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Journal articles on the topic 'Nuclear resonant scattering'

Author: Grafiati

Published: 11 March 2023

Last updated: 25 July 2025

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1

Soroka, V. I. "Elastic nuclear resonance backscattering spectrometry (broad resonances)." Nuclear Physics and Atomic Energy 2, no. 8 (2007): 147–54. https://doi.org/10.15407/jnpae2007.02.147.

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The possibilities of using of the elastic nuclear resonance backscattering of ions for the investigation of materials are analyzed. Broad resonances having the cross-section varying smoothly in large energy range are considered. Under this condition the simplicity of information extraction inherent in the Rutherford backscattering technique is retained. Concurrently, the detection sensitivity for low-mass impurities is improved. The elastic nuclear resonance scattering reaction is always accompanied by the Coulomb and potential scatterings. The above components of the elastic scattering are co

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2

de Oliveira Santos, Francois. "Resonant Elastic Scattering." EPJ Web of Conferences 184 (2018): 01006. http://dx.doi.org/10.1051/epjconf/201818401006.

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Elastic scattering of nuclei at energies typically below 10 MeV/nucleon can be used as a powerful method for studying nuclear spectroscopy. Resonances are observed in the excitation function, corresponding to unbound states in the compound nucleus. The analysis of the shape of these resonances can provide the excitation energy, the total width, the partial width, and the spin of the excited states.

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3

RÖHLSBERGER, RALF. "MAGNETISM AND LATTICE DYNAMICS OF NANOSCALE STRUCTURES STUDIED BY NUCLEAR RESONANT SCATTERING OF SYNCHROTRON RADIATION." International Journal of Nanoscience 04, no. 05n06 (2005): 975–86. http://dx.doi.org/10.1142/s0219581x05003942.

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Nuclear resonant scattering of synchrotron radiation is applied to investigate the magnetic structure and the lattice dynamics of nanoscale systems. The outstanding brilliance of modern synchrotron radiation sources allows for sensitivities to smallest amounts of material. Due to the isotopic sensitivity of the scattering process, ultrathin probe layers of Mössbauer isotopes can be used to map out the magnetic and vibrational structure of thin films with sub-nm spatial resolution. Elastic nuclear resonant scattering is applied to determine the magnetic spin structure of an exchange-coupled bil

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4

Tsutsui, Satoshi, Yasuhiro Kobayashi, Yoshitaka Yoda, Makoto Seto, Kentaro Indoh, and Hideya Onodera. "149Sm nuclear resonant scattering of SmB2C2." Journal of Magnetism and Magnetic Materials 272-276 (May 2004): 199–200. http://dx.doi.org/10.1016/j.jmmm.2003.11.077.

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5

Smirnov, G. V. "Nuclear resonant scattering of synchrotron radiation." Hyperfine Interactions 97-98, no. 1 (1996): 551–88. http://dx.doi.org/10.1007/bf02150198.

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6

Deák, L., L. Bottyán, R. Callens, et al. "Stroboscopic detection of nuclear resonance in an arbitrary scattering channel." Journal of Synchrotron Radiation 22, no. 2 (2015): 385–92. http://dx.doi.org/10.1107/s1600577514026344.

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The theory of heterodyne/stroboscopic detection of nuclear resonance scattering is developed, starting from the total scattering matrix as a product of the matrix of the reference sample and the sample under study. This general approach holds for all dynamical scattering channels. In the forward channel, which has been discussed in detail in the literature, the electronic scattering manifests itself only in an energy-independent diminution of the scattered intensity. In all other channels, complex resonance line shapes of the heterodyne/stroboscopic spectra are encountered, as a result of the

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7

Marx-Glowna, Berit, Ingo Uschmann, Kai S. Schulze, et al. "Advanced X-ray polarimeter design for nuclear resonant scattering." Journal of Synchrotron Radiation 28, no. 1 (2021): 120–24. http://dx.doi.org/10.1107/s1600577520015295.

