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1

Kubodera, K. "Neutrino-nucleus reaction cross sections." Nuclear Physics B - Proceedings Supplements 100, no. 1-3 (May 2001): 30–35. http://dx.doi.org/10.1016/s0920-5632(01)01403-7.

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2

Dietrich, F. S., and J. E. Escher. "Compound-nuclear reaction cross sections via surrogate reactions." Nuclear Physics A 787, no. 1-4 (May 2007): 237–42. http://dx.doi.org/10.1016/j.nuclphysa.2006.12.038.

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3

Luo, J., R. Liu, L. Jiang, Z. Liu, G. Sun, and S. Ge. "Cross-sections of 45Sc(n, 2n)44m,gSc reaction from the reaction threshold to 20 MeV." Radiochimica Acta 101, no. 10 (October 2013): 607–12. http://dx.doi.org/10.1524/ract.2013.2065.

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Summary Cross sections of 45Sc(n, 2n)44m,g Sc reactions and their isomeric cross section ratios σm/σg have been measured at three neutron energies between 13.5 and 14.8 MeV using the activation technique. The pure cross section of the groundstate was then obtained by utilizing the absolute cross section of the metastable state and analysis methods of residual nuclear decay. The monoenergetic neutron beam was produced via the 3H(d, n)4He reaction. The cross sections were also estimated with the TALYS-1.2 nuclear model code using different level density options, at neutron energies varying from the reaction threshold to 20 MeV. Results are also discussed and compared with some corresponding values found in the literature.
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4

DESCOUVEMONT, PIERRE. "CROSS SECTIONS FOR NUCLEAR ASTROPHYSICS." International Journal of Modern Physics E 17, no. 10 (November 2008): 2165–70. http://dx.doi.org/10.1142/s0218301308011288.

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General properties of low-energy cross sections and of reaction rates are presented. We describe different models used in nuclear astrophysics: microscopic models, the potential model, and the R-matrix method. Two important reactions, 7 Be ( p ,γ)8 B and 12 C (α,γ)16 O , are then briefly discussed.
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5

SHEN, PENGNIAN, HANTAO JING, and HUANQING CHIANG. "Λ-HYPERNUCLEUS PRODUCTION IN PROTON-INDUCED REACTION." International Journal of Modern Physics E 18, no. 02 (February 2009): 302–8. http://dx.doi.org/10.1142/s021830130901232x.

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The Λ-hypernucleus (LHN) production in the proton-induced reaction is studied in the distorted wave impulse approximation(DWIA). The cross sections for the LHN production in the reactions where the proton bombards the 6Li, 12C and 16O targets, respectively, are calculated. It is shown that the reaction cross sections are of the order of μb, and the distortion effects tend to reduce the cross sections by a factor of 3~10. For the sΛ–LHN production, the differential cross section is decreased with the increasing mass of the target nucleus. The pΛ–LHN production cross section is normally higher than that for the sΛ–LHN production. The double differential cross sections (DDXS) with respect to the momenta of the outgoing proton and kaon are also demonstrated. The missing mass spectra of the inclusive reaction p+A → p+K++X for the 6Li, 12C and 16O targets, an alternative way to study hypernuclear physics, are proposed. From these spectra, the masses of LHN can accurately be extracted. Moreover, the exotic LHN production in the same type of reaction is also studied . The same physical quantities are calculated. It is shown that the magnitude of the cross section is also in the order of μb. The halo effect of the core nucleus that locates at a place far away from the stable line would make the wave function broader, and consequently reduces the production cross section.
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6

Spyrou, A., H. W. Becker, A. Lagoyannis, S. Harissopulos, and C. Rolfs. "A 4π γ-summing method for cross-section measurements of capture reactions." HNPS Proceedings 15 (January 1, 2020): 111. http://dx.doi.org/10.12681/hnps.2627.

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Capture reaction cross sections at energies far below the Coulomb barrier are of major importance for the understanding of stellar nucleosynthesis. Since the cross sections of the majority of these reactions are very small, the use of high efficiency detectors is essential. In this work, a new method for capture reaction cross section measurements based on a large volume 4π NaI detector is presented.
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7

SAJJAD ATHAR, M., S. CHAUHAN, S. K. SINGH, and M. J. VICENTE VACAS. "NEUTRINO NUCLEUS CROSS-SECTIONS." International Journal of Modern Physics E 18, no. 07 (August 2009): 1469–81. http://dx.doi.org/10.1142/s0218301309013774.

