 2010
32. Lifetime of the yrastIπ=5−state andE1hindrance in the transitional nucleusCe58136
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Mohammad Nakhostin, K. Mulholland, R. Mărginean, C. R. Nita, C. Mihai, N. Alkhomashi, R. Britton, D. Ghita, D. Deleanu, T. Sava, T. Glodariu, A. Negret, Alison Bruce, D. Bucurescu, Zs. Podolyák, N. V. Zamfir, C. Townsley, P. H. Regan, N. Marginean, Oliver J. Roberts, D. M. Filipescu, R. Lica, T. Alharbi, and L. Stroe
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Physics ,Nuclear and High Energy Physics ,education.field_of_study ,Isotone ,Yrast ,Population ,State (functional analysis) ,Ionizing radiation ,medicine.anatomical_structure ,Pi ,medicine ,Atomic physics ,Spectroscopy ,education ,Nucleus - Abstract
The half-lives o fthe I=5- and 7- yrast stateys with Ex=1978 kev and Ex=2307 keV in the N=78 isotone 136Ce have been measured to be 496(23) ps and 270(24) ps respectively , using the concident fast-timing spectroscopy technique following population by a 124Sn(16O,4n) fusion-evporation reaction at an incident beam energy of 68 MeV.
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- 2015
33. Separation of the 1+/1− parity doublet in 20Ne
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J. Beller, C. Stumpf, M. Scheck, N. Pietralla, D. Deleanu, D.M. Filipescu, T. Glodariu, W. Haxton, A. Idini, J.H. Kelley, E. Kwan, G. Martinez-Pinedo, R. Raut, C. Romig, R. Roth, G. Rusev, D. Savran, A.P. Tonchev, W. Tornow, J. Wagner, H.R. Weller, N.-V. Zamfir, and M. Zweidinger
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Parity violation ,Parity doublet ,High Energy Physics::Phenomenology ,High Energy Physics::Experiment ,ddc:530 ,Nuclear Experiment ,lcsh:Physics ,lcsh:QC1-999 - Abstract
The (J,T)=(1,1) parity doublet in 20Ne at 11.26 MeV is a good candidate to study parity violation in nuclei. However, its energy splitting is known with insufficient accuracy for quantitative estimates of parity violating effects. To improve on this unsatisfactory situation, nuclear resonance fluorescence experiments using linearly and circularly polarized γ-ray beams were used to determine the energy difference of the parity doublet ΔE=E(1−)−E(1+)=−3.2(±0.7)stat(−1.2+0.6)sys keV and the ratio of their integrated cross sections Is,0(+)/Is,0(−)=29(±3)stat(−7+14)sys. Shell-model calculations predict a parity-violating matrix element having a value in the range 0.46–0.83 eV for the parity doublet. The small energy difference of the parity doublet makes 20Ne an excellent candidate to study parity violation in nuclear excitations. Keywords: Parity doublet, Parity violation
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- 2014
34. Erratum: Structure ofLa130at low and medium spins [Phys. Rev. C90, 014323 (2014)]
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D. M. Filipescu, A. Negret, Ioana Gheorghe, A. Iordachescu, Nilberto H. Medina, C. Mihai, D. Deleanu, M. Ionescu-Bujor, D. Ghiţă, N. Marginean, T. Glodariu, R. Mărginean, F. Brandolini, C. A. Ur, L. Stroe, R. Lica, and D. Bucurescu
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Physics ,Nuclear and High Energy Physics ,Spins ,Condensed matter physics ,Structure (category theory) - Published
- 2014
35. Structure ofLa130at low and medium spins