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This work presents the improvements in the design and testing of polarimeters based on channel-cut crystals for nuclear resonant scattering experiments at the 14.4 keV resonance of 57Fe. By using four asymmetric reflections at asymmetry angles of α1 = −28°, α2 = 28°, α3 = −28° and α4 = 28°, the degree of polarization purity could be improved to 2.2 × 10−9. For users, an advanced polarimeter without beam offset is now available at beamline P01 of the storage ring PETRA III.

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8

Seto, Makoto. "Condensed Matter Physics Using Nuclear Resonant Scattering." Journal of the Physical Society of Japan 82, no. 2 (2013): 021016. http://dx.doi.org/10.7566/jpsj.82.021016.

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9

Tsutsui, Satoshi, Takumi Hasegawa, Yuichi Takasu, et al. "149Sm nuclear resonant inelastic scattering of SmB6." Journal of Physics: Conference Series 176 (June 1, 2009): 012033. http://dx.doi.org/10.1088/1742-6596/176/1/012033.

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10

Kobayashi, Yasuhiro, Saburo Nasu, Takashi Nakamichi, Masayuki Sato, Makoto Seto, and Yoshitaka Yoda. "Nuclear Resonant Scattering of Ferromagnetic Amorphous Ribbon." Japanese Journal of Applied Physics 38, S1 (1999): 412. http://dx.doi.org/10.7567/jjaps.38s1.412.

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11

Yoda, Y., M. Yabashi, K. Izumi, et al. "Nuclear resonant scattering beamline at SPring-8." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 467-468 (July 2001): 715–18. http://dx.doi.org/10.1016/s0168-9002(01)00474-0.

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12

Asthalter, T., I. Sergueev, and U. van Bürck. "Molecular rotations studied by nuclear resonant scattering." Journal of Physics and Chemistry of Solids 66, no. 12 (2005): 2271–76. http://dx.doi.org/10.1016/j.jpcs.2005.09.076.

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13

Mitsui, Takaya, Ryo Masuda, Shinji Kitao, and Makoto Seto. "Nuclear Resonant Scattering of Synchrotron Radiation by158Gd." Journal of the Physical Society of Japan 74, no. 11 (2005): 3122–23. http://dx.doi.org/10.1143/jpsj.74.3122.

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14

Xu, Wei, and Ercan Alp. "First Nuclear Resonant Scattering Workshop in China." Synchrotron Radiation News 30, no. 4 (2017): 51–52. http://dx.doi.org/10.1080/08940886.2017.1316136.

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15

Jakuba�a-Amundsen, D. H. "Radiative electron capture accompanying resonant nuclear scattering." Zeitschrift f�r Physik A Atoms and Nuclei 322, no. 2 (1985): 191–97. http://dx.doi.org/10.1007/bf01411881.

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16

Kitao, Shinji, Takaya Mitsui, and Makoto Seto. "Nuclear Resonant Scattering of Synchrotron Radiation by121Sb and149Sm." Journal of the Physical Society of Japan 69, no. 3 (2000): 683–85. http://dx.doi.org/10.1143/jpsj.69.683.

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17

Rosenberg, L. "Effect of atomic electrons on resonant nuclear scattering." Journal of Physics B: Atomic and Molecular Physics 18, no. 5 (1985): 887–98. http://dx.doi.org/10.1088/0022-3700/18/5/009.

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18

Amundsen, P. A., and K. Aashamar. "Coincident inner-shell ionisation and nuclear resonant scattering." Journal of Physics B: Atomic and Molecular Physics 19, no. 11 (1986): 1657–73. http://dx.doi.org/10.1088/0022-3700/19/11/020.

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19

Kikuta, S. "Studies of nuclear resonant scattering at TRISTAN-AR." Hyperfine Interactions 90, no. 1 (1994): 335–49. http://dx.doi.org/10.1007/bf02069137.

