A. Nadasen
University of Michigan
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Featured researches published by A. Nadasen.
Nuclear Physics | 1998
R.E. Warner; H. Thirumurthy; J. Woodroffe; F. D. Becchetti; J. A. Brown; Barry Samuel Davids; A. Galonsky; J. J. Kolata; J. J. Kruse; M. Y. Lee; A. Nadasen; T.W. O'Donnell; D. A. Roberts; R. M. Ronningen; C. Samanta; P. Schwandt; J. von Schwarzenberg; M. Steiner; K. M. Subotic; J. Wang; J.A. Zimmerman
Abstract Total reaction cross sections, σ R , on Si were measured near 40 A MeV for the proton-halo candidate 12 N and the two-proton-halo candidate 17 Ne, and were compared with σ R for other light proton-rich nuclei. The A -dependence shows enhanced σ R s for 12 N and 17 Ne, relative to their neighbors, but the effect is smaller than for 8 B which has been argued to have a proton halo. In general, nuclei with loosely bound last protons ( S p ⩽ 1.5 MeV) have significantly larger σ R s than their neighbors. Cross sections for charge-removal from 12 N and 17 Ne also were obtained.
Nuclear Physics | 1985
R. E. Warner; J-Q. Yang; D.L. Friesel; P. Schwandt; G. Caskey; A. Galonsky; B. Remington; A. Nadasen; N.S. Chant; F. Khazaie; C. Wang
Abstract The 6 Li(p, pd) 4 He reaction was studied at 200.2 MeV, at the quasi-free angle pair ( θ p , θ d ) = (54°, −48.9°), for noncoplanarity angles φ from 0° to 28°. 6 Li αd spectroscopic factors of 0.84 and 0.76 are deduced from our coplanar data at this energy and 120 MeV, respectively, for ground-state 2S Woods-Saxon wave functions. A recent microscopic three-body calculation predicts spectroscopic factors from 0.70 to 0.75; using the ground-state wave functions from this study, we deduce a factor of 0.76 from the 200 MeV data. DWIA calculations fit the measured integrated cross sections versus φ for spectator momenta P α ≲ 100 MeV/ c at both bombarding energies, but underpredict them for larger P α . Momentum form factors were better reproduced with 1S αd cluster wave functions for a soft-core bound-state potential than with the 2S Woods-Saxon wave functions, but the former wave functions generate unphysically large (∼1.25) spectroscopic factors.
Physical Review C | 2006
R. E. Warner; F. Carstoiu; J. Brown; F. D. Becchetti; D. A. Roberts; B. Davids; A. Galonsky; R. M. Ronningen; M. Steiner; Mihai Horoi; J. J. Kolata; A. Nadasen; C. Samanta; J. Schwartzenberg; K. Subotic
Excitation functions for total reaction cross sections,
Nuclear Physics | 1984
R. E. Warner; R.S. Wakeland; J-Q. Yang; D.L. Friesel; P. Schwandt; G. Caskey; A. Galonsky; B. Remington; A. Nadasen
{\ensuremath{\sigma}}_{R}
Physics Letters B | 1995
J. Yee; E. Gualtieri; D. Craig; S. Hannuschke; T. Li; W. J. Llope; R. Pak; N. T. B. Stone; A. M. Vander Molen; G. D. Westfall; J. S. Winfield; S. J. Yennello; R. Lacey; A. Nadasen; Edwin Norbeck
, were measured for the light, mainly proton-rich nuclei
Physics Letters B | 1994
J. Lauret; R. Lacey; A. Elmaani; A. Tsepetis; A. Moores; G. D. Westfall; D. Craig; E. Gualtieri; S. Hannuschke; T. Li; W. J. Llope; R. Pak; N. T. B. Stone; A. M. Vander Molen; J. Yee; A. Nadasen; Robert Tickle; Edwin Norbeck
^{6}\mathrm{Li}
Nuclear Physics | 1987
R. E. Warner; F.G. Johnson; C. P. Browne; A.A. Rollefson; A. Galonsky; A. Nadasen
,
Nuclear Physics | 1986
R. E. Warner; B.A. Vaughan; D.L. Friesel; P. Schwandt; J-Q. Yang; G. Caskey; A. Galonsky; B. Remington; A. Nadasen
^{7}\mathrm{Be}
Nuclear Instruments & Methods in Physics Research Section B-beam Interactions With Materials and Atoms | 1986
D.L. Friesel; P. Schwandt; A. Nadasen; G. Caskey; A. Galonsky; R. E. Warner
,
Nuclear Physics | 1991
J. Jänecke; F. D. Becchetti; A. M. van den Berg; G.P.A. Berg; G. Brouwer; M.B. Greenfield; M.N. Harakeh; M.A. Hofstee; A. Nadasen; D. A. Roberts; R. Sawafta; J.M. Schippers; E.J. Stephenson; D.P. Stewart; S.Y. van der Werf
^{10}\mathrm{B}