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R. Mărginean, L. Stroe, N. Marginean, A. Negret, M. Ionescu-Bujor, F. Brandolini, D. Ghiţă, Ioana Gheorghe, C. Mihai, C. A. Ur, T. Glodariu, A. Iordachescu, D. Deleanu, D. Bucurescu, D. M. Filipescu, R. Lica, and Nilberto H. Medina
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Coupling constant ,Physics ,Nuclear and High Energy Physics ,Crystallography ,Angular distribution ,Spins ,Lattice (order) ,Quadrupole ,Ground state ,Spectroscopy - Abstract
Low- and medium-spin states of the odd-odd nucleus $^{130}\mathrm{La}$ were studied by in-beam and pulsed-beam $\ensuremath{\gamma}$-ray spectroscopy using the $^{121}\mathrm{Sb}(^{12}\mathrm{C},3n)$ and $^{116}\mathrm{Sn}(^{16}\mathrm{O},pn)$ fusion-evaporation reactions. The decay out of the $\ensuremath{\pi}{h}_{11/2}\ensuremath{\bigotimes}\ensuremath{\nu}{h}_{11/2}$ and $\ensuremath{\pi}{h}_{11/2}\ensuremath{\bigotimes}\ensuremath{\nu}{g}_{7/2}$ rotational structures to the ground state has been elucidated. Spin and parity values have been assigned to most of the newly observed states, as well as to the bandheads of the rotational bands. Two isomeric states were identified and placed in the level scheme, with the characteristics ${J}^{\ensuremath{\pi}}={5}^{+},{E}_{x}=214.0$ keV, ${T}_{1/2}=0.76(9)$ $\ensuremath{\mu}$s and ${J}^{\ensuremath{\pi}}={6}^{+},{E}_{x}=319.1$ keV, ${T}_{1/2}=33(1)$ ns. The magnetic and quadrupole interactions of the ${6}^{+}$ isomeric state have been investigated by the time-differential perturbed $\ensuremath{\gamma}$-ray angular distribution method. The $g$ factor value, $g({6}^{+})=+0.48(3)$, and the quadrupole coupling constant in polycrystalline metallic Sn lattice, ${\ensuremath{\nu}}_{Q}({6}^{+})=37(4)$ MHz, have been derived. The experimental data are compared with the predictions of two-quasiparticles plus rotor model calculations.
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- 2014
36. Fast-timing lifetime measurements of excited states inCu67
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D. Pantelica, Gianluca Colò, E. Wilson, S. Toma, A. Negret, D. Bucurescu, S. Leoni, L. Stroe, P. J. R. Mason, D. Ghita, T. Sava, Alison Bruce, P. H. Regan, N. Marginean, Zsolt Podolyak, S. Bottoni, D. Deleanu, G. Cata-Danil, A. Bracco, T. Glodariu, C. R. Nita, C. Mihai, M. Avrigeanu, R. Mărginean, C. A. Ur, D. M. Filipescu, and G. Bocchi
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Coupling ,Physics ,Nuclear and High Energy Physics ,Proton ,Yrast ,Nuclear Theory ,Function (mathematics) ,State (functional analysis) ,medicine.anatomical_structure ,Excited state ,medicine ,Atomic physics ,Ground state ,Nucleus - Abstract
The half-lives of the 9/2 + , 13/2+ , and 15/2+ yrast states in the neutron-rich 67Cu nucleus were determined by using the in-beam fast-timing technique. The experimentally deduced E3 transition strength for the decay of the 9/2+ level to the 3/2- ground state indicates that the wave function of this level might contain a collective component arising from the coupling of the odd proton p3/2 with the 3- state in 66Ni. Theoretical interpretations of the 9/2+ state are presented within the particle-vibration weak-coupling scheme involving the unpaired proton and the 3- state from 66Ni and within shell-model calculations with a 56Ni core using the jj44b residual interaction. The shell model also accounts reasonably well for the other measured electromagnetic transition probabilities.