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20

Sturhahn, W., C. L'abbé, and T. S. Toellner. "Exo-interferometric phase determination in nuclear resonant scattering." Europhysics Letters (EPL) 66, no. 4 (2004): 506–12. http://dx.doi.org/10.1209/epl/i2003-10235-7.

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21

YODA, Yoshitaka. "Research using Nuclear Resonant Scattering by Synchrotron Radiation―Synchrotron Mössbauer Spectroscopy and Nuclear Resonant Vibrational Spectroscopy―." RADIOISOTOPES 63, no. 6 (2014): 317–29. http://dx.doi.org/10.3769/radioisotopes.63.317.

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22

Caciuffo, Roberto, and Gerard H. Lander. "X-ray synchrotron radiation studies of actinide materials." Journal of Synchrotron Radiation 28, no. 6 (2021): 1692–708. http://dx.doi.org/10.1107/s1600577521009413.

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By reviewing a selection of X-ray diffraction (XRD), resonant X-ray scattering (RXS), X-ray magnetic circular dichroism (XMCD), resonant and non-resonant inelastic scattering (RIXS, NIXS), and dispersive inelastic scattering (IXS) experiments, the potential of synchrotron radiation techniques in studying lattice and electronic structure, hybridization effects, multipolar order and lattice dynamics in actinide materials is demonstrated.

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23

Stuhrmann, Heinrich B. "Small-angle scattering and its interplay with crystallography, contrast variation in SAXS and SANS." Acta Crystallographica Section A Foundations of Crystallography 64, no. 1 (2007): 181–91. http://dx.doi.org/10.1107/s0108767307046569.

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Methods of contrast variation are tools that are essential in macromolecular structure research. Anomalous dispersion of X-ray diffraction is widely used in protein crystallography. Recent attempts to extend this method to native resonant labels like sulfur and phosphorus are promising. Substitution of hydrogen isotopes is central to biological applications of neutron scattering. Proton spin polarization considerably enhances an existing contrast prepared by isotopic substitution. Concepts and methods of nuclear magnetic resonance (NMR) become an important ingredient in neutron scattering from

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24

SETO, Makoto. "Study of Condensed Matter by Using Nuclear Resonant Scattering." Nihon Kessho Gakkaishi 43, no. 6 (2001): 405–12. http://dx.doi.org/10.5940/jcrsj.43.405.

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25

Zhao, J. Y., T. S. Toellner, M. Y. Hu, et al. "High-energy-resolution monochromator for 83Kr nuclear resonant scattering." Review of Scientific Instruments 73, no. 3 (2002): 1608–10. http://dx.doi.org/10.1063/1.1445822.

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26

Toellner, T. S., M. Y. Hu, W. Sturhahn, K. Quast, and E. E. Alp. "Inelastic nuclear resonant scattering with sub-meV energy resolution." Applied Physics Letters 71, no. 15 (1997): 2112–14. http://dx.doi.org/10.1063/1.120448.

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27

Kitao, Shinji, Takaya Mitsui, Taikan Harami, Yoshitaka Yoda, and Makoto Seto. "Inelastic Nuclear Resonant Scattering of FeCl3-Graphite Intercalation Compounds." Japanese Journal of Applied Physics 38, S1 (1999): 535. http://dx.doi.org/10.7567/jjaps.38s1.535.

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28

Masuda, Ryo, Satoshi Higashitaniguchi, Shinji Kitao, et al. "Nuclear Resonant Scattering of Synchrotron Radiation by Yb Nuclides." Journal of the Physical Society of Japan 75, no. 9 (2006): 094716. http://dx.doi.org/10.1143/jpsj.75.094716.

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29

Baron, A. Q. R., A. I. Chumakov, S. L. Ruby, et al. "Nuclear resonant scattering of synchrotron radiation by gaseous krypton." Physical Review B 51, no. 22 (1995): 16384–87. http://dx.doi.org/10.1103/physrevb.51.16384.

