A.C. Shotter
University of Edinburgh
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Featured researches published by A.C. Shotter.
Nuclear Physics | 1999
C. Angulo; Marcel Arnould; Marc Rayet; Pierre Descouvemont; Daniel Jean Baye; Alain Coc; S. Barhoumi; P. Aguer; C. Rolfs; R. Kunz; J.W. Hammer; A. Mayer; T. Paradellis; S. Kossionides; C. Chronidou; K. Spyrou; S. Degl'Innocenti; G. Fiorentini; B. Ricci; S. Zavatarelli; C. Providencia; H. Wolters; J. Soares; C. Grama; J. Rahighi; A.C. Shotter; M. Lamehi Rachti
Low-energy cross section data for 86 charged-particle induced reactions involving light (1 less than or equal to Z less than or equal to 14), mostly stable, nuclei are compiled. The corresponding Maxwellian-averaged thermonuclear reaction rates of relevance in astrophysical plasmas at temperatures in the range from 10(6) K to 10(10) K are calculated. These evaluations assume either that the target nuclei are in their ground state, or that the target states are thermally populated following a Maxwell-Boltzmann distribution, except in some cases involving isomeric states. Adopted values complemented with lower and upper limits of the rates are presented in tabular form. Analytical approximations to the adopted rates, as well as to the inverse/direct rate ratios, are provided
Physical Review Letters | 2008
I. Tanihata; M. Alcorta; D. Bandyopadhyay; R. Bieri; L. Buchmann; B. Davids; N. Galinski; D. Howell; W. Mills; S. Mythili; R. Openshaw; E. Padilla-Rodal; G. Ruprecht; G. Sheffer; A.C. Shotter; M. Trinczek; P. Walden; H. Savajols; T. Roger; M. Caamaño; W. Mittig; P. Roussel-Chomaz; R. Kanungo; Gallant A; Notani M; G. Savard; Thompson Ij
The p(\nuc{11}{Li},\nuc{9}{Li})t reaction has been studied for the first time at an incident energy of 3
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
A. N. Ostrowski; S. Cherubini; T. Davinson; D. Groombridge; A.M. Laird; A. Musumarra; A. Ninane; A. Di Pietro; A.C. Shotter; P. J. Woods
A
Physical Review Letters | 2008
I. Tanihata; M. Alcorta; D. Bandyopadhyay; R. Bieri; L. Buchmann; B. Davids; N. Galinski; D. Howell; W. Mills; S. Mythili; R. Openshaw; E. Padilla-Rodal; G. Ruprecht; G. Sheffer; A.C. Shotter; M. Trinczek; P. Walden; H. Savajols; T. Roger; M. Caamaño; W. Mittig; P. Roussel-Chomaz; R. Kanungo; Gallant A; Notani M; G. Savard; Thompson Ij
MeV delivered by the new ISAC-2 facility at TRIUMF. An active target detector MAYA, build at GANIL, was used for the measurement. The differential cross sectionshave been determined for transitions to the \nuc{9}{Li} ground andthe first excited states in a wide range of scattering angles. Multistep transfer calculations using different \nuc{11}{Li} model wave functions, shows that wave functions with strong correlations between the halo neutrons are the most successful in reproducing the observation.
Tours symposium on nuclear physics III | 1998
J.D. King; James C. Chow; Andrew C. Morton; R. E. Azuma; N. Bateman; Richard N. Boyd; L. Buchmann; J. M. D’Auria; Thomas Davinson; M. Dombsky; W. Galster; E. Gete; U. Giesen; C. Iliadis; K. P. Jackson; G. Roy; T. D. Shoppa; A.C. Shotter
A very compact double sided silicon strip detector array is described, designed for use in reaction studies involving radioactive nuclear beams. It is small enough to fit inside a large solid angle g-detector array and will enable Dopplershift corrections at energies in the vicinity of the Coulomb barrier. The detector provides sufficient energy and time-offlight resolution for the identification of light reaction products and can be set up to cover a substantial part of the scattering angular distribution with good resolution. The device is available in thicknesses of up to 500 mm to stop all interesting reaction products. Moreover, a very thin (35–40 mm) variant of this detector is described that can be used as an energy loss detector in a DE@E telescope geometry followed by a detector that measures the residual energy. This provides additional particle identification capabilities, e.g. in light exotic nuclei induced reactions. First results from a commissioning run using a post-accelerated radioactive beam are presented. r 2002 Elsevier Science B.V. All rights reserved.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1987
J. Yorkston; A.C. Shotter; D.B. Syme; G. Huxtable
The p(\nuc{11}{Li},\nuc{9}{Li})t reaction has been studied for the first time at an incident energy of 3
Physics Letters B | 1999
R. Raabe; A. Piechaczek; A. N. Andreyev; Daniel Jean Baye; W. Bradfield-Smith; S. Cherubini; T. Davinson; Pierre Descouvemont; A. Di Pietro; W. Galster; M. Huyse; A.M. Laird; J. McKenzie; Wolfgang Mueller; A. N. Ostrowski; A.C. Shotter; P. Van Duppen; A. Wöhr
A
Physics Letters B | 1996
C.R. Bain; P. J. Woods; R. Coszach; Thomas Davinson; P. Decrock; M. Gaelens; W. Galster; M. Huyse; Rj Irvine; Pierre Leleux; E. Lienard; Marc Loiselet; C. Michotte; R. Neal; A. Ninane; Guido Ryckewaert; A.C. Shotter; G. Vancraeynest; Jean Vervier; J. Wauters
MeV delivered by the new ISAC-2 facility at TRIUMF. An active target detector MAYA, build at GANIL, was used for the measurement. The differential cross sectionshave been determined for transitions to the \nuc{9}{Li} ground andthe first excited states in a wide range of scattering angles. Multistep transfer calculations using different \nuc{11}{Li} model wave functions, shows that wave functions with strong correlations between the halo neutrons are the most successful in reproducing the observation.
Physics Letters B | 1986
J. C. McGeorge; G. I. Crawford; R. O. Owens; M.R. Sené; D. Branford; A.C. Shotter; B. Schoch; R. Beck; P. Jennewein; Frank Klein; Johannes Vogt; F. Zettl
We are studying the β-delayed proton decay of 17Ne with the goal of determining the E2 part of the 12C(α,γ)16O cross section at energies relevant to helium burning in stars. We have determined branching ratios for proton and α-decay for states in 17F from 8.08 to 11.193 MeV. In addition, we have observed the break-up of the isobaric analogue state (IAS) at 11.193 MeV into three particles via two channels: proton decay to the 9.59 MeV state in 16O which breaks up into an α-particle plus 12C; and α-decay to the 2.365 MeV state in 13N which breaks up into a proton plus 12C. This is the first reported observation of the decay of the IAS to the 1− state in 16O at 9.59 MeV.
Nuclear Physics | 1997
J.S. Graulich; Freddy Binon; W. Bradfield-Smith; M. Cogneau; R. Coszach; T. Davinson; Thierry Delbar; M. Gaelens; W. Galster; J. Görres; Daniel Labar; P. Leleux; Marc Loiselet; J. H. McKenzie; R. Neal; Guido Ryckewaert; A.C. Shotter; J. Vanhorenbeeck; Jean Vervier; M. Wiescher; P. J. Woods
Abstract An investigation is reported into charge sharing effects for highly ionising particles penetrating the interstrip gap for ion-implanted silicon strip detectors. It is found that under certain conditions anomalous polarity pulses are induced on adjacent strips. This effect is analysed with a model that takes account of the surface charge trapped on the SiSiO 2 interface between the adjacent strips.