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- 2014
37. Probing particle-phonon-coupled states in the neutron-rich nucleusCu65by lifetime measurements with fast-timing techniques
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B. Belvito, D. Bucurescu, I Georghe, C. A. Ur, P. F. Bortignon, A. Bracco, C. R. Nita, G. Bocchi, R. Lica, C. Mihai, Sibel Zehra Aydin, G. Benzoni, A. Negret, D. M. Filipescu, S. Leoni, L. Stroe, Gianluca Colò, R. Mărginean, N. Marginean, S. Bottoni, R. Suvaila, D. Deleanu, S. Toma, D. Ghita, T. Sava, and T. Glodariu
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Imagination ,Physics ,Nuclear and High Energy Physics ,Thesaurus (information retrieval) ,Chemical substance ,Phonon ,media_common.quotation_subject ,Nuclear physics ,Search engine ,medicine.anatomical_structure ,medicine ,Particle ,Neutron ,Nucleus ,media_common - Published
- 2014
38. Search for particle–vibration coupling in 65Cu
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T. Sava, D Ghiţǎ, D. M. Filipescu, Ioana Gheorghe, R. Şuvǎilǎ, R. Licǎ, A. Negreţ, A. Bracco, C. A. Ur, D. Deleanu, G. Benzoni, C. R. Nitǎ, C. Mihai, G. Bocchi, T. Glodariu, Pier Francesco Bortignon, Gh. Cǎta-Danil, S. Leoni, L. Stroe, N. Mǎrginean, S. Bottoni, I. Cǎta-Danil, R. Mǎrginean, D. Bucurescu, and Gianluca Colò
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Physics ,Baryon ,Nuclear physics ,Coupling ,Proton ,QC1-999 ,Hadron ,Elementary particle ,Fermion ,Atomic physics ,Nucleon ,Ground state - Abstract
The lifetime of the 9/2 + state of 65 Cu, at 2534 keV, has been measured by fast timing techniques, in order to establish wether such state arises from a weak coupling between a p3=2 proton and the 3 octupole vibration at 3.56 MeV in the 64 Ni core. The 65 Cu nucleus was populated by the reaction 7 Li + 64 Ni at 32 MeV, at the Horia Hu- lubei National Institute of Physics and Nuclear Engineering (NIPNE) in Bucharest, and its -decay was detected by the ROSPHERE array. The measured lifetime coresponds to a B(E3) reduced transition probability to the ground state equal to 8.89 W.u., in agreement with theoretical predictions in the weak coupling limit.
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- 2014
39. Quadrupole collectivity in neutron-rich Cd isotopes
- Author
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K. Nowak, G. S. Simpson, Marcus Scheck, Jan Diriken, Roman Gernhäuser, P. G. Thirolf, G. Rainovski, K. Hadyńska-Kęk, Pascal Fernier, C. Bauer, A. Illana Sisón, R. Lutter, B. Siebeck, Tomás R. Rodríguez, M. Thürauf, T. Kröll, D. Voulot, F. Wenander, R. Stegmann, A. Blazhev, D. L. Balabanski, A. Jungclaus, S. Ilieva, Thierry Stora, T. Bloch, S. Bönig, A. Negret, M. J. Vermeulen, D. Deleanu, Janne Pakarinen, M. Seidlitz, M. von Schmid, N. Warr, R. Orlandi, H. De Witte, Federal Ministry of Education and Research (Germany), Helmholtz International Center for FAIR, Lunardi, S, Bizzeti, PG, Kabana, S, Bucci, C, Chiari, M, Dainese, A, DiNezza, P, Menegazzo, R, Nannini, A, Signorini, C, and ValienteDobon, JJ
- Subjects
Physics ,Isotope ,QC1-999 ,Coulomb excitation ,Prolate spheroid ,Astrophysics ,7. Clean energy ,Semiconductor detector ,Transition strength ,Quadrupole ,Neutron ,Atomic physics ,Nuclear Experiment ,Excitation - Abstract
4 pags., 2 figs. -- INPC 2013 – International Nuclear Physics Conference, The investigation of the excitation energies of the 21+ –states in the neutron-rich Cd isotopes shows an irregular behaviour when approaching the neutron shell-closure at N = 82. The energy of the 21+–state in 128Cd is lower than the one in 126Cd. The transition strength B(E2, 0gs+ → 21+) in the even isotopes 122−128Cd was measured in Coulomb excitation experiments with the high-purity germanium detector array MINIBALL at REXISOLDE (CERN). The values for 122,124Cd coincide with beyond-mean-field calculations with a resultant prolate deformation, whereas 126,128Cd are better described by shell-model calculations., This project is supported by BMBF (No. 06 DA 9036I, No. 05 P12 RDCIA, No. 05 P12 RDCIB and No. 05 P12 PKFNE), HIC for FAIR, EU through EURONS (No. 506065) and ENSAR (No. 262010) and the MINIBALL and REX-ISOLDE collaborations.