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We present the results of our calculation which has been performed to study the nuclear effects in the quasielastic, inelastic and deep inelastic scattering of neutrinos(antineutrinos) from nuclear targets. These calculations are done in the local density approximation. We take into account the effect of Pauli blocking, Fermi motion, Coulomb effect, renormalization of weak transition strengths in the nuclear medium in the case of the quasielastic reaction. The inelastic reaction leading to production of pions is calculated in a Δ-dominance model taking into account the renormalization of Δ properties in the nuclear medium and the final state interaction effects of the outgoing pions with the residual nucleus. We discuss the nuclear effects in the [Formula: see text] structure function in the deep inelastic neutrino(antineutrino) reaction using a relativistic framework to describe the nucleon spectral function in the nucleus.
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8

Mintz, S. L., G. M. Gerstner, M. A. Barnett, and M. Pourkaviani. "The Neutrino Reaction in 3H." International Journal of Modern Physics E 07, no. 02 (April 1998): 275–85. http://dx.doi.org/10.1142/s0218301398000117.

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We calculate the cross sections for the reactions, νe+3 H → e-+3 He , and νμ+3 H → μ-+3 He from threshold to 1 GeV. We obtain typical contributions of the individual form factors as well as the interference terms to the cross sections. We find that the cross sections for these processes are extremely large for a number of reasons, making them worthy of consideration for possible experiments. We also obtain a typical differential cross section and note the presence of sharp minima for high neutrino energies.
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9

Ozawa, A. "Reaction cross-sections for carbon isotopes." Nuclear Physics A 738 (June 2004): 38–44. http://dx.doi.org/10.1016/j.nuclphysa.2004.04.009.

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10

Mukhamedzhanov, A. M., R. Yarmukhamedov, and Sh Yarmukhamedov. "Analytic continuation of reaction cross sections." Theoretical and Mathematical Physics 74, no. 2 (February 1988): 178–86. http://dx.doi.org/10.1007/bf01886490.

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11

Haque, M. M., M. T. Islam, M. A. Hafiz, R. U. Miah, and M. S. Uddin. "14.8 MeV Neutron Activation Cross Section Measurements for Ge Isotopes." Journal of Scientific Research 1, no. 2 (April 9, 2009): 173–81. http://dx.doi.org/10.3329/jsr.v1i2.1532.

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The cross sections of Ge isotopes were measured with the activation method at 14.8 MeV neutron energy. The quasi-monoenergetic neutron beams were produced via the 3H(d,n)4He reaction at the 150 kV J-25 neutron generator of INST, AERE. The characteristics γ-lines of the product nuclei were measured with a closed end coaxial 17.5 cm2 high purity germanium (HPGe) detector gamma ray spectroscopy. The cross sections were determined with reference to the known 27Al(n,α)24Na reaction. Cross section data are presented for 72Ge(n,p)72Ga, 74Ge(n,α)71mZn and 76Ge(n,2n)75m+gGe reactions. The cross section values obtained for the above reactions were 24.78±1.75 mb, 1.69±0.11 mb and 860±50 mb, respectively. The results obtained were compared with the values reported in literature as well as theoretical calculation performed by the statistical code SINCROS-II. The experimental data were found fairly in good agreement with the calculated and literature data. Keywords: Activation cross section; Neutron induced reaction; Gamma-ray spectroscopy; 14.8 MeV. © 2009 JSR Publications. ISSN: 2070-0237 (Print); 2070-0245 (Online). All rights reserved. DOI: 10.3329/jsr.v1i2.1532
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12

Moody, K. J., R. W. Lougheed, R. J. Dougan, E. K. Hulet, J. F. Wild, K. Summerer, R. L. Hahn, J. van Aarle, and G. R. Bethune. "Actinide cross sections from the reaction ofC13withEsg254." Physical Review C 41, no. 1 (January 1, 1990): 152–59. http://dx.doi.org/10.1103/physrevc.41.152.

