The Standard Model inclusive Higgs
cross section is known at
LO,
NLO
and
NNLO.
The Higgs
tranverse momentum distribution has been calculated to to
NNLO+NNLL.
The link
to the discussion of Higgs production in CHS can be found
here.
The cross section for Higgs production at NLO, using CTEQ6M pdfs,
as a function of its mass is shown below. The largest production
mechanism is gg fusion, through a top quark loop. The branching ratios
for the Standard Model Higgs decay, as a function of its mass are also
shown below.
The kinematics for Higgs production are an important component for LHC
searches. A comparison of various predictions for the Higgs transverse
momentum
distribution (for the gg subprocess) are shown below. The Higgs pT
distribution peaks
significantly higher than does the similar distribution for the Z boson
due to the larger color factor for the
initial state gluons and to the differences between the gluon and quark
splitting functions. The parton shower Monte Carlos do a reasonable job
in describing the shape of the pT
distribution, but not its normalization.
A link to the ResBos program for calculation of Higgs kinematics can be
found here.
The cross section for the production
of a 120 GeV Higgs is shown at LO, NLO and NNLO below. There is a
significant K-factor in going from LO to NLO, with a smaller additional
normalization from NLO to NNLO. The K-factor is essentially independent
of the Higgs rapidity.The scale dependence of the cross section is also
shown in the figure on the right.
As part of the CTEQ4LHC exercise,
Higgs cross sections were generated for the LHC using the following
standard parameters:
PDFs: CTEQ6.6, CTEQ6L1, CTEQ modified LO pdf's
Order of calculations: LO, NLO, NNLO, NNLO+NNLL
.
.
.
Total cross section predictions for the gg subprocess are shown in the
table below, at NLO and LO, with scales of mHiggs and mHiggs/2 and with
cteq6.6, cteq6l1 and modified LO pdf's. The relevant K-factor (NLO/LO
is shown in parentheses next to the LO cross section. The calculations
were performed with
MCFM.
order
|
NLO
|
NLO
|
LO
|
LO
|
LO
|
LO
|
LO
|
LO
|
PDF
|
cteq6.6
|
cteq6.6
|
cteq6.6
|
cteq6.6
|
cteq6l1
|
cteq6l1
|
mod LO
|
mod LO
|
scale
|
mHiggs
|
mHiggs/2
|
mHiggs
|
mHiggs/2
|
mHiggs
|
mHiggs/2
|
mHiggs
|
mHiggs/2
|
sigma (fb) mHiggs=120 GeV
|
36340
|
42455
|
15830 (2.30)
|
18190 (2.43)
|
|
|
|
|
sigma (fb) mHiggs=200 GeV
|
12815
|
15020
|
5865 (2.18)
|
|
|
|
|
|
sigma (fb) mHiggs=300 GeV
|
5070
|
5955
|
2395 (2.12)
|
2925 (2.04)
|
|
|
|
|
sigma (fb) mHiggs=400 GeV
|
|
|
|
|
|
|
|
|
Here are some cross section plots for production of a 120 GeV mass
Higgs through gg fusion.
Here is a cross section table for the rapidity distribution for a 120
GeV Higgs. Ultimately, this will be linkable, rather than appearing on
the main page.
order
|
NLO
|
NLO
|
LO
|
LO
|
LO
|
LO
|
LO
|
LO
|
PDF
|
cteq6.6
|
cteq6.6
|
cteq6.6
|
cteq6.6
|
cteq6l1
|
cteq6l1
|
mod LO
|
mod LO
|
scale
|
120 GeV
|
60 GeV
|
120 GeV
|
60 GeV
|
120 GeV
|
60 GeV
|
120 GeV
|
60 GeV
|
|y| range
|
sigma(fb)
|
sigma(fb)
|
sigma(fb)
|
sigma(fb)
|
|
|
|
|
0.0-0.2
|
3.41E3
|
3.93E3
|
1.47E3
|
1.67E3
|
|
|
|
|
0.2-0.4
|
3.37E3
|
3.96E3
|
1.46E3
|
1.66E3
|
|
|
|
|
0.4-0.6
|
3.29E3
|
3.90E3
|
1.43E3
|
1.62E3
|
|
|
|
|
0.6-0.8
|
3.23E3
|
3.71E3
|
1.38E3
|
1.58E3
|
|
|
|
|
0.8-1.0
|
3.10E3
|
3.49E3
|
1.32E3
|
1.51E3
|
|
|
|
|
1.0-1.2
|
2.80E3
|
3.43E3
|
1.26E3
|
1.44E3
|
|
|
|
|
1.2-1.4
|
2.70E3
|
3.08E3
|
1.17E3
|
1.34E3
|
|
|
|
|
1.4-1.6
|
2.52E3
|
3.08E3
|
1.08E3
|
1.24E3
