排序方式: 共有26条查询结果,搜索用时 375 毫秒
21.
Sandler PH Smith WH Bachmann K Blair R Foudas C King B Lefmann WC Leung WC Mishra SR Quintas P Rabinowitz SA Sciulli F Seligman W Shaevitz MH Merritt FS Oreglia MJ Schellman H Schumm B Bernstein RH Borcherding F Lamm MJ Marsh W Yovanovitch D Bodek A Budd HS de Barbaro P Sakumoto WK 《Physical review D: Particles and fields》1990,42(3):759-770
22.
Rabinowitz SA Arroyo C Bachmann KT Bazarko AO Bolton T Foudas C King BJ Lefmann WC Leung WC Mishra SR Oltman E Quintas PZ Sciulli FJ Seligman WG Shaevitz MH Merritt FS Oreglia MJ Schumm MJ Bernstein RH Borcherding F Fisk HE Lamm MJ Marsh W Merritt KW Schellman HM Yovanovitch DD Bodek A Budd HS de Barbaro P Sakumoto WK Kinnel T Sandler PH Smith WH 《Physical review letters》1993,70(2):134-137
23.
P. H. Sandler T. S. Kinnel W. H. Smith K. Bachmann R. Blair C. Foudas B. King W. C. Lefmann W. C. Leung S. R. Mishra P. Z. Quintas S. A. Rabinowitz F. Sciulli W. seligman M. H. Shaevitz F. S. Merritt M. J. Oreglia H. Schellman B. Schumm R. H. Bernstein F. Borcherding M. J. Lamm W. Marsh D. Yovanovitch A. Bodek H. S. Budd P. de Barbaro W. K. Sakumoto 《Zeitschrift fur Physik C Particles and Fields》1993,57(1):1-12
The rate of neutrino- and antineutrino-induced prompt same-sign dimuon production in steel was measured using a sample of μ?μ? events and 25 μ+μ+ events withP μ>9 GeV/c, produced in 1.5 millionv μ and 0.3 million \(\overline {v_\mu }\) induced charged-current events with energies between 30 GeV and 600 GeV. The data were obtained with the Chicago-Columbia-Fermilab-Rochester (CCFR) neutrino detector in the Fermilab Tevatron Quadrupole Triplet Neutrino Beam during experiments E 744 and E 770. After background subtraction, the prompt rate of same-sign dimuon production is (0.53±0.24)×10?4 perv μ charged-current event and (0.52±0.33)×10?4 per \(\overline {v_\mu }\) charged-current event. The kinematic distributions of the same-sign dimuon events after background subtraction are consistent with those of the non-prompt background due to meson decays in the hadron shower of a charged-current event. Calculations ofc \(\bar c\) gluon bremsstrahlung, based on improved measurements of the charm mass parameter and nucleon structure functions by the CCFR collaboration, yield a prompt rate of (0.09±0.39)×10?4 perv μ charged-current event. In this case,c \(\bar c\) gluon bremsstrahlung is probably not an observable source of prompt same-sign dimuons. 相似文献
24.
Sakumoto WK de Barbaro P Bodek A Budd HS Kim BJ Merritt FS Oreglia MJ Schellman H Schumm BA Bachmann KT Blair RE Foudas C King BJ Lefmann WC Leung WC Mishra SR Oltman E Quintas PZ Rabinowitz SA Sciulli F Seligman WG Shaevitz MH Bernstein RH Borcherding FO Fisk HE Lamm MJ Marsh W Merritt KW Rapidis PA Yovanovitch D Sandler PH Smith WH 《Physical review D: Particles and fields》1992,45(9):3042-3050
25.
26.
Mishra SR Rabinowitz SA Arroyo C Bachmann KT Blair RE Foudas C King BJ Lefmann WC Leung WC Oltman E Quintas PZ Sciulli FJ Seligman BG Shaevitz MH Merritt FS Oreglia MJ Schumm BA Bernstein RH Borcherding F Fisk HE Lamm MJ Marsh W Merritt KW Schellman H Yovanovitch DD Bodek A Budd HS de Barbaro P Sakumoto WK Sandler PH Smith WH 《Physical review letters》1991,66(24):3117-3120