This site uses cookies. By continuing to use this site you agree to our use of cookies. To find out more, see our Privacy and Cookies policy.
Brought to you by:
CORRIGENDUM The following article is Free article

Pair production of charged Higgs bosons in gluon - gluon collisions

, , , and

Published under licence by IOP Publishing Ltd
, , Citation Jiang Yi et al 1997 J. Phys. G: Nucl. Part. Phys. 23 1151 DOI 10.1088/0954-3899/23/9/016

0954-3899/23/9/1151

Abstract

Equation (6) of the published paper should read:

and equation (9) should be

In the appendix, the following two equations should replace factors and in equations (A.3) and (A.5), respectively.

The other form factors in the appendix remain unchanged. Because of the above changes, figures 2, 3, 4 and 5 of the published article should be replaced by the following ones:

 

Figure 2. ( a) Total cross sections of the subprocess gg → H+H- as functions of with GeV, GeV and GeV. The full curve is for tan β = 1.5, the dashed curve is for tan β = 30. ( b) Total cross sections of the subprocess gg → H+H- as functions of with GeV, GeV and GeV. The full curve is for tan β = 1.5, the dashed curve for tan β = 30.

 

Figure 3. Total cross sections of the subprocess gg → H+H- as functions of tan β with GeV, GeV and GeV. The full and dashed curves correspond to GeV and GeV, respectively.

 

Figure 4. Total cross sections of the subprocess gg → H+H- as functions of with GeV, GeV and TeV. The full curve is for tan β = 1.5, the dashed curve for tan β = 30.

 

Figure 5. ( a) Total cross sections of the process PP → gg → H+H- + X as functions of with GeV, GeV and GeV. The full curve is for tan β = 1.5, the dashed curve for tan β = 30. ( b) Total cross sections of the process PP → gg → H+H- + X as functions of with GeV, GeV and GeV. The full curve is for tan β = 1.5, the dashed curve for tan β = 30.

Export citation and abstract BibTeX RIS

10.1088/0954-3899/23/9/016