- Published
- 2014
40. Precision Lifetime Measurements Using LaBr3 Detectors With Stable and Radioactive Beams
- Author
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P. C. Bender, Thamer Alharbi, P. H. Regan, Stephen Rice, S. Kisyov, A. Negret, C. Townsley, D. M. Filipescu, R. Mǎrginean, P. A. Söderström, G. Suliman, Zs. Podolyák, N. Alazemi, Hirofumi Watanabe, L. Stroe, P. J. R. Mason, R. Britton, I. Căta-Danil, D. Deleanu, N. Cooper, C. R. Nita, P. Detistov, Mohammad Nakhostin, K. Mullholland, C. Mihai, D. Ghitǎ, G. Cata-Danil, V. Werner, Toshiyuki Sumikama, U. Garg, N. Alkhomashi, T. Sava, Alejandro Algora, F. Browne, J. F. Smith, Alison Bruce, S. Lalkovski, Oliver J. Roberts, Sean Liddick, N. Mǎrginean, T. Glodariu, D. Bucurescu, E. Wilson, and Z. Patel
- Subjects
Physics ,Scintillation ,010308 nuclear & particles physics ,QC1-999 ,Detector ,Astrophysics ,01 natural sciences ,7. Clean energy ,Particle detector ,Semiconductor detector ,Nuclear physics ,Excited state ,0103 physical sciences ,Scintillation counter ,Measuring instrument ,Physics::Accelerator Physics ,Gamma spectroscopy ,010306 general physics ,Nuclear Experiment - Abstract
A range of high resolution gamma-ray spectroscopy measurements have been carried out using arrays which include a number of Cerium-doped Lanthanum-Tribromide (LrBr3 (Ce)) scintillation detectors used in conjunction with high-resolution hyper-pure germanium detectors. Examples of the spectral and temporal responses of such set-ups, using both standard point radioactive sources 152 Eu and 56 Co, and in-beam fusionevaporation reaction experiments for precision measurements of nuclear excited states in 34 P and 138 Ce are presented. The current and future use of such arrays at existing (EURICA at RIKEN) and future (NUSTAR at FAIR) secondary radioactive beam facilities for precision measurements of excited nuclear state lifetimes in the 10 ps to 10 ns regime are also discussed.
