Higgs-Boson Production in Association with Heavy Quarks
ABSTRACT Associated production of a Higgs boson with a heavy, i.e. top or bottom, quark-anti-quark pair provide observation channels for Higgs bosons at the LHC which can be used to measure the respective Yukawa couplings. For the light supersymmetric Higgs boson we present SUSY-QCD corrections at the one-loop level, which constitute a significant contribution to the cross section.
- SourceAvailable from: arxiv.org[Show abstract] [Hide abstract]
ABSTRACT: Higgs-boson production in association with bottom quarks is an important discovery channel for supersymmetric Higgs particles at hadron colliders for large values of tan(beta). We present the complete O(alpha) electroweak and O(alpha_s) strong corrections to associated bottom-Higgs production through bb fusion in the MSSM and improve this next-to-leading-order prediction by known two-loop contributions to the Higgs self-energies, as provided by the program FeynHiggs. Choosing proper renormalization and input-parameter schemes, the bulk of the corrections (in particular the leading terms for tan(beta)) can be absorbed into an improved Born approximation. The remaining non-universal corrections are typically of the order of a few per cent. Numerical results are discussed for the benchmark scenarios SPS 1b and SPS 4. Comment: 24 pages, 5 figures, LaTex, 1 figure added, reference added, version published in JHEPJournal of High Energy Physics 11/2006; · 5.62 Impact Factor
Article: (SUSY) Higgs Search at the LHC[Show abstract] [Hide abstract]
ABSTRACT: The discovery of the Standard Model (SM) or supersymmetric (SUSY) Higgs bosons belongs to the main endeavors of the Large Hadron Collider (LHC). In this article the status of the signal and background calculations for Higgs boson production at the LHC is reviewed.11/2008;
- [Show abstract] [Hide abstract]
ABSTRACT: In models with an enhanced coupling of the Higgs boson to the bottom quark, the dominant production mechanism in hadronic collisions is often the partonic sub-process, bg ->bH. We derive the weak corrections to this process and show that they can be accurately approximated by an "Improved Born Approximation". At the Tevatron, these corrections are negligible and are dwarfed by PDF and scale uncertainties for M_H < 200 GeV. At the LHC, the weak corrections are small for M_H < 500 GeV. For large Higgs boson masses, the corrections become significant, and are ~18% for M_H ~ 1 TeV at E_CM=10 TeV. Comment: 25 pages, discussion of PDF uncertainties added. Version accepted for publication in Phys. Rev. D.Physical review D: Particles and fields 02/2010;
arXiv:hep-ph/0610340v1 25 Oct 2006
Higgs-Boson Production in Association with
Wolfgang Hollik∗and Michael Rauch†
∗Max-Planck-Institut für Physik, München, Germany
†School of Physics, SUPA, University of Edinburgh, Scotland, UK
Abstract. Associated production of a Higgs boson with a heavy, i.e. top or bottom, quark–anti-
quark pair provideobservationchannels for Higgs bosons at the LHC which can be used to measure
the respectiveYukawacouplings.Forthe lightsupersymmetricHiggsbosonwe presentSUSY-QCD
corrections at the one-loop level, which constitute a significant contribution to the cross section.
Higgs-boson Yukawa couplings to fermions are proportional to the fermion masses and
hence are very small for the light quarks, u, d, s and c. In contrast, the top-quark mass is
of thesame order as the Higgs vacuum expectation value, leading to a top-quark Yukawa
couplingcloseto 1. Thebottom-quarkmass also leads to a rather weak Yukawacoupling
in the Standard Model. In the Minimal Supersymmetric Standard Model (MSSM), the
coupling to the lighter CP-even neutral Higgs boson h0can be enhanced for large values
of tan(β), the ratio of the two vacuum expectation values. Such large Yukawa couplings
make Higgs-boson production in association with heavy quarks  a phenomenologi-
cally interesting process. At O?α2
quark lines; the cross section is thus sensitive to the Yukawa coupling and can be used
to measure the respective Yukawa coupling. A precise determination requires to include
at least the next-order QCD corrections. Here we present for the case of MSSM Higgs
bosons the results from a calculation of the SUSY-QCD corrections, supplementing the
standard QCD corrections by the loop contributions with virtual gluinos and squarks.
sα?, the Higgs boson is emitted off one of the heavy-
The production of a Higgs boson in association with a bottom quark–anti-quark pair
was intensively studied in the literature [2, 3]. The analysis was soon extended [4, 5]
to include the lightest MSSM-Higgs boson h0. The diagram types are exactly the same
as in the Standard Model case; only the bottom-quark–Higgs coupling is changed to
its supersymmetric counterpart. The standard QCD corrections  to this process are
already known and reduce the dependence of the cross section on the factorization
and renormalization scales. The final-state bottom quarks are required to be explicitly
observed in the detector via b-tagging, in contrast to inclusive processes  without
b-tagging. Therefore, a transverse-momentum cut on the bottom-quark jets, typically
pT≥ 20 GeV, is applied. The additional cuts reduce the cross section by one or two
orders of magnitude, but also greatly reduce the background and ensure that the Higgs
boson was emitted from a bottom quark and is therefore proportional to the square of
the b-quark Yukawa coupling.