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30

Alp, E. E., T. M. Mooney, T. Toellner, et al. "Time resolved nuclear resonant scattering fromSn119nuclei using synchrotron radiation." Physical Review Letters 70, no. 21 (1993): 3351–54. http://dx.doi.org/10.1103/physrevlett.70.3351.

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31

Chumakov, A. I., J. Metge, A. Q. R. Baron, et al. "Radiation trapping in nuclear resonant scattering of x rays." Physical Review B 56, no. 14 (1997): R8455—R8458. http://dx.doi.org/10.1103/physrevb.56.r8455.

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32

Arthur, J. "Resonant nuclear X-ray scattering as a crystallographic tool." Acta Crystallographica Section A Foundations of Crystallography 49, s1 (1993): c18. http://dx.doi.org/10.1107/s0108767378099493.

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33

Alp, E. E., T. M. Mooney, T. Toellner, and W. Sturhahn. "Nuclear resonant scattering beamline at the Advanced Photon Source." Hyperfine Interactions 90, no. 1 (1994): 323–34. http://dx.doi.org/10.1007/bf02069136.

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34

Yoda, Y., X. W. Zhang, M. Seto, S. Kitao, and S. Kikuta. "High-resolution monochromator for nuclear resonant scattering by151Eu and149Sm." Acta Crystallographica Section A Foundations of Crystallography 58, s1 (2002): c166. http://dx.doi.org/10.1107/s0108767302091675.

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35

Zhao, Jiyong, Wolfgang Sturhahn, Jung-fu Lin, Guoyin Shen, Ercan E. Alp, and Ho-kwang Mao. "Nuclear resonant scattering at high pressure and high temperature." High Pressure Research 24, no. 4 (2004): 447–57. http://dx.doi.org/10.1080/08957950412331331727.

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36

Coussement, R., S. Cottenier, and C. L’abbé. "Time-integrated nuclear resonant forward scattering of synchrotron radiation." Physical Review B 54, no. 22 (1996): 16003–9. http://dx.doi.org/10.1103/physrevb.54.16003.

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37

Alp, E. E., W. Sturhahn, and T. S. Toellner. "Lattice dynamics and inelastic nuclear resonant x-ray scattering." Journal of Physics: Condensed Matter 13, no. 34 (2001): 7645–58. http://dx.doi.org/10.1088/0953-8984/13/34/311.

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38

Kikuta, S., Y. Yoda, Y. Hasegawa, et al. "Nuclear Resonant scattering experiments with synchrotron radiation at KEK." Hyperfine Interactions 71, no. 1-4 (1992): 1491–94. http://dx.doi.org/10.1007/bf02397365.

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39

Falgel, G. "Determination of partial structure factors using resonant nuclear scattering." Hyperfine Interactions 61, no. 1-4 (1990): 1355–58. http://dx.doi.org/10.1007/bf02407624.

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40

Deák, L., L. Bottyán, and D. L. Nagy. "Calculation of nuclear resonant scattering spectra of magnetic multilayers." Hyperfine Interactions 92, no. 1 (1994): 1083–88. http://dx.doi.org/10.1007/bf02065737.

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41

OLKHOVSKY, V. S., M. E. DOLINSKA, S. A. OMELCHENKO, and M. V. ROMANIUK. "NEW DEVELOPMENTS IN THE TUNNELING AND TIME ANALYSIS OF LOW-ENERGY NUCLEAR PROCESSES." International Journal of Modern Physics E 19, no. 05n06 (2010): 1212–19. http://dx.doi.org/10.1142/s0218301310015692.

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The new applications of the three-dimensional tunnelling and time analysis to low-energy nuclear processes are presented. The three-dimensional tunnelling is strictly quantum-mechanical and considers the internal multiple reflections. The time analysis of the nucleon-nucleons scattering near a resonance, distorted by the non-resonant background, does show the solution in the L -system of the paradox of the delay-advance in the C -system.