- Published
- 2013
41. PP.40.15
- Author
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R. Jurcut, D. Deleanu, I. Arsenescu, Ana Maria Daraban, Carmen Ginghina, and C. Scheau
- Subjects
Kidney ,medicine.medical_specialty ,medicine.anatomical_structure ,Complicated hypertension ,Physiology ,business.industry ,Internal medicine ,Internal Medicine ,Cardiology ,Medicine ,Cardiology and Cardiovascular Medicine ,business - Published
- 2015
42. Half-life of the yrast2+state in188W: Evolution of deformation and collectivity in neutron-rich tungsten isotopes
- Author
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D. Bucurescu, E. Wilson, I. Căta-Danil, D. Ivanova, M. Bunce, N. Cooper, Rachael Wood, M. Zhekova, C. Zhou, Ioana Gheorghe, Sean Liddick, D. M. Filipescu, R. Marginean, S. Toma, P-A Soederstroem, T. Glodariu, M. Bowry, Werner, G. Ilie, K. Mulholland, R. Lica, R. Suvaila, Paul Stevenson, R. Britton, D. Delion, L. Stroe, P. J. R. Mason, Stephen Rice, W. Gelletly, D. Deleanu, G. Cata-Danil, C. R. Nita, T. Alharbi, Jon Smith, Zsolt Podolyak, A. Negret, T. Sava, Alison Bruce, S. Kisyov, C. Townsley, G. Suliman, D. Ghita, S. Pascu, Alejandro Algora, C. Mihai, Oliver J. Roberts, T. Alexander, S. Lalkovski, P. H. Regan, and N. Marginean
- Subjects
Physics ,Nuclear and High Energy Physics ,Isotope ,Yrast ,Half-life ,chemistry.chemical_element ,Tungsten ,Semiconductor detector ,medicine.anatomical_structure ,chemistry ,Potential energy surface ,medicine ,Neutron ,Atomic physics ,Nucleus - Abstract
The half-life of the yrast I π = 2+ state in the neutron-rich nucleus 188W has been measured using fast-timing techniques with the HPGe and LaBr3:Ce array at the National Institute of Physics and Nuclear Engineering, Bucharest. The resulting value of t1/2 = 0.87(12) ns is equivalent to a reduced transition probability of B(E2; 2+ 1 → 0+ 1 ) = 85(12) W.u. for this transition. The B(E2; 2+ 1 → 0+ 1 ) is compared to neighboring tungsten isotopes and nuclei in the Hf, Os, and Pt isotopic chains. Woods-Saxon potential energy surface (PES) calculations have been performed for nuclei in the tungsten isotopic chain and predict prolate deformed minima with rapidly increasing γ softness for 184–192W and an oblate minimum for 194W.
- Published
- 2013
43. Cross sections for inelastic scattering of neutrons on28Si and comparison with the25Mg(α,n)28Si reaction
- Author
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L. Stroe, Ph. Dessagne, C. Borcea, N. Marginean, R. Mărginean, A. J. M. Plompen, A. Negret, T. Glodariu, S. Pascu, D. Ghita, T. Sava, D. Bucurescu, D. M. Filipescu, C. Mihai, M. Kerveno, and D. Deleanu
- Subjects
Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Neutron ,Inelastic scattering ,Inelastic neutron scattering - Published
- 2013
44. Excited states in129I
- Author
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G. Suliman, P. Detistov, Gh. Căta-Danil, N. Marginean, N. V. Zamfir, L. Stroe, E. Ganioglu, I. Căta-Danil, T. Sava, L. Atanasova, R. Mărginean, D. Bucurescu, C. Mihai, D. M. Filipescu, Ts. Venkova, M. Ivascu, S. Pascu, D. Ghiţă, D. L. Balabanski, D. Deleanu, T. Glodariu, and A. Negret
- Subjects
Physics ,Nuclear and High Energy Physics ,Routhian ,Excited state ,Oblate spheroid ,Parity (physics) ,Atomic physics ,Ground state ,Electronic band structure ,Hpge detector - Abstract
Excited states in ${}^{129}$I were populated with the ${}^{124}$Sn(${}^{7}$Li,$2n$) reaction at 23 MeV. In-beam measurements of $\ensuremath{\gamma}$-ray coincidences were performed with an array of eight HPGe detectors and five LaBr${}_{3}$(Ce) scintillation detectors. Based on the $\ensuremath{\gamma}\ensuremath{\gamma}$ coincidence data, a positive parity band structure built on the $7/{2}^{+}$ ground state was established and the $\ensuremath{\pi}{g}_{7/2}$ configuration at oblate deformation was assigned to it. The results are compared to interacting Boson-Fermion model (IBFM) and total Routhian surface (TRS) calculations.
