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Mohammad M. Alsharo’a et al.
Show Abstract
We describe the status of our effort to realize a first neutrino factory and the progress made in understanding the problems associated with the collection and cooling of muons towards that end. We summarize the physics that can be done with neutrino factories as well as with intense cold beams of muons. The physics potential of muon colliders is reviewed, both as Higgs factories and compact high-energy lepton colliders. The status and time scale of our research and development effort is reviewed as well as the latest designs in cooling channels including the promise of ring coolers in achieving longitudinal and transverse cooling simultaneously. We detail the efforts being made to mount an international cooling experiment to demonstrate the ionization cooling of muons.
Phys. Rev. ST Accel. Beams 6, 081001 (2003)
Cited 27 times
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J. Cook, K. W. Kemper, P. V. Drumm, L. K. Fifield, M. A. Hotchkis, T. R. Ophel, and C. L. Woods
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The elastic scattering of 7Li+16O has been measured at ELi=50 MeV and fitted with an optical model potential. The 16O(7Li,7Be)16N reaction has been investigated at ELi=50 MeV. States and groups of states were observed up to 6.3 MeV excitation in the 16N+7Be system. Angular distributions for 16N in 2- 0.0 MeV, 3- 0.297 MeV, and 4- 6.17 MeV states with 7Be in its ground state (7Be0), and for 16N in the 3- 0.297 MeV state with 7Be in its first excited state (7Be1), have been compared with distorted-wave Born approximation calculations. The distorted-wave Born approximation form factors were calculated microscopically using central and tensor forces and realistic transition densities. The calculations fail to reproduce the cross sections.
Phys. Rev. C 30, 1538 (1984)
Cited 22 times
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S. Roman, O. Karban, J. M. Barnwell, J. D. Brown, P. V. Drumm, P. M. Lewis, and J. M. Nelson
Show Abstract
Polarized 3He particles have been used to initiate (3He→, p) reactions on light nuclei. The results obtained have been compared with the available data for (3He, p→) and the inverse (p→, 3He) reactions. It is suggested that the reactions proceed predominantly by a direct transfer mechanism and follow a simple reaction model which relates the polarization of the (3He, p→) to the analyzing power of the (3He→, p) reaction according to the S transfer. If time-reversal invariance is applied, the present (3He→, p) results for 7Li and 9Be are in agreement with the (p→, 3He) measurements on 9Be and 11B targets. NUCLEAR REACTIONS 7Li(3He→, p)9Be, 9Be(3He→, p)11B; E=14 MeV; 12C(3He→, p)14N, E=33 MeV; measured Ay(θ).
Phys. Rev. C 28, 2515 (1983)
Cited 0 times
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