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13

Han, Yinlu. "Theoretical Calculations ofn+232,234,236,238,240U Reaction Cross Sections." Nuclear Science and Engineering 158, no. 1 (January 2008): 78–87. http://dx.doi.org/10.13182/nse08-a2740.

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14

Simpson, E. C. "Nuclear reaction cross sections for hadron therapy." Journal of Physics: Conference Series 1662 (October 2020): 012003. http://dx.doi.org/10.1088/1742-6596/1662/1/012003.

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15

Wang, Jimin, Xi Tao, Xiaolong Huang, and Zhigang Ge. "The systematics of neutron reaction cross sections." EPJ Web of Conferences 239 (2020): 11003. http://dx.doi.org/10.1051/epjconf/202023911003.

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The parameterized theoretical formulae of excitation functions for (n, 2n) and (n, γ) reactions have been established, and for (n,tot), (n,non), (n,3n), (n,p), (n,d), (n,t), (n,3 He) and (n,α) have been recommended. According to these formulae, the SEF code have been developed for systematics calculation of these reactions. The calculated results with the systematics of the corresponding reactions of the discretional nucleus can be provided by the SEF code in the applied range quickly. At the same time, the comparison of calculated results with experimental and evaluated data can be given graphically.
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16

Akkoyun, S., T. Bayram, and S. O. Kara. "Photonuclear Reaction Cross Sections for Gallium Isotopes." Journal of Physics: Conference Series 590 (April 8, 2015): 012047. http://dx.doi.org/10.1088/1742-6596/590/1/012047.

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17

Adloff, J. C., V. S. Butsev, H. H. Cui, M. Debeauvais, F. Fernández, Y. H. Guo, S. Jokić, et al. "Total reaction cross sections at relativistic energies." International Journal of Radiation Applications and Instrumentation. Part D. Nuclear Tracks and Radiation Measurements 19, no. 1-4 (January 1991): 547–52. http://dx.doi.org/10.1016/1359-0189(91)90265-j.

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18

Fukugita, M., Y. Kohyama, and K. Kubodera. "Neutrino reaction cross sections on 12C target." Physics Letters B 212, no. 2 (September 1988): 139–44. http://dx.doi.org/10.1016/0370-2693(88)90513-8.

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19

Gomes, P. R. S., D. R. Mendes Junior, L. F. Canto, J. Lubian, and P. N. de Faria. "Reduction Methods for Total Reaction Cross Sections." Few-Body Systems 57, no. 3 (January 11, 2016): 205–16. http://dx.doi.org/10.1007/s00601-015-1042-4.

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20

Generalov, L. N., O. P. Vikhlyantsev, I. A. Karpov, A. V. Kuryakin, A. D. Tumkin, S. V. Fil’chagin, and D. A. Fedotov. "6, 7Li + d Reaction Cross Sections Measurements." Bulletin of the Russian Academy of Sciences: Physics 84, no. 12 (December 2020): 1511–17. http://dx.doi.org/10.3103/s1062873820120126.

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21

Yiğit, Mustafa. "A new empirical formula for cross-sections of (n,nα) reactions." International Journal of Modern Physics E 29, no. 08 (August 2020): 2050062. http://dx.doi.org/10.1142/s0218301320500627.

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Studies on the cross-sections of (n,n[Formula: see text]) reactions which are energetically possible, about 14 MeV neutrons are quite scarce. In this paper, the cross-sections of (n,n[Formula: see text] nuclear reactions at [Formula: see text]14–15 MeV are analyzed by using a new empirical formula based on the statistical theory. We show that neutron cross-sections are closely related to the [Formula: see text]-value of nuclear reaction, in particular for (n,n[Formula: see text]) channels. Results obtained with this empirical formula show good agreement with the available measured cross-section values. We hope that the estimations on the cross-sections using the present formalism may be helpful in future studies in this field.
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22

Carlson, R. F. "Proton-Nucleus Total Reaction Cross Sections and Total Cross Sections Up to 1 GeV." Atomic Data and Nuclear Data Tables 63, no. 1 (May 1996): 93–116. http://dx.doi.org/10.1006/adnd.1996.0010.