- Published
- 2013
45. Electromagnetic transition rates in theN=80nucleus58138Ce
- Author
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N. Cooper, W. Gelletly, Sean Liddick, M. Bunce, S. Kisyov, T. Alharbi, T. Glodariu, A. Negret, R. Britton, D. Ghita, T. Sava, Mohammad Nakhostin, G. Ilie, Alison Bruce, D. Bucurescu, D. Deleanu, C. Townsley, K. Mulholland, D. M. Filipescu, L. Stroe, P. J. R. Mason, R. Mărginean, Edward Simpson, Zs. Podolyák, J. F. Smith, N. V. Zamfir, V. Werner, Stephen Rice, J. Lintott, E. Wilson, M. Zhekova, N. Alazemi, S. Lalkovski, P. H. Regan, N. Marginean, C. R. Nita, C. Mihai, Oliver J. Roberts, and Alejandro Algora
- Subjects
Physics ,Nuclear and High Energy Physics ,Work (thermodynamics) ,medicine.anatomical_structure ,Yrast ,Excited state ,SHELL model ,medicine ,Incident beam ,Anomalous behavior ,Atomic physics ,Nucleus ,Coincidence - Abstract
The half-life of the Iπ=6+ yrast state at Ex=2294 keV in 138Ce has been measured as T1/2=880(19) ps using the fast-timing γ-ray coincidence method with a mixed LaBr3(Ce)-HPGe array. The excited states in 138Ce have been populated by the 130Te(12C,4n) fusion-evaporation reaction at an incident beam energy of 56 MeV. The extracted B(E2;61+→41+)=0.101(24) W.u. value is compared with the predictions of truncated basis shell model calculations and with the systematics of the region. This shows an anomalous behavior compared to the neighboring isotonic and isotopic chains. Half-lives for the yrast 5-, 11+ and 14+ states in 138Ce have also been determined in this work.
- Published
- 2013
46. Half-life of theIπ=4−intruder state in34P:M2transition strengths approaching the island of inversion
- Author
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D. Bucurescu, N. V. Zamfir, G. Suliman, D. Ghita, N. Alkhomashi, D. Deleanu, P. H. Regan, P. Detistov, S. Pascu, A. Negret, R. Marginean, U. Garg, N. Marginean, CR Triguero, R. Chakrabarti, A. Kusoglu, S. S. Ghugre, T. Sava, T. Glodariu, M. Bowry, G. Cata-Danil, M. N. Erduran, A. K. Sinha, Edward Simpson, Alison Bruce, Zsolt Podolyak, Mohammad Nakhostin, Thamer Alharbi, M. Bostan, I. Căta-Danil, L. Stroe, P. J. R. Mason, P. C. Bender, C. Mihai, and D. M. Filipescu
- Subjects
Physics ,Nuclear and High Energy Physics ,Island of inversion ,Excited state ,Mixing ratio ,Half-life ,Neutron ,Atomic physics ,Coincidence ,Intruder state ,Semiconductor detector - Abstract
The half-life of the 2305-keV, Iπ=4(−) intruder state in 34P has been measured as t1/2=2.0(1) ns using γ-ray coincidence, fast-timing techniques with the Bucharest HPGe and LaBr3:Ce detector array. Excited states in 34P were populated using the 18O(18O,pn)34P fusion-evaporation reaction at a beam energy of 36 MeV. Reduced transition probabilities have been calculated for different values of the M2/E3 mixing ratio, δE3/M2, and compared with shell-model estimates. For small values of the mixing ratio, the B(M2) value was found to be consistent with similar transitions associated with the occupation of neutron f7/2 configurations in this mass region.
