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Journal articles on the topic 'Nuclear size (Physics)'

Author: Grafiati

Published: 4 June 2021

Last updated: 30 January 2023

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1

Bonatsos, D., and C. Dascaloyannis. "Quantum algebraic symmetries in nuclear physics." HNPS Proceedings 3 (December 5, 2019): 175. http://dx.doi.org/10.12681/hnps.2384.

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The pairing correlations in a single-j nuclear shell are considered. It is proven that a simple boson mapping in terms of q-defonned bosons exists, which reproduces correctly both the commutation relations and the energy up to first order corrections, the parameter q being connected to the size of the shell. An exact solution in terms of a generalized deformed oscillator is also found

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2

Almoukhalalati, Adel, Avijit Shee, and Trond Saue. "Nuclear size effects in vibrational spectra." Physical Chemistry Chemical Physics 18, no. 22 (2016): 15406–17. http://dx.doi.org/10.1039/c6cp01913g.

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3

Campi, Xavler. "Finite size scaling in nuclear fragmentation." Nuclear Physics A 495, no. 1-2 (April 1989): 259–66. http://dx.doi.org/10.1016/0375-9474(89)90324-2.

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4

Wolynec, E., V. A. Serrao, and M. N. Martins. "Nuclear size effects in virtual photon spectra." Journal of Physics G: Nuclear Physics 13, no. 4 (April 1987): 515–26. http://dx.doi.org/10.1088/0305-4616/13/4/015.

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5

Chen, Jianming, Liyuan Zhang, and Ren-yuan Zhu. "Large size LSO and LYSO crystal scintillators for future high-energy physics and nuclear physics experiments." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 572, no. 1 (March 2007): 218–24. http://dx.doi.org/10.1016/j.nima.2006.10.213.

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6

Bespalov, V. I. "Large-Size Monosectorial Crystal Elements for Powerful Laser Systems." Journal of Nonlinear Optical Physics & Materials 06, no. 04 (December 1997): 467–72. http://dx.doi.org/10.1142/s0218863597000344.

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The potentialities of fabricating large-size monosectorial crystals for powerful laser systems are discussed. Two types of technologies used for high-rate growth of profiled crystals and some results attained in crystal growth in the Institute of Applied Physics of the Russian Academy of Science are described briefly. It is concluded that the growth technique developed may be used for producing large-size optical elements (about 400 × 400 mm2) for laser systems intended for nuclear fusion experiments.

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7

Rajasekaran, M., and N. Meenakumari. "Finite size nucleonic effects in the nuclear medium." Pramana 39, no. 5 (November 1992): 559–63. http://dx.doi.org/10.1007/bf02847344.

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8

Ogloblin, A. A., A. S. Demyanova, A. N. Danilov, T. L. Belyaeva, S. A. Goncharov, and W. Trzaska. "Nuclear states with anomalously large radius (size isomers)." Physics of Atomic Nuclei 79, no. 4 (July 2016): 514–24. http://dx.doi.org/10.1134/s1063778816040177.

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9

Wei, Ye. "γ probe of nuclear dissipation." International Journal of Modern Physics E 23, no. 06 (June 2014): 1460003. http://dx.doi.org/10.1142/s0218301314600039.

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The Langevin model is applied to investigate the roles of excitation energy and system size in the evolution of post-saddle giant dipole resonance (GDR) γ-ray multiplicity (Mγ) with post-saddle friction strength (β). It is demonstrated that Mγ is more sensitive to β at high energy. Furthermore, it is shown that the dependence of γ emission on friction is sensitive to the size of fissioning nuclei, and a large system size significantly increases the sensitivity. Our findings indicate that in experiments, to tightly constrain post-saddle dissipation through the γ probe, it is optimal to produce heavy fissioning systems with high energy.