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23

Yiğit, M. "Analysis of the reaction Q-value effect using newly evaluated empirical formulas of (n,2n) cross-sections near 14.6MeV." International Journal of Modern Physics E 29, no. 02 (February 2020): 2050005. http://dx.doi.org/10.1142/s0218301320500056.

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Empirical formulas in determining the cross-sections play an important role at the energies of which there are no experimental data scattered about. The purpose of the present communication is to further improve the formulas of the cross-section of [Formula: see text] reactions at the energies near 14.6[Formula: see text]MeV. A systematics for the evaluation of these cross-sections is studied. We present the empirical formulas based on the statistical theory of nuclear reactions in connection with the compound nucleus. The new empirical formulas are found by using the experimental cross-sections as a function of the reaction [Formula: see text]-value. Thus, the new formulas provide the best description of the existing measured data compared with systematics suggested earlier by other authors.
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24

E. Escher, J., J. T. Burke, R. J. Casperson, R. O. Hughes, and N. D. Scielzo. "One-nucleon pickup reactions and compound-nuclear decays." EPJ Web of Conferences 178 (2018): 03002. http://dx.doi.org/10.1051/epjconf/201817803002.

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One-nucleon transfer reactions, long used as a tool to study the structure of nuclei, are potentially valuable for determining reaction cross sections indirectly. This is significant, as many reactions of interest to astrophysics and other applications involve short-lived isotopes and cannot be measured directly. We describe a procedure for obtaining constraints for calculations of neutron capture cross sections using observables from experiments with transfer reactions. As a first step toward demonstrating the method, we outline the theory developments used to properly describe the production of the compound nucleus 88Y* via the one-nucleon pickup reaction 89Y(p,d)88Y* and test the description with data from a recent experiment. We indicate how this development can be used to extract the unknown 87Y(n,γ) cross section from 89Y(p,dγ) data. The example illustrates a more generally applicable method for determining unknown cross sections via a combination of theory and transfer (or inelastic scattering) experiments.
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25

Kosmas, T. S., and E. Oset. "Inclusive neutrino-nucleus reaction cross sections at intermediate energies." HNPS Proceedings 5 (February 19, 2020): 29. http://dx.doi.org/10.12681/hnps.2892.

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Inclusive neutrino-nucleus reaction cross sections at intermediate energies (20 MeV < Ey < 500 MeV) are calculated throughout the periodic table for the most interesting nu­ clei from an experimental point of view. The method used had previously proved to be very accurate in calculating the induced reaction cross section for T=0 light nuclei (12C and 16O) and in the study of other similar processes like the ordinary muon capture. The electron-neutrino (ve) cross section weighted by the Michel distribution is also discussed in conjuction with the existing experimental results at LAMPF and ΚARMEN.
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26

Ma, Nanru, Chengjian Lin, Huiming Jia, Xinxing Xu, Feng Yang, Lei Yang, Lijie Sun, Dongxi Wang, Huanqiao Zhang, and Zuhua Liu. "Measurement of (n, f) and (n, xn) cross sections with surrogate reaction method." EPJ Web of Conferences 239 (2020): 01007. http://dx.doi.org/10.1051/epjconf/202023901007.

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Surrogate reaction method is an important approach to overcome the difficulties meet in the direct measurement of neutron induced nuclear reaction. The current existing surrogate reactions generally employ the peripheral reactions such as inelastic excitation and transfer reaction where the involved angular momenta are much larger than the neutron capture reaction, which causes a difficulty in theoretical correction of spin of compound nucleus. We proposed to use capture reaction of light charged particle as the surrogate reaction, thus the spin distributions of compound nucleus in two reactions are quite similar and therefore the spin correction is not strongly desired. Based on this idea, the 239Pu(n, f) and (n, 2n) cross sections were successfully extracted by using 236U(α,, f) and (α, 2n) reactions as the surrogate reactions. The well coincidence of the present results with the data of ENDFB7 within the error bars shows the reliability of the proposed surrogate capture reaction method.
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27

Ahmed, G. S. M., M. Tohamy, P. Bühler, and M. N. H. Comsan. "Measurements of the cross-section of 111Cd(n,n′)111mCd reaction for 241Am/Be neutrons." Modern Physics Letters A 36, no. 12 (April 7, 2021): 2150084. http://dx.doi.org/10.1142/s021773232150084x.