- Published
- 2012
47. Excited states of the150Pm odd-odd nucleus
- Author
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E. Drăgulescu, L. Stroe, Kathrin Wimmer, R. Krücken, D. Bucurescu, I. Căta-Danil, T. Faestermann, C. Mihai, D. Deleanu, D. M. Filipescu, A. Negret, R. Mărginean, H.-F. Wirth, N. Marginean, N. V. Zamfir, Ralf Hertenberger, K. Eppinger, T. Sava, S. Pascu, G. Cata-Danil, T. Glodariu, D. Ghiţă, and M. Ivascu
- Subjects
Physics ,Quantum phase transition ,Nuclear and High Energy Physics ,Nuclear structure ,Tandem accelerator ,Spectral line ,Nuclear physics ,medicine.anatomical_structure ,Excited state ,medicine ,Direct reaction ,Atomic physics ,Nuclear Experiment ,Spectroscopy ,Nucleus - Abstract
The knowledge of excited states in the odd-odd ${}^{150}$Pm, completely unknown until recently, is important both for understanding double $\ensuremath{\beta}$ decay of ${}^{150}$Nd and for nuclear structure studies in mass regions with a quantum phase transition. A large number of excited states have been determined for the first time in this nucleus by measuring spectra of the ${}^{152}$Sm($d$,$\ensuremath{\alpha}$) direct reaction at 25 MeV with the Munich Q3D spectrograph and by $\ensuremath{\gamma}$-ray spectroscopy with the ($p,n\ensuremath{\gamma}$) reaction at 7.1 MeV at the Bucharest tandem accelerator. Some of these levels correspond to peaks recently observed with the ${(}^{3}$He,$t$) reaction at 140 MeV/u.
- Published
- 2012
48. Low-spin excitations in 146Sm
- Author
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D. M. Filipescu, S. Pascu, N. Marginean, M. Elvers, L. Stroe, K. O. Zell, D. Ghiţă, Gh. Căta-Danil, A. Negreţ, C. Frießner, T. Glodariu, T. Sava, N. V. Zamfir, D. Bucurescu, J. Endres, P. von Brentano, C. Kuppersbusch, Andreas Zilges, C. Mihai, D. Deleanu, R. Mărginean, and V. Werner
- Subjects
Physics ,Nuclear and High Energy Physics ,Series (mathematics) ,Nuclear Theory ,Hadron ,Shell (structure) ,medicine.anatomical_structure ,medicine ,Nuclear fusion ,Neutron ,Atomic physics ,Spin (physics) ,Nucleus ,Multiplet - Abstract
The low-spin excitations of the nucleus 146Sm which is just two neutrons and two protons away from the N = 82 shell and Z = 64 subshell closures have been investigated by means of the 143Nd (α, n) and 144Nd (α, 2n) fusion-evaporation reactions. We established 47 hitherto unknown energy levels up to 4.7MeV and 75 new transitions. In addition, 7 spin assignments were possible from the γ-γ angular correlation analysis. The structure of the possible candidates for a 2+ ⊗ 3− quadrupole-octupole multiplet are first discussed in terms of the harmonic vibrational model. A comparison of these states with the corresponding ones in the neighboring N = 84 isotones is also presented. Finally, the structure of the 146Sm nucleus is interpreted in terms of the IBA-spdf model. It is shown that the model is able to reproduce the experimental relative transition strengths of the 2+ ⊗ 3− quadrupole-octupole multiplet and also a series of collective properties such as the proposed double-octupole excitations.