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42

Fraser, Paul, Ken Amos, Carlos Bertulani, et al. "A multichannel algebraic scattering approach to astrophysical reactions." EPJ Web of Conferences 292 (2024): 04005. http://dx.doi.org/10.1051/epjconf/202429204005.

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The investigation of many astrophysical processes is dependent upon an understanding of nuclear reaction rates. However, nuclear capture reactions of astrophysical interest occur at extremely low energies, taking place at the Gamow energy within the stellar environment. Hence, they are hard to study experimentally due to Coulomb repulsion. They may also involve compound resonances stemming from a delicate interplay of many quantum states in the colliding bodies. The multi-channel algebraic scattering (MCAS) method is one that addresses both of these challenges; it has a history of successfully

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43

Suzuki, D., T. Sumikama, M. Ogura, et al. "Resonant neutrino scattering: An impossible experiment?" Physics Letters B 687, no. 2-3 (2010): 144–48. http://dx.doi.org/10.1016/j.physletb.2010.03.024.

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44

Reinhardt, J., A. Scherdin, B. M�ller, and W. Greiner. "Resonant Bhabha scattering at MeV energies." Zeitschrift f�r Physik A Atomic Nuclei 327, no. 4 (1987): 367–81. http://dx.doi.org/10.1007/bf01289561.

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45

Li, Tang, and Xiaowei Zhang. "The Prime Beat Components Extraction Method for the Time Spectra Analysis of Nuclear Resonant Forward Scattering." Materials 12, no. 10 (2019): 1657. http://dx.doi.org/10.3390/ma12101657.

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Spectra of quantum beats (QBs) of nuclear resonant forward scattering contain the interference information of all allowed energy transitions of a nucleus, which makes it complicated to extract hyperfine structure directly. Here, we propose a new method, based upon the extraction of prime beat components, to understand QBs. In this method, the origin of major spectral lines in the Fourier Transformation of QBs is studied, and the energy levels of hyperfine structure are obtained directly from the QBs. We applied this method to the temperature dependent QBs of hematite. The Morin temperature and

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46

Dagan, Ron, Yaron Danon, and Alexander Konobeev. "Open issues on scattering kernels of compound nuclear reactors." EPJ Web of Conferences 322 (2025): 10005. https://doi.org/10.1051/epjconf/202532210005.

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Scattering kernel models, define the energy change and angular distribution of a scattered neutron. In the keV and fast energy ranges these are often determined by phenomenological concepts or using fits to measurements due to lack of microscopic details and/or complicated mathematical issues with some models. Some scattering kernels neglect the temperature dependency or the resonant structure of the nuclide. Moreover, most of the double differential solutions do not sum up mathematically to the integral scattering cross section itself and are in the best case artificially adapted. This study

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47

Suzuki, Carlos K., Xiao W. Zhang, Masami Ando, et al. "Synchrotron radiation time gate quartz device for nuclear resonant scattering." Review of Scientific Instruments 66, no. 2 (1995): 2235–37. http://dx.doi.org/10.1063/1.1145716.

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48

Hasegawa, Yuji, Yoshitaka Yoda, Koichi Izumi, et al. "Time-Delayed Interferometry with Nuclear Resonant Scattering of Synchrotron Radiation." Japanese Journal of Applied Physics 33, Part 2, No. 6A (1994): L772—L775. http://dx.doi.org/10.1143/jjap.33.l772.

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49

Troyan, I., A. Gavriliuk, R. Ruffer, et al. "Observation of superconductivity in hydrogen sulfide from nuclear resonant scattering." Science 351, no. 6279 (2016): 1303–6. http://dx.doi.org/10.1126/science.aac8176.

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50

Hoy, Gilbert R. "Quantum mechanical model for nuclear-resonant scattering of gamma radiation." Journal of Physics: Condensed Matter 9, no. 41 (1997): 8749–65. http://dx.doi.org/10.1088/0953-8984/9/41/019.

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