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The cross-section of the [Formula: see text] reaction was measured with [Formula: see text] neutrons using a natural cadmium target [Formula: see text]. The neutron fluence and mean neutron energy of the source were determined using the ISO 8529-1 neutron spectrum and the known cross-sections of the monitor reaction [Formula: see text]. In order to measure the poor [Formula: see text]-ray activity of the reaction products, an HPGe detector with 70% detection efficiency surrounded by an adequate graded shield was applied. The efficiency calculations for the detector were performed using standard point calibration sources and the EFFTRAN efficiency code. Using the measured values of the neutron flux and the induced [Formula: see text]-ray activity of [Formula: see text], the cross-section of the [Formula: see text] reaction at the average neutron energy of 4.05 MeV was found to be [Formula: see text] mb. An estimation of the contribution to the total cross-section by the accompanied reactions [Formula: see text] and [Formula: see text] was achieved and the related cross-sections were found to be 0.16 mb and 8.99 mb, respectively.
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28

Penionzhkevich, Yu, Yu Sobolev, V. Samarin, and M. Naumenko. "Energy Dependence of Total Cross Sections for Reactions with 4, 6he, 6, 7, 9li Nuclei." KnE Energy 3, no. 1 (April 9, 2018): 21. http://dx.doi.org/10.18502/ken.v3i1.1717.

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The paper presents the results of measurement of the total cross sections for reactions 4,6He + Si and 6,7,9Li + Si in the beam energy range 5−50 A⋅MeV. The enhancements of the total cross sections for reaction 6He + Si compared with reaction 4He + Si, and 9Li + Si compared with reactions 6,7Li + Si have been observed. The performed microscopic analysis of total cross sections for reactions 6He + Si and 9Li + Si based on numerical solution of the time-dependent Schrödinger equation for external neutrons of projectile nuclei 6He and 9Li yielded good agreement with experimental data.
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29

DEMİRKOL, İSKENDER. "FRAGMENTATION PRODUCTION CROSS-SECTIONS IN RELATIVISTIC COLLISIONS." Modern Physics Letters A 21, no. 38 (December 14, 2006): 2881–92. http://dx.doi.org/10.1142/s0217732306021074.

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In this study, the fragmentation production cross-sections of heavy residual nuclides in the reactions 238 U (1 A GeV ) + p and p (1.2 GeV ) + 232 Th were calculated and the production of more than 370 different isotopes for this incident reactions was presented. The calculations were made by using the Cascade-Exciton Model including pre-equilibrium effect, the Intranuclear Cascade Model, the empirical and the semi-empirical parametrization. The results of the cross-sections obtained were compared with available experimental data and examined the relation between each other. It is seen that the precision of this models to estimate residue production cross-sections is still far from the performance required for technical applications and this incident model should be improved to obtain a deeper understanding of the reaction mechanisms involved in the production of isotopes.
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30

Ou, Li, Zhuxia Li, and Xizhen Wu. "Study on in-medium nucleon–nucleon cross sections with proton-induced reaction cross sections data." Journal of Physics G: Nuclear and Particle Physics 35, no. 5 (March 19, 2008): 055101. http://dx.doi.org/10.1088/0954-3899/35/5/055101.

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31

Escher, J., L. Ahle, L. Bernstein, J. Burke, J. A. Church, F. Dietrich, C. Forssén, V. Gueorguiev, and R. Hoffman. "Surrogate nuclear reactions: an indirect method for determining reaction cross sections." Journal of Physics G: Nuclear and Particle Physics 31, no. 10 (September 12, 2005): S1687—S1690. http://dx.doi.org/10.1088/0954-3899/31/10/054.

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32

Griffiths, W. J., M. L. Langford, and F. M. Harris. "A Reaction Window in Cross-sections for Double-electron-capture Reactions." Rapid Communications in Mass Spectrometry 10, no. 9 (July 15, 1996): 997–1000. http://dx.doi.org/10.1002/(sici)1097-0231(19960715)10:9<997::aid-rcm554>3.0.co;2-a.