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10

Renner, O., L. Juha, J. Krasa, E. Krousky, M. Pfeifer, A. Velyhan, C. Granja, et al. "Low-energy nuclear transitions in subrelativistic laser-generated plasmas." Laser and Particle Beams 26, no. 2 (June 2008): 249–57. http://dx.doi.org/10.1017/s0263034608000293.

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AbstractThe aim of the reported research is to contribute to investigation of new processes and methods interlinking nuclear and laser-plasma physics. With respect to requirements of nuclear experiments at medium-size high-power lasers, the selection of proper candidates for studying the excitation and decay of low-lying nuclear states is reviewed. An experimental approach to the identification of low-energy nuclear transitions is discussed, simple estimates of the 181Ta excitation yield in the laser-generated plasma provide a theoretical basis for planning future work. First tests and results of the experiments at the laser facility PALS are presented.

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11

Lee, S. J., and A. Z. Mekjian. "Neutron skin size dependence of the nuclear symmetry energy." Journal of the Korean Physical Society 62, no. 11 (June 2013): 1600–1609. http://dx.doi.org/10.3938/jkps.62.1600.

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12

Özarslan, Evren, Noam Shemesh, Cheng Guan Koay, Yoram Cohen, and Peter J. Basser. "Nuclear magnetic resonance characterization of general compartment size distributions." New Journal of Physics 13, no. 1 (January 28, 2011): 015010. http://dx.doi.org/10.1088/1367-2630/13/1/015010.

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13

Yuming, Zheng, Osamu Miyamura, and Kenji Kumagai. "Study of Pion-Source Size in Relativistic Nuclear Collisions." Communications in Theoretical Physics 29, no. 2 (March 15, 1998): 257–64. http://dx.doi.org/10.1088/0253-6102/29/2/257.

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14

Aguilar-Saavedra, J. A., F. J. Botella, G. C. Branco, and M. Nebot. "The size of and physics beyond the Standard Model." Nuclear Physics B 706, no. 1-2 (January 2005): 204–20. http://dx.doi.org/10.1016/j.nuclphysb.2004.11.024.

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15

YEN, G. D., and H. G. MILLER. "NUCLEAR LEVEL DENSITIES CORRECTED FOR FINITE SIZE EFFECTS." Modern Physics Letters A 07, no. 17 (June 7, 1992): 1503–7. http://dx.doi.org/10.1142/s0217732392001178.

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Finite size corrections in the calculation of nuclear level densities are considered within the framework of a Fermi gas model. A simple geometrical correction to the single particle density of states leads to an increase in the Fermi energy which drastically reduces the many body density of states. For light nuclei such as 24Mg, the nuclear level density at T≡3 MeVis reduced by roughly an order of magnitude when finite size effects are taken into account and the reduction is more pronounced in heavier systems such as 208Pb.

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16

Hegedűs, Á., F. Ravanini, and J. Suzuki. "Exact finite size spectrum in super sine-Gordon model." Nuclear Physics B 763, no. 3 (February 2007): 330–53. http://dx.doi.org/10.1016/j.nuclphysb.2006.11.006.

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17

Nägeli, Christoph, and Roland Horisberger. "Impact of pixel size and shape on physics analyses." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 731 (December 2013): 194–97. http://dx.doi.org/10.1016/j.nima.2013.05.021.

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18

Xinhua, Yang, and Li Heshen. "EMC effect and the nucleon size in the nuclear environment." Chinese Physics Letters 3, no. 1 (January 1986): 37–40. http://dx.doi.org/10.1088/0256-307x/3/1/010.

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19

Jianming Chen, Liyuan Zhang, and Ren-Yuan Zhu. "Large size LYSO crystals for future high energy physics experiments." IEEE Transactions on Nuclear Science 52, no. 6 (December 2005): 3133–40. http://dx.doi.org/10.1109/tns.2005.862923.

