CERN Accelerating science

CERN Document Server 530 registres trobats  1 - 10següentfinal  anar al registre: La cerca s'ha fet en 0.61 segons. 
1.
Precision measurement of the structure of the CMS inner tracking system using nuclear interactions / CMS Collaboration
The structure of the CMS inner tracking system has been studied using nuclear interactions of hadrons striking its material. Data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded in 2015 at the LHC are used to reconstruct millions of secondary vertices from these nuclear interactions. [...]
arXiv:1807.03289; CMS-TRK-17-001; CERN-EP-2018-144; CMS-TRK-17-001-003.- Geneva : CERN, 2018-10-29 - 41 p. - Published in : JINST 13 (2018) P10034 Fulltext: 1807.03289 - PDF; fulltext1682069 - PDF; Fulltext from Publisher: PDF; External link: Figures, tables and other information
2.
Presentations on LHC, CMS and physics from the Neighborhood event at CMS 24/25 May 2014 / Beauceron, Stephanie (Centre National de la Recherche Scientifique (FR)) ; Daubie, Evelyne (Universite de Mons (BE))
Language: French Target audience: General public<br /><br />Working files are accessible in DocDB: <br /><a href="https://cms-docdb.cern.ch/cgi-bin/DocDB/ShowDocument?docid=12304">https://cms-docdb.cern.ch/cgi-bin/DocDB/ShowDocument?docid=12304</a>
CMS-OUTREACH-2018-019.
- 2014.
Language: French
3.
Characterisation of irradiated thin silicon sensors for the CMS phase II pixel upgrade / Adam, W (Vienna, OAW) ; Bergauer, T (Vienna, OAW) ; Brondolin, E (Vienna, OAW) ; Dragicevic, M (Vienna, OAW) ; Friedl, M (Vienna, OAW) ; Frühwirth, R (Vienna, OAW) ; Hoch, M (Vienna, OAW) ; Hrubec, J (Vienna, OAW) ; König, A (Vienna, OAW) ; Steininger, H (Vienna, OAW) et al. /Tracker Group
The high luminosity upgrade of the Large Hadron Collider, foreseen for 2026, necessitates the replacement of the CMS experiment’s silicon tracker. The innermost layer of the new pixel detector will be exposed to severe radiation, corresponding to a 1 MeV neutron equivalent fluence of up to $\Phi _{eq} = 2 \times 10^{16}$  cm$^{-2}$ , and an ionising dose of ${\approx } 5$  MGy after an integrated luminosity of 3000 fb$^{-1}$ . [...]
2017 - 13 p. - Published in : Eur. Phys. J. C 77 (2017) 567
4.
P-Type Silicon Strip Sensors for the new CMS Tracker at HL-LHC / Adam, W (Vienna, OAW) ; Bergauer, T (Vienna, OAW) ; Brondolin, E (Vienna, OAW) ; Dragicevic, M (Vienna, OAW) ; Friedl, M (Vienna, OAW) ; Frühwirth, R (Vienna, OAW) ; Hoch, M (Vienna, OAW) ; Hrubec, J (Vienna, OAW) ; König, A (Vienna, OAW) ; Steininger, H (Vienna, OAW) et al. /CMS
The upgrade of the LHC to the High-Luminosity LHC (HL-LHC) is expected to increase the LHC design luminosity by an order of magnitude. This will require silicon tracking detectors with a significantly higher radiation hardness. [...]
2017 - 27 p. - Published in : JINST 12 (2017) P06018 Fulltext: PDF;
5.
Measurement of the mass difference between top quark and antiquark in pp collisions at $\sqrt{s} = 8$ TeV / CMS Collaboration
The invariance of the standard model (SM) under the CPT transformation predicts equality of particle and antiparticle masses. This prediction is tested by measuring the mass difference between the top quark and antiquark (Delta m[t] = m[t] - m[t-bar]) that are produced in pp collisions at a center-of-mass energy of 8 TeV, using events with a muon or an electron and at least four jets in the final state. [...]
arXiv:1610.09551; CMS-TOP-12-031; CERN-EP-2016-249.- Geneva : Elsevier, 2017-07-10 - 22 p. - Published in : Phys. Lett. B 770 (2017) 50-71 Article from SCOAP3: PDF; Fulltext: fermilab-pub-16-592-cms - PDF; arXiv:1610.09551 - PDF; External link: Figures, tables and other information
6.
