Search for a light pseudoscalar Higgs boson in the dimuon decay channel in pp collisions at sqrt{s} = 7 TeV
Published in Physical Review Letters
http://cds.cern.ch/record/1458514?ln=en
What follows is a condensed description with plots for the analysis CMS-HIG-12-004
Abstract
The dimuon invariant mass spectrum is investigated in the mass range between 5.5
GeV and 14
GeV using 1.3 fb
-1 of pp collision data at a center of mass energy of 7
TeV collected by the CMS detector at the LHC to search for a light pseudoscalar Higgs boson. Such a light Higgs boson is predicted in many models, including the Next-to-Minimal Supersymmetric Standard Model (NMSSM) which avoids the m-term problem of the MSSM. A limit on the cross section times branching ratio

is set.
Main Results
We perform a search for a narrow, low mass, pseudoscalar a which is produced by

and decays via

in the mass ranges 5.5-8.8
GeV and 11.5-14
GeV, using a data sample corresponding to 1.3 fb
-1 collected with the CMS detector. Given the good agreement with SM background predictions, we set upper limits on the cross section times branching ratio of

in the mass ranges considered. These upper limits are applied in the context of the light pseudoscalar a
1 of the NMSSM to yield upper limits on the NMSSM parameter

, which specifies the fraction by which the a
1 overlaps the MSSM doublet Higgs fields at the amplitude level. These limits are superior to those from
BaBar for a significant portion of the

mass range, and are the only limits available in the

mass range.
Figures from the publication. They can/should be used in talks:
-- Maxwell Chertok Nov. 21, 2013
Figures from CMS-HIG-12-004
PAS Figure |
Image |
File |
Description |
Figure 1a |
|
pdf, png |
Feynman diagram for the production mechanism |
Figure 1b |
|
pdf, png |
Cross section for production at s = 7 TeV for = 1, 2, 3, 10, 30, 50. We plot the cross section including all available higher order corrections as per HIGLU, especially those from resolvable parton final state contributions ( ) |
Figure 2a |
|
pdf, png |
Dimuon invariant mass distribution for the central region after the optimization of the cuts for the background reduction. The invariant mass distributions are fitted (red curves) accounting for the three bottomonium resonances and QCD background |
Figure 2b |
|
pdf, png |
Dimuon invariant mass distribution for the endcap region after the optimization of the cuts for the background reduction. The invariant mass distributions are fitted (red curves) accounting for the three bottomonium resonances and QCD background |
Figure 3a |
|
pdf, png |
Invariant mass spectrum in the barrel region (y-axis zoom) |
Figure 3b |
|
pdf, png |
Invariant mass spectrum in the endcap region (y-axis zoom) |
Figure 4a |
|
pdf, png |
Upper limit for mass range 1 |
Figure 4b |
|
pdf, png |
Upper limit for mass range 2 |
Figure 5 |
|
pdf, png |
Upper limit for . For each value in mass range 1 there is a second dotted curve that shows the limits from the BaBar analyses. |
--
MarioPelliccioni - 01-Mar-2012