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20

Helgesson, Johan, Roberta Ghetti, Luciano G. Moretto, Dimitry E. Breus, James B. Elliott, Larry W. Phair, and Gordon J. Wozniak. "Finite size scalings and the nuclear liquid-gas phase transition." Nuclear Physics A 734 (April 2004): 549–52. http://dx.doi.org/10.1016/j.nuclphysa.2004.01.102.

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21

Bhattacharjee, B., and R. Talukdar. "System size effect on the critical behavior in nuclear multifragmentation." Nuclear Physics A 864, no. 1 (August 2011): 167–75. http://dx.doi.org/10.1016/j.nuclphysa.2011.06.019.

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22

Campi, X., and H. Krivine. "Critical behaviour, fluctuations and finite size scaling in nuclear multifragmentation." Nuclear Physics A 545, no. 1-2 (August 1992): 161–72. http://dx.doi.org/10.1016/0375-9474(92)90456-t.

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23

Feng, Wu, and Ye Wei. "System size effects on probing nuclear dissipation with neutrons." Chinese Physics C 34, no. 5 (May 2010): 551–54. http://dx.doi.org/10.1088/1674-1137/34/5/007.

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24

Nickel, Bernie. "Nuclear size effects on hydrogenic atom energies: a semi-analytic formulation." Journal of Physics B: Atomic, Molecular and Optical Physics 46, no. 1 (December 17, 2012): 015001. http://dx.doi.org/10.1088/0953-4075/46/1/015001.

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25

Aleksandrov, I. A., A. A. Shchepetnov, D. A. Glazov, and V. M. Shabaev. "Finite nuclear size corrections to the recoil effect in hydrogenlike ions." Journal of Physics B: Atomic, Molecular and Optical Physics 48, no. 14 (May 28, 2015): 144004. http://dx.doi.org/10.1088/0953-4075/48/14/144004.

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26

Knecht, Stefan, and Trond Saue. "Nuclear size effects in rotational spectra: A tale with a twist." Chemical Physics 401 (June 2012): 103–12. http://dx.doi.org/10.1016/j.chemphys.2011.10.030.

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27

Pérez, Margarita Garcı́a, Tamás G. Kovács, and Pierre van Baal. "Instanton size distribution." Physics Letters B 472, no. 3-4 (January 2000): 295–301. http://dx.doi.org/10.1016/s0370-2693(99)01451-3.

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28

SUHONEN, JOUNI. "NUCLEAR-STRUCTURE EFFECTS ON DOUBLE BETA DECAYS TO 0+ STATES IN 76Ge." International Journal of Modern Physics E 20, no. 02 (February 2011): 451–58. http://dx.doi.org/10.1142/s0218301311017843.

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Neutrinoless double beta (0νββ) decay of 76 Ge to the ground state and first excited 0+ state in 76 Se is discussed in terms of the associated nuclear matrix elements. The effects arizing from the size of the single-particle model space and the occupancies of the individual orbits are discussed in the framework of the (higher) quasiparticle random-phase approximation with effective, G -matrix-derived nuclear forces. It is found that the orbital occupancies play a role for the size of the nuclear matrix element. Contrary to the ground-state transition the transition to the first excited 0+ state does not depend sensitively on the size of the model space.

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29

Braun, F. N. "Thermodynamics of the prokaryote nuclear zone." International Journal of Astrobiology 7, no. 2 (April 2008): 183–85. http://dx.doi.org/10.1017/s1473550408004217.

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AbstractIn studying the functional and evolutionary significance of compartmentation in biology, it is instructive to consider its thermodynamic context as a conceptual centrepiece of entropy and phase transitions. Here we focus specifically on compartmentation at the intracellular level of microbial organellar cytology. Via a colloid-statistical argument, supplemented with order of magnitude estimates for the relevant physical quantities, we find that the DNA-containing nucleoid of prokaryotes presents a plausible nucleation site for phase-transitional behaviour, provided the genome exceeds some threshold size of the order of 10 Mbp. Large genome size seems capable in this respect of seeding compartmentation effects such as the nuclear envelope of Planctomycetes bacteria, which is widely regarded as a possible precursor to the nuclear envelope of eukaryotes.

