2013-05-22
22:44 |
Search for RPV SUSY in the four-lepton final state
/CMS Collaboration
We present a search for anomalous production of events with four isolated leptons in $19.5\,\text{fb}^{\text{$-$1}}$ of data collected by the CMS experiment in $pp$ collisions at $\sqrt{s}$ = 8 TeV. No excess of events is observed over the standard model background. [...]
CMS-PAS-SUS-13-010.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_001-d: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004-a: PNG; Figure_004-b: PNG; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_007-c: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_014-a: PDF; Figure_014-b: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-22
16:12 |
Search for baryon number violating top quark decays in pp collisions at 8 TeV
/CMS Collaboration
A search for the decay of top quarks that violate baryon number conservation
is performed using pp collisions produced by the LHC at $\sqrt{s}=8$
TeV. The top quark decay signature considered in this analysis
consists of one light lepton (electron or muon), two jets, but no
neutrino in the final state. [...]
CMS-PAS-B2G-12-023.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-22
16:10 |
Prompt psi(2S) polarization in pp collisions at 7 TeV
/CMS Collaboration
The polarization of prompt $\psi$(2S) mesons is
measured in proton-proton collisions at $\sqrt{s} = 7\,$TeV, using a data sample
of $\psi\mathrm{(2S)} \rightarrow \mu^+\mu^-$ decays collected by the CMS experiment,
corresponding to an integrated luminosity of 4.9$\,$fb$^{-1}$.
The dimuon decay angular distributions are analysed in three different
polarization frames. The prompt $\psi$(2S) polarization parameters $\lambda_\vartheta$,
$\lambda_\varphi$, and $\lambda_{\vartheta\varphi}$, as well as the frame-invariant
$\tilde{\lambda}$, are measured as a function of the $\psi$(2S) transverse
momentum, $p_{\rm T}$, between 14 and 50$\,$GeV, in the rapidity ranges $|y|<0.6$ and $0.6<|y|<1.2$.
No evidence of large transverse or longitudinal polarizations is seen in the
explored kinematic region..
CMS-PAS-BPH-13-003.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-19
22:15 |
Upsilon(1S), Upsilon(2S) and Upsilon(3S) cross section measurements in pp collisions at sqrt(s) = 7 TeV
/CMS Collaboration
The differential cross section as a function of transverse momentum for the production of the $\Upsilon(nS)$ ($n$=1,2,3) states decaying into a pair of muons has been measured in pp collisions at $\sqrt{s}$ = 7 TeV using 4.9 fb$^{-1}$ of data collected by the CMS detector. The analysis selected events with dimuon rapidity $|y(\mu\mu)|< 0.6$, and the measurements cover dimuon transverse momentum in the range $p_T(\mu\mu)=$10-100 GeV. [...]
CMS-PAS-BPH-12-006.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-18
10:48 |
Measurement of diffraction dissociation cross sections at sqrt(s)=7 TeV at the LHC
/CMS Collaboration
Results are presented for the single- and double-diffractive cross sections in pp collisions at $\sqrt{s}=7$ TeV at the LHC using the CMS detector. The differential SD cross section is measured as a function of $\xi$, the forward momentum loss of the incoming proton, for $-5.5<\log_{10}\xi<-2.5$. [...]
CMS-PAS-FSQ-12-005.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_010: PDF; Figure_011: PDF; Figure_012: PDF; Figure_013: PDF; Figure_014: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_015-c: PDF; Figure_015-d: PDF; Figure_016: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-17
12:28 |
Search for RPV SUSY resonant second generation slepton production in same-sign dimuon events at sqrt(s) = 7 TeV
/CMS Collaboration
A search for resonant production of second generation sleptons ($\tilde{\mu}$,
$\tilde{\nu}_{\mu}$) via the R-parity violating coupling $\lambda'_{211}$,
with two same-sign muons and at least two jets in the final state is
performed. While one muon is expected to be produced directly in the slepton
decay, the second muon and at least two jets are produced in the subsequent
decay of a neutralino or chargino originating from the resonant slepton. [...]
