Calculation of the cross section fore+-e−(Korbit) pairs by very-high-energy fully stripped heavy ions at perturbational impact parameters

1993 ◽  
Vol 48 (3) ◽  
pp. 2002-2011 ◽  
Author(s):  
A. J. Baltz ◽  
M. J. Rhoades-Brown ◽  
J. Weneser
2014 ◽  
Vol 734 ◽  
pp. 207-209 ◽  
Author(s):  
M.M. Block ◽  
L. Stodolsky

1997 ◽  
Vol 504 ◽  
Author(s):  
A. Barbu ◽  
G. Jaskierowicz

ABSTRACTThe creep velocity of B203 glass fibers under irradiation with 2.5 MeV electrons at low flux ( around 5 1013 e-cm−2s−1) has been studied versus temperature. As under very high energy heavy ions irradiation (1.6 GeV argon), the viscosity is drastically reduced below 300°C. An important difference between the two kinds of irradiation is the occurrence of a compaction phenomenon at the beginning of electron irradiation experiments. The results can be understood by assuming two totally different mechanisms: a relaxation driven by melting of the glass along the path of the ions for very high energy heavy ion irradiations and a relaxation driven by individual radiation induced points defects for high energy electron irradiations.


1992 ◽  
Vol 07 (20) ◽  
pp. 4707-4745 ◽  
Author(s):  
G.L. KOTKIN ◽  
V.G. SERBO ◽  
A. SCHILLER

At the collider VEPP-4 a remarkable deviation of the measured bremsstrahlung photons from the standard calculation method has been measured in the reaction e+e−→e+e−γ. The decreasing number of photons is explained by the fact that large impact parameters give the essential contributions to the cross section. These parameters are by several orders of magnitude larger than the transverse beam sizes. In that case the standard definitions of “cross section” and “number of events” are invalid. Similar effects are expected for the single photon bremsstrahlung and the e+e− pair production at existing and planned high energy e±e−, ep and eγ colliders. A calculation scheme for particle production in the interaction of two bunches, which allows one to take into account these effects quantitatively, is presented. In this scheme the colliding bunches are represented as wave packets, and quantum distribution functions are used. The modified definitions of the cross section and the number of events contain the features of “nonlocality” and “interference”. Reasonable approximations which can be easily used are discussed. The results are applied to analyze the influence of the finite beam sizes on reactions which have been proposed for measuring the luminosity and the beam polarization at the colliders LEP and HERA.


1994 ◽  
Vol 49 (5) ◽  
pp. 2310-2315 ◽  
Author(s):  
M. C. Gonzalez-Garcia ◽  
F. Halzen ◽  
R. A. Vázquez ◽  
E. Zas

Author(s):  
A. Barbu ◽  
A. Dunlop ◽  
D. Lesueur ◽  
G. Jaskierowicz

2009 ◽  
Vol 63 (1) ◽  
pp. 69-85 ◽  
Author(s):  
R. M. Godbole ◽  
A. Grau ◽  
G. Pancheri ◽  
Y. N. Srivastava

1955 ◽  
Vol 33 (12) ◽  
pp. 828-840 ◽  
Author(s):  
J. T. Sample ◽  
G. C. Neilson ◽  
G. B. Chadwick ◽  
J. B. Warren

Bombardment of B10 with 1.4 Mev. deuterons has been found to produce gamma rays of energy 4.46 ±.04, 4.75 ±.03, 5.03 ±.09, 5.35 ±.05, 6.52 ±.04, 6.78 ±.07, 7.29 ±.04, 8.27 ±.09, and 8.87 ±.02 Mev., as measured with a three-crystal pair spectrometer. Tentative assignments to transitions in B11 and C11 agree well in most cases with the known energy level schemes. No gamma rays of very high energy were observed, even with a single-crystal spectrometer; consequently an upper limit of 10−31 cm.2 has been placed on the cross-section of B10(d, γ)C12 at 0.95 Mev. bombarding energy.


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