|
|
|
|
|
1.6-1.8
|
2.21E3
|
2.38E3
|
9.78E2
|
1.13E3
|
|
|
|
|
1.8-2.0
|
2.02E3
|
2.47E3
|
7.58E2
|
1.01E3
|
|
|
|
|
2.0-2.2
|
1.71E3
|
2.01E3
|
6.49E2
|
8.78E2
|
|
|
|
|
2.2-2.4
|
1.49E3
|
1.73E3
|
5.36E2
|
7.53E2
|
|
|
|
|
2.4-2.6
|
1.21E3
|
1.41E3
|
4.30E2
|
6.26E2
|
|
|
|
|
2.6-2.8
|
9.80E2
|
1.18E3
|
3.37E2
|
5.04E2
|
|
|
|
|
2.8-3.0
|
7.49E2
|
8.50E2
|
2.51E2
|
3.95E2
|
|
|
|
|
3.0-3.2
|
5.58E2
|
6.88E2
|
1.80E2
|
2.98E2
|
|
|
|
|
3.2-3.4
|
4.16E2
|
4.81E2
|
1.20E2
|
2.13E2
|
|
|
|
|
3.4-3.6
|
2.54E2
|
3.08E2
|
7.47E1
|
1.45E2
|
|
|
|
|
3.6-3.8
|
1.69E2
|
2.01E2
|
4.26E1
|
9.15E1
|
|
|
|
|
3.8-4.0
|
8.97E1
|
1.03E2
|
2.07E1
|
5.36E1
|
|
|
|
|
4.0-4.2
|
4.58E1
|
6.02E1
|
7.51E0
|
2.73E1
|
|
|
|
|
4.2-4.4
|
1.77E1
|
2.16E1
|
1.36E0
|
1.06E1
|
|
|
|
|
4.4-4.6
|
3.40E0
|
4.29E0
|
2.59E-2
|
2.10E0
|
|
|
|
|
4.6-4.8
|
7.19E-2
|
1.18E-1
|
|
|
|
|
|
|
ROOT ntuples for each of the predictions above can be found below,
along with a sample ROOT analysis
script.
Since the ntuples may be quite large, we'll have to find the best way
of making
them available.
order
|
NLO
|
NLO
|
LO
|
LO
|
LO
|
LO
|
LO
|
LO
|
PDF
|
cteq6.6
|
cteq6.6
|
cteq6.6
|
cteq6.6
|
cteq6l1
|
cteq6l1
|
mod LO
|
mod LO
|
scale
|
mHiggs
|
mHiggs/2
|
mHiggs
|
mHiggs/2
|
mHiggs
|
mHiggs/2
|
mHiggs
|
mHiggs/2
|
mHiggs=120 GeV
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
mHiggs=200 GeV
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
mHIggs=300 GeV
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
mHiggs=400 GeV
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
ntuple
|
Here we can link to pages on other Higgs cross section programs,
VBF production, Higgs + 1 jet, Higgs +
2 jets, etc.
Higgs physics on the back
of an envelope
Estimating the cross sections and related quantities for Higgs
production does not necessarily require running programs. Estimates
accurate to within a few tens of percent should be possible with
'back-of-the-envelope' types of calculations. The pdf luminosity
plots for the LHC are shown below. The gg luminosity is given by the
blue curve. The LO cross section for Higgs production is shown below to
the right.
For example, for a Higgs mass of 120 GeV, the gg pdf luminosity is
~1E7pb. The Higgs sub-process cross section (at LO) at 120 GeV is 2E-06
pb, leading to a prediction for the Higgs cross section of 20 pb. The
K-factor for Higgs production at the LHC can be read from the table
below as 2.3 leading to a prediction at NLO as 46 pb, in agreement with
the plot showon at the top of the page.
The pdf luminosity for Higgs production through gg production can be
estimated from the figure below. For low mass Higgs production, the pdf
uncertainty is less than 5%. The pdf correlations are shown on the
lower right. Here we might also make available some pdf correlation
tools.
The initial state Sudakov form factor for one of the gluons producing
the Higgs can be read from the plot shown below. The Sudakov form
factors (for Q=100 GeV) are for x values of (top to bottom)
0.3,0.1,0.03,0.01, 0.001,0.0001. Production of a low mass Higgs
involves initial state gluons with x values on the order of 0.01 (the
purple curve). The Sudakov form factor for emitted
gluons on the order of 20 GeV is ~0.7, i.e. there is a probability of
0.3 of emitting such a gluon. The probability of neither initial state
gluon emitting a gluon of 20 GeV or greater is
0.7*0.7, or ~0.5. Using Poisson statistics, the average jet
multiplicity (for transverse momenta > 20 GeV) is 0.7.