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30

KIM, Y. E., M. RABINOWITZ, Y. K. BAE, G. S. CHULICK, and R. A. RICE. "CLUSTER–IMPACT NUCLEAR FUSION: SHOCK–WAVE STATISTICAL ANALYSIS." Modern Physics Letters B 05, no. 14n15 (June 1991): 941–59. http://dx.doi.org/10.1142/s0217984991001179.

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Cluster–impact nuclear fusion is analyzed via a shock–wave model. We show that shock waves can be generated by clusters. Energy loss mechanisms are considered, and the conditions when they are not negligible are determined. Our theoretical model indicates that shock–wave enhanced fusion temperatures are possible with molecular size clusters impacting upon hydrogen isotope targets, somewhat as envisioned by Winterberg and Harrison for macro–projectiles. Our theory explains and reproduces the yields from known target and cluster compositions, as a function of cluster size and energy. Predictions are made, and new tests proposed. We show that contaminants are an unlikely artifact in the experimental data.

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31

Reisdorf, W., F. Rami, B. de Schauenburg, Y. Leifels, J. P. Alard, A. Andronic, V. Barret, et al. "Droplet formation in expanding nuclear matter: a system-size dependent study." Physics Letters B 595, no. 1-4 (August 2004): 118–26. http://dx.doi.org/10.1016/j.physletb.2004.05.031.

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32

Vergados, J. D., H. Ejiri, and F. Šimkovic. "Neutrinoless double beta decay and neutrino mass." International Journal of Modern Physics E 25, no. 11 (November 2016): 1630007. http://dx.doi.org/10.1142/s0218301316300071.

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The observation of neutrinoless double beta decay (DBD) will have important consequences. First it will signal that lepton number is not conserved and the neutrinos are Majorana particles. Second, it represents our best hope for determining the absolute neutrino mass scale at the level of a few tens of meV. To achieve the last goal, however, certain hurdles have to be overcome involving particle, nuclear and experimental physics. Particle physics is important since it provides the mechanisms for neutrinoless DBD. In this review, we emphasize the light neutrino mass mechanism. Nuclear physics is important for extracting the useful information from the data. One must accurately evaluate the relevant nuclear matrix elements (NMEs), a formidable task. To this end, we review the recently developed sophisticated nuclear structure approaches, employing different methods and techniques of calculation. We also examine the question of quenching of the axial vector coupling constant, which may have important consequences on the size of the NMEs. From an experimental point of view it is challenging, since the life times are extremely long and one has to fight against formidable backgrounds. One needs large isotopically enriched sources and detectors with good energy resolution and very low background.

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33

Vasileiou, Polytimos, and Theo J. Mertzimekis. "Extending the UoA Nuclear Physics Laboratory capabilities with low-γ and α spectrometers." HNPS Proceedings 26 (April 1, 2019): 259. http://dx.doi.org/10.12681/hnps.1835.

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In this project the steps taken toward the characterization, calibration and testing of two spectroscopy stations are presented. The first one is suitable for alpha spectroscopy, consisting of a large-window silicon surface barrier detector (SSB), a goniometric arm and a movable multiple source-holder inside a dark vacuum chamber. The second station contains two small-size, thin-window NaI(Tl) scintillators, and it is suitable for low-γ ray spectroscopy.

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34

FAGHIHI, F., and M. R. ESKANDARI. "NUCLEAR FUSION RATE STUDY OF A MUONIC MOLECULE VIA NUCLEAR THRESHOLD RESONANCES." International Journal of Modern Physics E 14, no. 08 (November 2005): 1213–21. http://dx.doi.org/10.1142/s0218301305003818.