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33

Santry, D. C., and R. D. Werner. "Cross sections for the 93Nb(n,2n)92mNb reaction." Canadian Journal of Physics 68, no. 7-8 (July 1, 1990): 582–86. http://dx.doi.org/10.1139/p90-088.

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The cross section of the 93Nb(n,2n)92mNb reaction has been studied by use of the activation method from the threshold energy of 8.8–19.8 MeV. Measurements are relative to the known cross-section values for the reactions H(n,n)H, 32S(n,p)32p, and 27Al(n,α)24Na. The cross-section value increases smoothly with energy and reaches a maximum value of 444 ± 18 mb at about 14.5 MeV then decreases to values of 293 ± 14 mb at 19.8 MeV. An effective cross-section value for a fission neutron spectrum calculated from the results is 0.321 ± 0.019 mb. The activation of Nb as a transfer standard for 14 MeV neutrons is discussed.
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34

GOLDSTEIN, GARY R., and MICHAEL J. MORAVCSIK. "INCLUSIVE REACTIONS AND TOTAL CROSS SECTIONS WITH POLARIZED INITIAL STATES." International Journal of Modern Physics A 01, no. 01 (April 1986): 211–25. http://dx.doi.org/10.1142/s0217751x86000101.

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Total cross section measurements and the type of inclusive reactions in which no final-state polarizations are measured are discussed. The numbers and kinds of independent non-zero experiments are given and related to the exclusive reaction amplitudes. Only a well-specified and limited type of bilinear product of exclusive reaction amplitudes enter the picture. Certain classes of theories imply certain simple relationships among the observables. The main results of the investigation are summarized in Sec. 5.
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35

Warner, R. E., and G. N. Felder. "Microscopic calculations of low-energy reaction cross sections." Physical Review C 42, no. 5 (November 1, 1990): 2252–55. http://dx.doi.org/10.1103/physrevc.42.2252.

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36

Rauscher, Thomas. "Differences between stellar and laboratory reaction cross sections." Journal of Physics: Conference Series 202 (January 1, 2010): 012013. http://dx.doi.org/10.1088/1742-6596/202/1/012013.

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37

Hassan, M. Y. M., M. Y. H. Farag, A. Y. Abul-Magd, and T. E. I. Nassar. "Nucleus–nucleus reaction cross sections for deformed nuclei." Physica Scripta 78, no. 4 (October 2008): 045202. http://dx.doi.org/10.1088/0031-8949/78/04/045202.

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38

Han, Yinlu, Qingbiao Shen, Jingshang Zhang, and Zhengjun Zhang. "Calculation and Analysis ofn+232Th Reaction Cross Sections." Nuclear Science and Engineering 143, no. 2 (February 2003): 202–10. http://dx.doi.org/10.13182/nse03-a2330.

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39

Escher, Jutta E., Jason T. Burke, Frank S. Dietrich, Nicholas D. Scielzo, Ian J. Thompson, and Walid Younes. "Compound-nuclear reaction cross sections from surrogate measurements." Reviews of Modern Physics 84, no. 1 (March 13, 2012): 353–97. http://dx.doi.org/10.1103/revmodphys.84.353.

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40

Tostevin, J. A., and J. S. Al-Khalili. "Calculations of reaction cross sections for19Cat relativistic energies." Physical Review C 59, no. 1 (January 1, 1999): R5—R8. http://dx.doi.org/10.1103/physrevc.59.r5.

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41

Fukuda, M., D. Nishimura, S. Suzuki, M. Tanaka, M. Takechi, K. Iwamoto, S. Wakabayashi, et al. "Neutron halo in14B studied via reaction cross sections." EPJ Web of Conferences 66 (2014): 02037. http://dx.doi.org/10.1051/epjconf/20146602037.

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42

Arasoglu, Ali, and Omer Faruk Ozdemir. "Calculation of photo-nuclear reaction cross sections for16O." EPJ Web of Conferences 100 (2015): 01001. http://dx.doi.org/10.1051/epjconf/201510001001.

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43

Bertsch, G. F., B. A. Brown, and H. Sagawa. "High-energy reaction cross sections of light nuclei." Physical Review C 39, no. 3 (March 1, 1989): 1154–57. http://dx.doi.org/10.1103/physrevc.39.1154.

