메뉴 건너뛰기




Volumn 35, Issue 1, 1987, Pages 173-178

Pair production of supersymmetric charged Higgs bosons

Author keywords

[No Author keywords available]

Indexed keywords


EID: 0000573936     PISSN: 05562821     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevD.35.173     Document Type: Article
Times cited : (71)

References (39)
  • 15
    • 84927843764 scopus 로고    scopus 로고
    • Note that Eq. (5.2) of Ref. 8 contains several errors;
  • 16
    • 84927843763 scopus 로고    scopus 로고
    • the above reference gives the correct expression.
  • 17
    • 84927843762 scopus 로고    scopus 로고
    • E. Eichten, I. Hinchliffe, K. Lane, and C. Quigg, in Proceedings of the 1984 DPF Summer Study on the Design and Utilization of the Superconducting Super Collider, edited by Rene Donaldson and Jorge G. Morfin (Fermilab, Batavia, IL, 1984), p.99.
  • 18
    • 84927843761 scopus 로고    scopus 로고
    • These curves agree qualitatively with those given in Fig. 7 of Ref. 10, where a rapidity cut | y | < 1.5 has been imposed on the produced particles.
  • 19
    • 84927843760 scopus 로고    scopus 로고
    • This process was proposed in Refs. 8 and 10, where it is correctly stated that gluon fusion is negligible if there do not exist sufficiently heavy quarks.
  • 20
    • 84927843759 scopus 로고    scopus 로고
    • Not all of the Feynman diagrams are shown. Figure 1(b) must be added to a diagram with the gluon lines crossed. Figure 1(c) is only one of six box diagrams which contribute to the amplitude. If the particle in the loop is a scalar quark, there are additional diagrams involving the quartic gluon–gluon–scalar-quark–anti-scalar-quark coupling.
  • 22
    • 84927843758 scopus 로고    scopus 로고
    • It is interesting to note that C conservation (called Furry's theorem in this context) forbids the coupling of two gluons to a photon via quark and scalar-quark loops and to a Z boson via a scalar-quark loop. The only non-vanishing coupling of two gluons to a vector boson is due to the axial-vector coupling of the Z boson to quarks.
  • 25
    • 84927843757 scopus 로고    scopus 로고
    • This agrees with Eq. (14) of Ref. 16, when we include a factor of 2 from inserting both left- and right-handed scalar quarks in the loop.
  • 29
    • 84927843756 scopus 로고    scopus 로고
    • As an intermediate step in our calculation we have verified the result given in Eq. (19) of Ref. 16 for the large-mass limit of the box diagram with two vector and two scalar couplings.
  • 30
    • 84927843755 scopus 로고    scopus 로고
    • A more precise statement of unitarity is that partial-wave amplitudes cannot grow at arbitrarily high energies. The amplitude derived from the interaction H+H-Fμν Fμν is pure s wave and grows like s hat, in violation of unitarity.
  • 31
    • 84927843754 scopus 로고    scopus 로고
    • It is also possible that very heavy quarks could alter the spectrum of the standard model. We thank W. Fischler for bringing this point to our attention.
  • 34
    • 84927843753 scopus 로고    scopus 로고
    • There are also loop diagrams involving the quartic H+H-ndashscalar-quark–anti-scalar-quark coupling, but these vanish in the large-mass limit.
  • 35
    • 84927843752 scopus 로고    scopus 로고
    • This agrees with the result given in Eq. (19) of Ref. 16, when we include a factor of 2 from inserting both left- and right-handed scalar quarks in the loop.
  • 37
    • 84927843750 scopus 로고    scopus 로고
    • H. E. Haber, in Supercollider Physics, proceedings of the Oregon Workshop on Super High Energy Physics, edited by Davison E. Soper (World Scientific, Singapore, 1986), p. 194.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.