Future prospects of baryon instability search in p-decay and n-n̄ oscillation experiments
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Future prospects of baryon instability search in p-decay and n-n̄ oscillation experiments proceedings of the International Workshop on Future Prospects of Baryon Instability Search in p-Decay and n-n̄ Oscillation Experiments : Oak Ridge, Tennessee, U.S.A., March 28-30, 1996 by International Workshop on Future Prospects of Baryon Instability Search in p-Decay and n-nМ„ Oscillation Experiments (1996 Oak Ridge, Tenn.)

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Published by Oak Ridge National Laboratory in Oak Ridge, Tenn .
Written in English

Subjects:

  • Baryons -- Congresses.,
  • Protons -- Decay -- Congresses.

Book details:

Edition Notes

Statementedited by S. J. Ball and Y.A. Kamyshkov ; organizing committee, W.M. Bugg ... [et al.].
GenreCongresses.
ContributionsBall, S. J., Kamyshkov, Y. A.
Classifications
LC ClassificationsQC793.5.B32 I58 1996
The Physical Object
Paginationvii, 405 p. :
Number of Pages405
ID Numbers
Open LibraryOL285633M
LC Control Number97188742
OCLC/WorldCa36247944

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The work of C.Q. Geng and Y.K. Hsiao was supported in part by the National Center for Theoretical Sciences, MoST (MoSTMMY3), and the Author: Y. K. Hsiao, C. Q. Geng, C. Q. Geng, Eduardo Rodrigues. Baryon semileptonic decays The typical spin-1/2 baryon semileptonic decay is described by a matrix element, the hadronic part of which may be written as: Bf £ f1(q2)γλ +i f2(q2)σλ qµ +g1(q2)γλγ5 +g3(q2)γ5qλ ¤ Bi. (1) Here Bi and Bf are spinors describing the initial and final baryons, and q = pi − pf, while the terms in f1, f2. Search for Nucleon Instability (Origin and History), in the Proceedings of International Workshop on Future Prospects of Baryon Instability Search in p-Decay and n → ¯ n Oscillation Experiments. of helicity amplitudes and angular distributions and so on. More experiments on the charmonium decays into baryon anti-baryon pair are expected for determining the color octet wave function. Another interesting measurement is the angular distribution for the process e+e¡! J=ˆ or ˆ0! B8B„8, which takes the form: d¡ dcosµ / 1+ +¡ J=ˆ.

Future prospects of baryon instability search in p-decay and n-n̄ oscillation experiments: proceedings of the International Workshop on Future Prospects of Baryon Instability Search in p-Decay and n-n̄ Oscillation Experiments: Oak Ridge, Tennessee, U.S. A search query can be a title of the book, a name of the author, ISBN or anything else. International Workshop on Future Prospects of Baryon Instability Search in p decay and n > anti-n Oscillation Experiments, ; book chapter. 2. book. 1. proceedings. 1. Author. Hans Ströher. Michael Hartmann. Sergey Dymov. Progress and Simulations for Intranuclear Neutron--Antineutron Transformations in ${}^{40}_{18} Ar. June baryons. Theoretically, b baryons [ ] provide in- teresting tests of the spectator model ofb-hadron de- cays and heavy flavour spectroscopy. In this letter, a study of the decay Ab--,A + ~-9 fol- lowed by the decay A + -~AX is reported. Here and throughout this letter charge conjugate reactions are.

  In the light of future prospects of LHCb, we further extended our analysis with focus on the study of non-leptonic weak decays of the doubly charmed baryon, \(\Omega _{cc}^{+}\). In the factorization model, we obtained the form factors, \(f_i\) and \(g_i\), using the approaches based on the nonrelativistic quark model [ 53 ] and heavy quark. Baryons and mesons How are baryons and mesons classified? What are baryons and mesons made of? What decay processes involve baryons and mesons? How are mesons classified? The earliest classification scheme for particles was based on their masses. They can be grouped into three. N BARYONS (S = 0, I = 1/2) p, N+ = uud; n, N0 = udd p I(JP) = 1 2(1 2 +) Mass m = ± u p DECAY MODESDECAY MODESDECAY MODES ( years) Confidence level (MeV/c) Mean nn-oscillation time > × s, CL = 90% [f].   The cross sections (σ in and σ e1) of low energy n interaction with different nuclei are optical-cascade model of slow n̄ annihilation on nuclear target is developed with the aim to use it as an event generator for n → n̄ search experiment. New limit for the n → n̄ oscillation period in vacuum is obtained from the stability of 16 O.