- Published
- 2012
49. Gamma-ray fast-timing coincidence measurements from the O-18+O-18 fusion-evaporation reaction using a mixed LaBr3-HPGe array
- Author
-
C. Mihai, D. Ghiţă, N. Alkhomashi, T. Sava, U. Garg, Mohammad Nakhostin, D. M. Filipescu, Alison Bruce, R. Marginean, T. Alharbi, S. S. Ghugre, S. Pascu, R. Chakrabarti, A. K. Sinha, A. Negret, C. Rodríguez Triguero, N. V. Zamfir, G. Suliman, P. J. R. Mason, D. Bucurescu, D. Deleanu, Zs. Podolyák, A. Kusoglu, M. N. Erduran, P. H. Regan, M. Bostan, I. Căta-Danil, P. Detistov, T. Glodariu, M. Bowry, L. Stroe, P. C. Bender, Gh. Căta-Danil, and N. Marginean
- Subjects
Physics ,Lifetimes of excited nuclear states ,Scintillation ,Radiation ,Gamma ray ,Tantalum ,chemistry.chemical_element ,Germanium ,Coincidence ,Semiconductor detector ,chemistry ,Excited state ,Gamma spectroscopy ,EM nuclear transition rates ,Gamma-ray spectroscopy ,Atomic physics - Abstract
8th Topical Meeting on Industrial Radiation and Radioisotope Measurement Applications (IRRMA) -- JUN 24-JUL 01, 2011 -- Kansas City, MO WOS: 000306937800064 PubMed ID: 22154387 We report on a gamma-ray coincidence analysis using a mixed array of hyperpure germanium and cerium-doped lanthanum tri-bromide (LaBr3:Ce) scintillation detectors to study nuclear electromagnetic transition rates in the pico-to-nanosecond time regime in P-33,P-34 and S-33 following fusion-evaporation reactions between an O-18 beam and an isotopically enriched O-18 implanted tantalum target. Energies from decay gamma-rays associated with the reaction residues were measured in event-by-event coincidence mode, with the measured time difference information between the pairs of gamma-rays in each event also recorded using the ultra-fast coincidence timing technique. The experiment used the good full-energy peak resolution of the LaBr3:Ce detectors coupled with their excellent timing responses in order to determine the excited state lifetime associated with the lowest lying, cross-shell, I-pi = 4(-) "intruder" state previously reported in the N=19 isotone P-34. The extracted lifetime is consistent with a mainly single-particle M2 multipolarity associated with a f(7/2) -> d(5/2) single particle transition. (C) 2011 Elsevier Ltd. All rights reserved. Kansas State Univ (KSU), Coll Engn, KSU, Dept Mech & Nucl Engn, KSU, Radiat Measurement Applicat Lab, N Carolina Sate Univ, Ctr Engn Applicat Radiosotopes, Int Radiat Phys Soc (IRPS) Science and Technology Facilities Council [ST/J000051/1, ST/F006950/1, ST/G000751/1 NuSTAR, ST/G000751/1]
- Published
- 2012
50. [sup 7]Li-induced reactions for fast-timing with LaBr[sub 3]:Ce detectors
- Author
-
S. Toma, I. Căta-Danil, G. Ilie, P. A. Söderström, D. M. Filipescu, R. Lica, V. Werner, N. Cooper, Ioana Gheorghe, M. Bunce, D. Ivanova, T. Alexander, E. Wilson, Paul Stevenson, A. Negret, N. V. Zamfir, R. T. Wood, M. Zhekova, Thamer Alharbi, Alejandro Algora, W. Gelletly, S. Lalkovski, P. H. Regan, N. Marginean, R. Britton, S. Kisyov, T. Sava, K. Mulholland, Alison Bruce, J. F. Smith, R. Mărginean, D. Deleanu, C. R. Nita, Stephen Rice, C. Mihai, C. Townsley, D. Delion, L. Stroe, P. J. R. Mason, Sean Liddick, Zs. Podolyák, D. Bucurescu, T. Glodariu, M. Bowry, Oliver J. Roberts, G. Cata-Danil, and D. Ghiţă
- Subjects
Nuclear physics ,chemistry ,Yrast ,Detector ,chemistry.chemical_element ,Lanthanum bromide ,Germanium ,Semiconductor detector - Abstract
7Li induced-reactions have been used with a 186W target to populate nuclei around A∼180-190 at the National Institute of Physics and Nuclear Engineering in Bucharest, Romania. An array of high-purity germanium (HPGe) and cerium-doped lanthanum bromide (LaBr3:Ce) detectors have been used to measure sub-nanosecond half-lives with fast-timing techniques. The yrast 2+ state in 190Os was measured to be t1/2 = 375(20)ps, in excellent agreement with the literature value. The previously unreported half-life of the 564-keV state in 189Ir has also been measured and a value of t1/2 = 540(100)ps ps obtained.
- Published
- 2012
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