Quark and Lepton Compositeness (searches for) by K. Hagiwara

By K. Hagiwara

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3 for exclusion plot in the m e –Λ plane for m e = 35–220 GeV. 8 GeV. The same assumptions as in BARTEL 87B are used. 16 used) is subject to the e8 M s same restriction as for BARTEL 85K. 78 GeV. The limits assume 8 pair production cross sections to be eight times larger than those of the corresponding heavy lepton pair production. 306 In BARTEL 85K, R can be affected by e + e − → g g via e exchange. Their limit q m e >173 GeV (CL=95%) at λ = m e /ΛM = 1 (ηL = ηR = 1) is not listed above 8 8 because the cross section is sensitive to the product ηL ηR , which should be absent in ordinary theory with electronic chiral invariance.

DORENBOS... HAGIWARA 97 97C 97 96 96S 96K 96D 96L 96K 96Q 96W 96Z 95N 95G 95 95B 94 94 94 93G 93 93M 93 93Q 93B 92B 92D 92M 92C 92D 92B 92F 92 92 92 92 92 92 91D 91E 91F 91 91F 91B 91B 91C 90I 90F 90K 90L 90O 90F 90I 90J 90G 90O 90 89 89B 89D 89H 89J 89L 89B 89 89 89B 89C 89 89 PR D55 19 T. Arima et al. ) ZPHY C76 631 J. Breitweg et al. ) PL B409 277 A. Deandrea (MARS) PRL 77 438 F. Abe et al. ) PRL 77 5336 F. Abe et al. ) PL B380 480 P. Abreu et al. ) PL B370 211 M. Acciarri et al. ) PL B384 323 M.

Abbiendi et al. PRL 82 2457 B. Abbott et al. PRL 82 4769 B. Abbott et al. EPJ C11 383 P. Abreu et al. EPJ C8 41 P. Abreu et al. F. Zarnecki PRL 80 666 B. Abbott et al. PL B433 429 P. Abreu et al. PL B433 163 M. Acciarri et al. PL B439 183 M. Acciarri et al. EPJ C1 21 K. Ackerstaff et al. EPJ C1 45 K. Ackerstaff et al. EPJ C2 441 K. Ackerstaff et al. PL B438 379 K. Ackerstaff et al. PL B429 201 R. Barate et al. EPJ C4 571 R. Barate et al. PR D57 391 V. Barger et al. PL B443 347 I. H. S. McFarland et al.

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