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In a fusion reactor, a proton and a neutron generated in previous reactions may again fuse with each other. Or they can in turn fuse with or be captured by an un-reacted deuteron. The average center-of-mass (COM) energy for such reaction is…

Nuclear Theory · Physics 2009-10-21 Nie Luo

The proton capture cross-section of the least abundant proton-rich stable isotope of cadmium, $^{108}$Cd (abundance 0.89\%), has been measured near the Gamow window corresponding to a temperature range of 3-4 GK. The measurement of the…

Differential cross sections for Compton scattering from the proton have been measured at scattering angles of $55^\circ$, $90^\circ$, and $125^\circ$ in the laboratory frame using quasimonoenergetic linearly (circularly) polarized photon…

Carbon-enhanced metal-poor (CEMP) stars in the Galactic Halo display enrichments in heavy elements associated with either the s (slow) or the r (rapid) neutron-capture process (e.g., barium and europium respectively), and in some cases they…

Solar and Stellar Astrophysics · Physics 2016-11-15 Melanie Hampel , Richard J. Stancliffe , Maria Lugaro , Bradley S. Meyer

Charge-changing transitions play a significant role in stellar weak-decay processes. The fate of the massive stars is decided by these weak-decay rates including lepton (positron and electron) captures rates, which play a consequential role…

Nuclear Theory · Physics 2025-05-07 Jameel-Un Nabi , Muhammad Majid

The nuclear level density of $^{115}$Sn has been measured in an excitation energy range of $\sim $2 - 9 MeV using the experimental neutron evaporation spectra from the $^{115}$In($p,n$)$^{115}$Sn reaction. The experimental level densities…

We present the first calculations to follow the evolution of all stable isotopes (and their abundant radioactive progenitors) in a finely zoned stellar model computed from the onset of central hydrogen burning through explosion as a Type II…

Astrophysics · Physics 2007-05-23 A. Heger , R. D. Hoffman , T. Rauscher , S. E. Woosley

The neutron capture cross section of 48Ca was measured relative to the known gold cross section at kT = 52 keV using the fast cyclic activation technique. The experiment was performed at the Van-de-Graaff accelerator, Universitaet…

Nuclear Experiment · Physics 2008-11-26 P. Mohr , H. Oberhummer , H. Beer , W. Rochow , V. Koelle , G. Staudt , P. V. Sedyshev , Yu. P. Popov

Neutron capture cross-section measurements are fundamental in the study of astrophysical phenomena, such as the slow neutron capture (s-) process of nucleosynthesis operating in red-giant and massive stars. However, neutron capture…

The results of the study of gamma-transition description in fast neutron capture and photofission are presented. Recent experimental data were used, namely, the spectrum of prompt gamma-rays in the energy range 2{\div}18 MeV from 14-MeV…

We investigated the probability distribution of the thermal neutron capture cross section ($\sigma_{th}$) deduced stochastically with the resonance parameters randomly sampled from Wigner and Porter-Thomas distributions. We found that the…

Nuclear Theory · Physics 2019-07-31 N. Furutachi , F. Minato , O. Iwamoto

Neutron total reaction cross sections at 45, 50, 55, 60, 65, and 75 MeV from nuclei 12C, 28Si, 56Fe, 90Zr, and 208Pb have been measured and are compared with (microscopic) optical model predictions. The optical potentials were obtained in…

Nuclear Theory · Physics 2009-11-07 K. Amos , S. Karataglidis

The 15N(p,n) reaction is a promising candidate for the production of monoenergetic neutrons with energies of up to 5.7 MeV at the facilities where the T(p,n)3He reaction cannot be used. The characteristic properties of this reaction were…

Nuclear Experiment · Physics 2022-11-08 Erik Poenitz , Ralf Nolte , Dankwart Schmidt , Guochang Chen

Proton-$\gamma$ coincidences from $(\mathrm{d},\mathrm{p})$ reactions between a $^{66}\mathrm{Ni}$ beam and a deuterated polyethylene target have been analyzed with the inverse-Oslo method to find the nuclear level density (NLD) and…