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This work follows our previous calculations of the ground state binding energy, size, and the effective nuclear charge of the muonic T3 molecule, using the Born–Oppenheimer adiabatic approximation. In our past articles, we showed that the system possesses two minimum positions, the first one at the muonic distance and the second at the atomic distance. Also, the symmetric planner vibrational model assumed between the two minima and the approximated potential were calculated. Following from the previous studies, we now calculate the fusion rate of the T3 muonic molecule according to the overlap integral of the resonance nuclear compound nucleus and the molecular wave functions.

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35

Shabaev, V. M. "Finite nuclear size corrections to the energy levels of the multicharged ions." Journal of Physics B: Atomic, Molecular and Optical Physics 26, no. 6 (March 28, 1993): 1103–8. http://dx.doi.org/10.1088/0953-4075/26/6/011.

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36

Yerokhin, V. A., C. H. Keitel, and Z. Harman. "Nuclear-size self-energy and vacuum-polarization corrections to the bound-electrongfactor." Journal of Physics B: Atomic, Molecular and Optical Physics 46, no. 24 (November 27, 2013): 245002. http://dx.doi.org/10.1088/0953-4075/46/24/245002.

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37

James, J., and P. G. H. Sandars. "A parametric approach to nuclear size and shape in atomic parity nonconservation." Journal of Physics B: Atomic, Molecular and Optical Physics 32, no. 14 (July 20, 1999): 3295–307. http://dx.doi.org/10.1088/0953-4075/32/14/301.

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38

Niţescu, Ovidiu, Rastislav Dvornický, Sabin Stoica, and Fedor Šimkovic. "Angular Distributions of Emitted Electrons in the Two-Neutrino ββ Decay." Universe 7, no. 5 (May 14, 2021): 147. http://dx.doi.org/10.3390/universe7050147.

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The two-neutrino double-beta decay (2νββ-decay) process is attracting more and more attention of the physics community due to its potential to explain nuclear structure aspects of involved atomic nuclei and to constrain new (beyond the Standard model) physics scenarios. Topics of interest are energy and angular distributions of the emitted electrons, which might allow the deduction of valuable information about fundamental properties and interactions of neutrinos once a new generation of the double-beta decay experiments will be realized. These tasks require an improved theoretical description of the 2νββ-decay differential decay rates, which is presented. The dependence of the denominators in nuclear matrix elements on lepton energies is taken into account via the Taylor expansion. Both the Fermi and Gamow-Teller matrix elements are considered. For nuclei of experimental interest, relevant phase-space factors are calculated by using exact Dirac wave functions with finite nuclear size and electron screening. The uncertainty of the angular correlation factor on nuclear structure parameters is discussed. It is emphasized that the effective axial-vector coupling constant gAeff can be determined more reliably by accurately measuring the angular correlation factor.

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39

Vaca Chávez, Fabián, and Monika Schönhoff. "Pore size distributions in polyelectrolyte multilayers determined by nuclear magnetic resonance cryoporometry." Journal of Chemical Physics 126, no. 10 (March 14, 2007): 104705. http://dx.doi.org/10.1063/1.2565841.

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40

Quist, Per‐Ola, Bertil Halle, and István Furó. "Micelle size and order in lyotropic nematic phases from nuclear spin relaxation." Journal of Chemical Physics 96, no. 5 (March 1992): 3875–91. http://dx.doi.org/10.1063/1.461892.

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41

Panich, A. M., N. A. Sergeev, A. I. Shames, V. Yu Osipov, J.-P. Boudou, and S. D. Goren. "Size dependence of13C nuclear spin-lattice relaxation in micro- and nanodiamonds." Journal of Physics: Condensed Matter 27, no. 7 (February 3, 2015): 072203. http://dx.doi.org/10.1088/0953-8984/27/7/072203.

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42

Bożek, P., M. Płoszajczak, and A. Tucholski. "Finite size effects in the intermittency analysis of the fragment-size correlations." Nuclear Physics A 539, no. 4 (April 1992): 693–712. http://dx.doi.org/10.1016/0375-9474(92)90133-5.

