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gb→tH One Loop SUSY-QCD Corrections and Nondecoupling Effects

  • In this paper one loop SUSY QCD radiative correction to gb→tHcross section is calculated in the context of Minimal Supersymmetric Standard Model. We found that non decoupling effects of SUSY QCD will occur if the gluino mass and the SUSY soft breaking parameter μ or At,Ab are at the same order and get large. The non decoupling contribution can be enhanced by large tan β and therefore large corrections to the hadronic production rates at the Tevatron and LHC are expected in the large tan β limit. The fundamental reason for such non decoupling behavior is found to be some couplings in the loops being proportional to SUSY mass parameters.
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  • [1] . KUANG Y P .HEP NP ,1999,23:110(in Chinese)(邝宇平.高能物理与核物理,1999,23:110)2. LI C S .HEP NP ,1999,23:117(in Chinese)(李重生.高能物理与核物理,1999,23:117)3. Haber H E ,Kane G L .Phys.Rept.,1985,117:754. LI C S ,YANG J M .Phys.Lett.,1993,B315:367;LI C S ,HU B Q ,YANG J M .1993,D47:2865;YANG J .M .,LI C S ,HU B Q .Phys.Lett.,1993,D47:2872;Coarasa J A et al.Eur.Phys.J.,1998,C2:3735. Borzumati F ,Kneur J L ,Polonsky N .Phys.Rev.,1999,D60:115011;JIN L G et al.Phys.Rev.,2000,D62:053008 6. Bawa A C ,Kim C S ,Martion A D .Z .Phys.,1990,C47:75;Barger V ,Phillips R J,Roy D P .Phys.Lett.,1994,B324:236;Moretti S ,Odagiri K .Phys.Rev.,1997,D55:5627. Guasch J,Jimenez R A ,Sola J.Phys.Lett.,1995,B360:47;Jimenez R ,Sola J .Phys.Lett.,1996,B389:53;Coarasa J A ,Jimenez R A ,Sola J.Phys.Lett.,1996,B389:3128. Carena M ,Mrenna S ,Wagner C E M . Phys.Rev.,1999,D60:075010;2000,D62:055008;Belyaev A et al.Phys.Rev.,2002,D65:031701;Curiel A et al.Phys.Rev.,2002,D65:075006;Alanakyan R A ,Grabski V .hep- ph/9711436 9 Haber H E et al.Phys.Rev.,2001,D63:05500410. Herrero M J ,Penaranda P ,Temes D .Phys.Rev.,2001,D64:11500311. Dobado A ,Herrero M J ,Temes D .Phys.Rev.,2002,D65:07502312. Appelquist T ,Carazzone J .Phys.Rev.,1975,D11:285613. LAI H L et al.Eur.Phys.J.,2000,C12:37514. Gunion J F ,Harber H E .Nucl.Phys.,1986,B272:115. Djouadi A ,Kalinowski J,Spira M .Comp.Phys.Commun.,1998,108:5616. Brown H N et al.Phys.Rev.Lett.,2001,86:222717. Particle Physics Group.Eur.Phys.J .,2000,C15:27418. Carena M et al.Nucl.Phys.,2000,B577:88;Eberl H et al.Phys.Rev.,2000,D62:05500619. ZHU S H .hep- ph/011210920.'t Hooft G ,Veltman M .Nucl.Phys.,1979,B153:365;Passarino G ,Veltman M .Nucl.Phys.,1979,B160:151
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Get Citation
WAN Ling-De, LU Gong-Ru and GAO Guang-Ping. gb→tH One Loop SUSY-QCD Corrections and Nondecoupling Effects[J]. Chinese Physics C, 2003, 27(3): 189-195.
WAN Ling-De, LU Gong-Ru and GAO Guang-Ping. gb→tH One Loop SUSY-QCD Corrections and Nondecoupling Effects[J]. Chinese Physics C, 2003, 27(3): 189-195. shu
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Received: 2002-06-25
Revised: 1900-01-01
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gb→tH One Loop SUSY-QCD Corrections and Nondecoupling Effects

    Corresponding author: WAN Ling-De,
  • The Physics Department of Hannan Normal University, Xinxiang 453002, China

Abstract: In this paper one loop SUSY QCD radiative correction to gb→tHcross section is calculated in the context of Minimal Supersymmetric Standard Model. We found that non decoupling effects of SUSY QCD will occur if the gluino mass and the SUSY soft breaking parameter μ or At,Ab are at the same order and get large. The non decoupling contribution can be enhanced by large tan β and therefore large corrections to the hadronic production rates at the Tevatron and LHC are expected in the large tan β limit. The fundamental reason for such non decoupling behavior is found to be some couplings in the loops being proportional to SUSY mass parameters.

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