CMS-PAS-SUS-13-005.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-16
23:14 |
Measurement of the double-differential inclusive jet cross
section at sqrt(s) = 8 TeV with the CMS detector
/CMS Collaboration
% A measurement of the inclusive jet cross section, double-differential in jet transverse momentum $p_\mathrm{T}$ and absolute jet rapidity $|y|$, is presented. Data from LHC proton-proton collisions at $\sqrt{s}=8\TeV$, corresponding to an integrated luminosity of $10.71\,\mathrm{fb}^{-1}$, have been collected with the CMS detector [...]
CMS-PAS-SMP-12-012.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_002-d: PDF; Figure_002-e: PDF; Figure_002-f: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_003-e: PDF; Figure_003-f: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_004-e: PDF; Figure_004-f: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_005-d: PDF; Figure_005-e: PDF; Figure_005-f: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: PDF; Figure_006-e: PDF; Figure_006-f: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_007-c: PDF; Figure_007-d: PDF; Figure_007-e: PDF; Figure_007-f: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_008-e: PDF; Figure_008-f: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_009-c: PDF; Figure_009-d: PDF; Figure_009-e: PDF; Figure_009-f: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_010-d: PDF; Figure_010-e: PDF; Figure_010-f: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_011-c: PDF; Figure_011-d: PDF; Figure_011-e: PDF; Figure_011-f: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-16
18:03 |
Higgs to bb in the VBF channel
/CMS Collaboration
A search for the standard model Higgs boson in the vector boson fusion production channel with decay to bottom quarks is reported. A data sample comprising 19.0~fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=8$~TeV collected during the 2012 running period has been analyzed and 95\% Confidence Level upper limits are derived for five mass points from 115 to 135 GeV. [...]
CMS-PAS-HIG-13-011.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_009: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-16
15:35 |
Search for supersymmetry in the 3 lepton + b-tag final state
/CMS Collaboration
Results are reported from a search for new physics processes in events with three leptons and at least one b-tagged jet. The analysis is based on a sample of proton-proton collisions at a center-of-mass energy of 8 TeV with an integrated luminosity of 19.5/fb, collected by the CMS detector at the LHC. [...]
CMS-PAS-SUS-13-008.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_011-c: PDF; Figure_012: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
2013-05-16
15:03 |
Search for top-squark pair production in the single lepton final state in pp collisions at 8 TeV
/CMS Collaboration
This report presents a search for the pair production of top squarks in events with a single isolated electron or muon, jets, large missing transverse energy, and large transverse mass.
The data sample corresponds to an integrated luminosity of
$19.5$ fb$^{-1}$ of pp collisions collected in 2012 by the CMS experiment at the LHC, at a center-of-mass energy $\sqrt{s}=8$ TeV. No significant excess in data is observed above the expected standard model backgrounds. [...]
CMS-PAS-SUS-13-011.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_002-d: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_005-d: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_008-e: PDF; Figure_008-f: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_009-c: PDF; Figure_009-d: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_010-d: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_011-c: PDF; Figure_011-d: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_014: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_015-c: PDF; Figure_015-d: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_016-c: PDF; Figure_016-d: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_017-c: PDF; Figure_017-d: PDF; Figure_018-a: PDF; Figure_018-b: PDF; Figure_018-c: PDF; Figure_018-d: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_019-c: PDF; Figure_019-d: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_020-c: PDF; Figure_020-d: PDF; Figure_021-a: PDF; Figure_021-b: PDF; Figure_021-c: PDF; Figure_021-d: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Figure_022-c: PDF; Figure_022-d: PDF; Figure_023-a: PDF; Figure_023-b: PDF; Figure_023-c: PDF; Figure_023-d: PDF; Figure_024-a: PDF; Figure_024-b: PDF; Fulltext in PDF: PDF;
|
Detailed record - Similar records
|
|
|