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43

Reed, B. Cameron. "Estimating the size of Fermi’s CP-1 nuclear pile: a classroom approach." European Journal of Physics 42, no. 5 (July 15, 2021): 055801. http://dx.doi.org/10.1088/1361-6404/ac0e41.

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44

Chen, Jianming, Rihua Mao, Liyuan Zhang, and Ren-Yuan Zhu. "Large Size LSO and LYSO Crystals for Future High Energy Physics Experiments." IEEE Transactions on Nuclear Science 54, no. 3 (June 2007): 718–24. http://dx.doi.org/10.1109/tns.2007.897823.

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45

Hatefi Hesari, Shahram, Mohammad Aminul Haque, and Nicole McFarlane. "A Comprehensive Survey of Readout Strategies for SiPMs Used in Nuclear Imaging Systems." Photonics 8, no. 7 (July 7, 2021): 266. http://dx.doi.org/10.3390/photonics8070266.

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Silicon photomultipliers (SiPMs) offer advantages such as lower relative cost, smaller size, and lower operating voltages compared to photomultiplier tubes. A SiPM’s readout circuit topology can significantly affect the characteristics of an imaging array. In nuclear imaging and detection, energy, timing, and position are the primary characteristics of interest. Nuclear imaging has applications in the medical, astronomy, and high energy physics fields, making SiPMs an active research area. This work is focused on the circuit topologies required for nuclear imaging. We surveyed the readout strategies including the front end preamplification topology choices of transimpedance amplifier, charge amplifier, and voltage amplifier. In addition, a review of circuit topologies suitable for energy, timing, and position information extraction was performed along with a summary of performance limitations and current challenges.

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46

Breese, M. B. H., L. T. Romano, C. J. Salter, G. W. Grime, and F. Watt. "Determination of size and distribution of second phases using nuclear microscopy." Journal of Materials Research 7, no. 9 (September 1992): 2373–78. http://dx.doi.org/10.1557/jmr.1992.2373.

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Nuclear microscopy combines a range of MeV light ion beam analytical techniques such as Proton Induced X-ray Emission (PIXE), Rutherford Backscattering Spectrometry (RBS), and Scanning Transmission Ion Microscopy (STIM). One of the main advantages of using MeV light ion beams for materials characterization is the large analytical volume due to their high penetration depth. This paper shows how nuclear microscopy is used to determine the size and distribution of Pb precipitates in a 40 μm thick alloy sample with a nominal composition of Al–5 wt.% Pb.

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47

Katiyar, Aditya, V. J. Tocco, Yuan Li, Varun Aggarwal, Andrew C. Tamashunas, Richard B. Dickinson, and Tanmay P. Lele. "Nuclear size changes caused by local motion of cell boundaries unfold the nuclear lamina and dilate chromatin and intranuclear bodies." Soft Matter 15, no. 45 (2019): 9310–17. http://dx.doi.org/10.1039/c9sm01666j.

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48

Ahn, Changrim, and Rafael I. Nepomechie. "Finite size effects in the XXZ and sine-Gordon models with two boundaries." Nuclear Physics B 676, no. 3 (January 2004): 637–58. http://dx.doi.org/10.1016/j.nuclphysb.2003.11.012.

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49

Caira, M., M. Cumo, and A. Naviglio. "The MARS nuclear reactor plant: A inherently safe, small/medium size multipurpose nuclear plant." Nuclear Engineering and Design 97, no. 2 (November 1986): 145–60. http://dx.doi.org/10.1016/0029-5493(86)90104-4.

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50

Dukelsky, J., F. Fernandez, and E. Moya de Guerra. "Nuclear medium effects on the size of the nucleon valence quark distribution." Journal of Physics G: Nuclear and Particle Physics 21, no. 3 (March 1, 1995): 317–30. http://dx.doi.org/10.1088/0954-3899/21/3/007.

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