Here we concentrate on the SUSY-QCD corrections with squarks and gluinos in the
loops. Part of these corrections were already calculated in ref. . There an effective
b¯bh0-coupling was used which includes the one-loop vertex corrections, but no box-type
or pentagon diagrams were added in their analysis. We have performed a full one-loop
calculation of the SUSY-QCD corrections.
In certain regions of the MSSM parameter space a large contribution to the SUSY-
QCD corrections originates from the effective coupling of the bottom quark to the sec-
ond Higgs doublet. This changes the relation between bottom-quark mass and Yukawa
coupling and the additional contribution is commonly referred to as ∆bin the litera-
ture . It is proportional to tan(β) and represents for large values of tan(β) the dom-
inant supersymmetric correction. If the ∆b-contribution is compared with full one-loop
results it is necessary to include it only to one-loop order as well and not use any re-
summed version, resulting in the replacement
which has been used when calculating ∆b-corrected tree-level cross sections.
In order to assess the relative differences between cross sections the following quan-
tities have been defined. The relative one-loop correction is given as
where σ0denotes the tree-level cross section and σ1the one-loop one including SUSY-
QCD corrections. Additionally,a ∆b-corrected tree-level cross section σ∆was calculated
by using the replacement of eq. (1) and treating the ∆bterm as a one-loop contribution.
Additionally, the contribution to the vertex from the term proportional to the second
mixing angle in the MSSM-Higgs sector, α, was included in σ∆according to ref. [4, 9,
10]. The relative correction using only these contributions is defined as
The Feynman diagrams were generated using FeynArts , the matrix elements
calculated by FormCalc  and the loop integrals numerically evaluated by Loop-
Tools . The convolution with the parton distribution functions was performed with
HadCalc  using the PDF set of ref. .
The left-hand side of Table 1 contains the individual contributions from the various
partonic processes to the hadronic process pp → b¯bh0and their sum, for the MSSM ref-
erence point SPS1a′. The gluon-fusion process clearly dominates the total hadronic
cross section. This is because for the quark–anti-quark annihilation diagrams only an s-
channel topology exists, which is propagator-suppressed. For the gluon-fusion diagrams
d¯d → b¯bh0
u¯ u → b¯bh0
s¯ s → b¯bh0
c¯ c → b¯bh0
gg → b¯bh0
pp → b¯bh0
Hadronic cross sections for b¯bh0and t¯ th0production at the parameter point SPS1a′.
d¯d → t¯ th0
u¯ u →t¯ th0
s¯ s → t¯ th0
c¯ c → t¯ th0
gg →t¯ th0
pp → t¯ th0
there is an additional t-channel diagram which does not suffer from such a suppression.
Additionally one can see that the ∆b-corrected tree-level cross section accounts only for
less than half of the total SUSY-QCD corrections for this parameter point, and therefore
a full calculation is necessary to determine the size of the additional contribution. The
details of this additional contribution will be discussed in a future publication .
The production of a Higgs boson in association with a top quark–anti-quark pair 
proceeds in the same way as the one with a bottom quark–anti-quark pair and the same
Feynman diagrams appear, where the bottom-quark line is replaced by a top-quark line.
The standard QCD corrections to this process are also available in the literature .
A calculation of the SUSY-QCD corrections was performed recently in ref. . As
the figures of this article include both standard and SUSY-QCD contributions a direct
comparison of the numerical results is difficult. The principal behavior when varying
MSSM parameters agrees. Our calculation was performed using the same tools as
mentioned beforehand in the bottom-quark case. No cuts were applied to the final state.
On the right-hand side of Table 1 the results for the MSSM parameter point SPS1a′
are presented. In this case the gluon-fusion contribution is still the dominant one, but
also the quark–anti-quark–annihilation subprocesses reach a significant size and cannot
be neglected any more. This is because to produce the final state a higher center-of-mass
energy than for bottom quarks is needed. The rapid decrease of the gluon density in
the proton with growing momentum fraction x partly cancels the effect of the s-channel
propagator suppression in quark–anti-quark annihilation. We find that the total size of
the SUSY-QCD corrections is of the order of several percent.
Higgs-boson production in association with heavy, i.e. bottom or top, quarks is an
important way to measure the respective Yukawa couplings. In the MSSM besides
the standard QCD corrections also SUSY-QCD corrections appear. They modify the
total cross section significantly and should be taken into account to extract the Yukawa
coupling precisely from future experimental data.
We would like to thank T Plehn for careful reading of the manuscript. The work of MR
was supported by the Scottish Universities Physics Alliance (SUPA).