The SNO+ experiment collected data as a low-threshold water Cherenkov detector from September 2017 to July 2019. Measurements of the 2.2-MeV $\gamma$ produced by neutron capture on hydrogen have been made using an Am-Be calibration source,…

Instrumentation and Detectors · Physics 2020-07-15 The SNO+ Collaboration , : , M. R. Anderson , S. Andringa , M. Askins , D. J. Auty , N. Barros , F. Barão , R. Bayes , E. W. Beier , A. Bialek , S. D. Biller , E. Blucher , R. Bonventre , M. Boulay , E. Caden , E. J. Callaghan , J. Caravaca , D. Chauhan , M. Chen , O. Chkvorets , B. Cleveland , M. A. Cox , M. M. Depatie , J. Dittmer , F. Di Lodovico , A. D. Earle , E. Falk , N. Fatemighomi , V. Fischer , E. Fletcher , R. Ford , K. Frankiewicz , K. Gilje , D. Gooding , C. Grant , J. Grove , A. L. Hallin , D. Hallman , S. Hans , J. Hartnell , P. Harvey , W. J. Heintzelman , R. L. Helmer , D. Horne , B. Hreljac , J. Hu , A. S. M. Hussain , A. S. Inácio , C. J. Jillings , T. Kaptanoglu , P. Khaghani , J. R. Klein , R. Knapik , L. L. Kormos , B. Krar , C. Kraus , C. B. Krauss , T. Kroupova , I. Lam , B. J. Land , A. LaTorre , I. Lawson , L. Lebanowski , E. J. Leming , A. Li , J. Lidgard , B. Liggins , Y. H. Lin , Y. Liu , V. Lozza , M. Luo , S. Maguire , A. Maio , S. Manecki , J. Maneira , R. D. Martin , E. Marzec , A. Mastbaum , N. McCauley , A. B. McDonald , P. Mekarski , M. Meyer , C. Mills , I. Morton-Blake , S. Nae , M. Nirkko , L. J. Nolan , H. M. O'Keeffe , G. D. Orebi Gann , M. J. Parnell , J. Paton , S. J. M. Peeters , T. Pershing , L. Pickard , G. Prior , A. Reichold , S. Riccetto , R. Richardson , M. Rigan , J. Rose , R. Rosero , P. M. Rost , J. Rumleskie , I. Semenec , F. Shaker , M. K. Sharma , K. Singh , P. Skensved , M. Smiley , M. I. Stringer , R. Svoboda , B. Tam , L. Tian , J. Tseng , E. Turner , R. Van Berg , J. G. C. Veinot , C. J. Virtue , E. Vázquez-Jáuregui , S. C. Walton , J. Wang , M. Ward , J. J. Weigand , J. R. Wilson , P. Woosaree , A. Wright , J. P. Yanez , M. Yeh , T. Zhang , Y. Zhang , K. Zuber , A. Zummo

We use distorted wave electron scattering calculations to extract the weak charge form factor F_W(q), the weak charge radius R_W, and the point neutron radius R_n, of 208Pb from the PREX parity violating asymmetry measurement. The form…

Based on large-scale shell model calculations we have determined the electron capture, positron capture and beta-decay rates on more than 100 nuclei in the mass range A=45-65. The rates are given for densities \rho Y_e =10^7-10^{10}…

Nuclear Theory · Physics 2011-05-05 K. Langanke , G. Martinez-Pinedo

The cross sections of the astrophysically relevant 85$Rb(p,n)85Srg,m reaction have been measured between Ec.m. = 2.16 and 3.96 MeV. The cross sections have been derived by measuring the gamma radiation following the beta decay of the…

Nuclear Experiment · Physics 2009-11-13 G. G. Kiss , Gy. Gyürky , A. Simon , Zs. Fülöp , E. Somorjai , T. Rauscher

In stars with temperatures above 20*10^6 K, hydrogen burning is dominated by the CNO cycle. Its rate is determined by the slowest process, the 14N(p,gamma)15O reaction. Deep underground in Italy's Gran Sasso laboratory, at the LUNA 400 kV…

The 95Zr(n,gamma)96Zr reaction cross section is crucial in the modelling of s-process nucleosynthesis in asymptotic giant branch stars because it controls the operation of the branching point at the unstable 95Zr and the subsequent…