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44

Hu-Yong, Zhang, Shen Wen-Qing, Ren Zhong-Zhou, Ma Yu-Gang, Jiang Wei-Zhou, Cai Xiang-Zhou, Zhong Chen, et al. "Nuclear Radii Extracted from Experimental Reaction Cross Sections." Chinese Physics Letters 20, no. 8 (July 30, 2003): 1234–37. http://dx.doi.org/10.1088/0256-307x/20/8/314.

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Lu, P., and P. Suebka. "On the calculated cross-sections of fusion reaction." Lettere Al Nuovo Cimento Series 2 42, no. 4 (February 1985): 145–48. http://dx.doi.org/10.1007/bf02739560.

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46

Enferadi, Milad, Saber Sarbazvatan, Mahdi Sadeghi, Ji-Hong Hong, Chuan-Jong Tung, Tsi-Chian Chao, Chung-Chi Lee, and Shiaw-Pyng Wey. "Nuclear reaction cross sections for proton therapy applications." Journal of Radioanalytical and Nuclear Chemistry 314, no. 2 (October 10, 2017): 1207–35. http://dx.doi.org/10.1007/s10967-017-5503-8.

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Fujiwara, Y., and Y. C. Tang. "Reaction cross sections in the ten-nucleon system." Few-Body Systems 16, no. 2 (1994): 91–100. http://dx.doi.org/10.1007/bf01074543.

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48

Generalov, L. N., and S. N. Abramovich. "Measuring Total 6Li(d, xt) Reaction Cross Sections." Bulletin of the Russian Academy of Sciences: Physics 85, no. 5 (May 2021): 574–80. http://dx.doi.org/10.3103/s1062873821050075.

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49

LUKYANOV, V. K., E. V. ZEMLYANAYA, and K. V. LUKYANOV. "ESTIMATION OF THE BREAKUP CROSS-SECTIONS IN 6He + 12C REACTION WITHIN HIGH-ENERGY APPROXIMATION AND MICROSCOPIC OPTICAL POTENTIAL." International Journal of Modern Physics E 20, no. 09 (September 2011): 2039–47. http://dx.doi.org/10.1142/s0218301311019738.

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Abstract:
The breakup cross-sections in the reaction 6 He + 12 C are calculated at about 40 MeV/nucleon using the high-energy approximation (HEA) and with the help of microscopic optical potentials (OP) of interaction with the target nucleus 12 C of the projectile nucleus fragments 4 He and 2n. Considering the di-neutron h = 2n as a single particle the relative motion hα wave function is estimated so that to explain both the separation energy of h in 6 He and the rms radius of the latter. The stripping and absorbtion total cross-sections are calculated and their sum is compared with the total reaction cross-section obtained within a double-folding microscopic OP for the 6 He + 12 C scattering. It is concluded that the breakup cross-sections contribute to about 50% of the total reaction cross-section.
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50

Kalamara, A., M. Serris, A. Spiliotis, D. Sigalos, N. Patronis, M. Kokkoris, M. Diakaki, M. Axiotis, A. Lagoyannis, and R. Vlastou. "Activation cross section of the (n,2n) reaction on Hf isotopes." HNPS Proceedings 23 (March 8, 2019): 47. http://dx.doi.org/10.12681/hnps.1906.

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Cross sections of the 174Hf(n,2n)173Hf and 176Hf(n,2n)175Hf reactions have been experimentally determined relative to the 27Al(n,α)24Na reference reaction at incident neutron energies of 15.3 and 17.1 MeV by means of the activation technique. The irradiations were carried out at the 5 MV tandem T11/25 Accelerator Laboratory of NCSR "Demokritos" with monoenergetic neutron beams provided via the 3H(d,n)4He reaction, using a new Ti-tritiated target of 373 GBq activity. In the determination of the 176Hf(n,2n)175Hf reaction cross section the contamination of the 174Hf(n,γ)175Hf and 177Hf(n,3n)175Hf reactions has been taken into account. Moreover, the neutron beam energy has been studied by means of Monte Carlo simulation codes and the neutron flux has been determined via the 27Al(n,α)24Na reference reaction.
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