1.R. Raitio, and W. W. Wada, Phys. Rev. D19, 941 (1979); A. S. Bagdasaryan, R. S. Egorian, S. G.
Grigorian, and S. G. Matinyan, Sov. J. Nucl. Phys. 46, 315 (1987); J. N. Ng, and P. Zakarauskas,
Phys. Rev. D29, 876 (1984).
ATL-PHYS-2003-024; S. Cucciarelli et al., CERN-CMS-NOTE-2006-119.
D. A. Dicus, and S. Willenbrock, Phys. Rev. D39, 751 (1989); J. Campbell, et al. (2004),
M. Carena, S. Mrenna, and C. E. M. Wagner, Phys. Rev. D60, 075010 (1999), hep-ph/9808312.
Z.Kunszt,and F. Zwirner,Nucl. Phys. B385,3–75(1992),hep-ph/9203223; J. Dai, J. F. Gunion,
and R. Vega, Phys. Lett. B345, 29–35 (1995), hep-ph/9403362, Phys. Lett. B387, 801–803
(1996), hep-ph/9607379; E. Richter-Was, and D. Froidevaux, Z. Phys. C76, 665–676 (1997),
hep-ph/9708455; J. L. Diaz-Cruz, H.-J. He, T. Tait, and C. P. Yuan, Phys. Rev. Lett. 80, 4641–
4644 (1998), hep-ph/9802294; C. Balazs, J. L. Diaz-Cruz, H. J. He, T. Tait, and C. P. Yuan,
Phys. Rev. D59, 055016 (1999), hep-ph/9807349.
C. Balazs, H.-J. He, and C. P. Yuan, Phys. Rev. D60, 114001(1999),hep-ph/9812263; D. Dicus,
T. Stelzer, Z. Sullivan, and S. Willenbrock, Phys. Rev. D59, 094016 (1999), hep-ph/9811492;
S. Dittmaier, M. Kramer, and M. Spira, Phys. Rev. D70, 074010 (2004), hep-ph/0309204;
S. Dawson, C. B. Jackson, L. Reina, and D. Wackeroth, Phys. Rev. D69, 074027 (2004),
hep-ph/0311067, (2005), hep-ph/0508293.
R. V. Harlander and W. B. Kilgore, Phys. Rev. D68, 013001 (2003), hep-ph/0304035.
G. Gao, R. J. Oakes, and J. M. Yang, Phys. Rev. D71, 095005 (2005), hep-ph/0412356.
M. Carena, M. Olechowski, S. Pokorski and C. E. M. Wagner, Nucl. Phys. B426, 269–300 (1994),
hep-ph/9402253; L. J. Hall, R. Rattazzi and U. Sarid, Phys. Rev. D50, 7048–7065 (1994),
hep-ph/9306309; M. Carena, D. Garcia, U. Nierste, and C. E. M. Wagner, Nucl. Phys. B577,
88–120 (2000), hep-ph/9912516; J. Guasch, W. Hollik, and S. Penaranda, Phys. Lett. B515,
367–374(2001), hep-ph/0106027; J. Guasch, P. Hafliger, and M. Spira, Phys. Rev. D68, 115001
10. M. Carena, S. Mrenna, and C. E. M. Wagner, Phys. Rev. D62, 055008 (2000), hep-ph/9907422.
11. J. Kublbeck, M. Bohm, and A. Denner, Comput. Phys. Commun. 60, 165–180 (1990).
12. T.Hahn,andM. Perez-Victoria,
13. T. Hahn, and M. Rauch, Nucl. Phys. Proc. Suppl. 157, 236–240 (2006), hep-ph/0601248.
14. M. Rauch, PhD thesis, (2006), urn:nbn:de:bvb:91-diss20060502-1522300621.
15. A. D. Martin, R. G. Roberts, W. J. Stirling, and R. S. Thorne, Eur. Phys. J. C28, 455–473 (2003),
16. J. A. Aguilar-Saavedra, et al. (2005), hep-ph/0511344.
17. W. Hollik, M. Rauch, (in preparation).
18. Z. Kunszt, Nucl. Phys. B247, 339 (1984);W. J. Marciano, and F. E. Paige, Phys. Rev. Lett. 66, 2433–
2435 (1991); J. F. Gunion, Phys. Lett. B261, 510–517(1991); J. Goldstein, et al., Phys. Rev. Lett. 86,
19. W. Beenakker, et al., Phys. Rev. Lett. 87, 201805 (2001), hep-ph/0107081, Nucl. Phys. B653,
151–203(2003),hep-ph/0211352; L. Reina, and S. Dawson,Phys. Rev.Lett. 87, 201804(2001),
hep-ph/0107101; S. Dawson, L. H. Orr, L. Reina, and D. Wackeroth, Phys. Rev. D67, 071503
20. W. Peng, et al. (2005), hep-ph/0505086.
2. J.Cammin, andM. Schumacher,