Production of leading charged particles and leading charged-particle jets at small transverse momenta in pp collisions at sqrt(s) = 8 TeV / CMS Collaboration
The per-event yield of the highest transverse momentum charged particle and charged-particle jet, integrated above a given $p_{\mathrm{T}}^{\mathrm{min}}$ threshold starting at $p_{\mathrm{T}}^{\mathrm{min}} = $ 0.8 and 1 GeV, respectively, is studied in PbPb collisions at $\sqrt{s} =$ 8 TeV. The particles and the jets are measured for absolute pseudorapidities lower than 2.4 and 1.9, respectively. [...]
arXiv:1507.00233; CMS-FSQ-12-032; CERN-PH-EP-2015-135.- Geneva : CERN, 2015-12-01 - 17 p. - Published in : Phys. Rev. D 92 (2015) 112001 APS Open Access article: PDF; Fulltext: 10.1103_PhysRevD.92.112001 - PDF; arXiv:1507.00233 - PDF; External links: Rivet analyses reference; Open Access fulltext
7.
Measurement of the differential cross section for top quark pair production in pp collisions at $\sqrt{s} =$ 8 TeV / CMS Collaboration
The normalized differential cross section for top quark pair ($ \mathrm{ t \bar{t} } $) production is measured in pp collisions at a centre-of-mass energy of 8 TeV at the CERN LHC using the CMS detector in data corresponding to an integrated luminosity of 19.7 fb$^{-1}$. The measurements are performed in the lepton+jets (e/$ \mu $+jets) and in the dilepton (ee, $ \mu \mu $, and e$ \mu $) decay channels. [...]
arXiv:1505.04480; CMS-TOP-12-028; CERN-PH-EP-2015-117; CMS-TOP-12-028; CERN-PH-EP-2015-117.- Geneva : CERN, 2015-11-20 - 65 p. - Published in : Eur. Phys. J. C 75 (2015) 542 Article from SCOAP3: PDF; Fulltext: PDF; Springer Open Access article: PDF; External links: Rivet analyses reference; Rivet analyses reference
8.
Impact of low-dose electron irradiation on n+p silicon strip sensors / Tracker Group of the CMS Collaboration
The response of n+p silicon strip sensors to electrons from a Sr-90 source was measured using a multi-channel read-out system with 25 ns sampling time. The measurements were performed over a period of several weeks, during which the operating conditions were varied. [...]
arXiv:1505.02672.- 2015-12-11 - 13 p. - Published in : Nucl. Instrum. Methods Phys. Res., A 803 (2015) 100-112 Elsevier Open Access article: PDF; Fulltext: openaccess_1-s2.0-S0168900215009602-main - PDF; arXiv:1505.02672 - PDF; 10.1016_j.nima.2015.08.026 - PDF; External link: Open Access fulltext
9.
Trapping in irradiated p-on-n silicon sensors at fluences anticipated at the HL-LHC outer tracker / Adam, W. (Vienna, OAW) ; Bergauer, T. (Vienna, OAW) ; Dragicevic, M. (Vienna, OAW) ; Friedl, M. (Vienna, OAW) ; Fruehwirth, R. (Vienna, OAW) ; Hoch, M. (Vienna, OAW) ; Hrubec, J. (Vienna, OAW) ; Krammer, M. (Vienna, OAW) ; Treberspurg, W. (Vienna, OAW) ; Waltenberger, W. (Vienna, OAW) et al. /CMS Tracker Group
The degradation of signal in silicon sensors is studied under conditions expected at the CERN High-Luminosity LHC. 200 $\mu$m thick n-type silicon sensors are irradiated with protons of different energies to fluences of up to $3 \cdot 10^{15}$ neq/cm$^2$. [...]
arXiv:1505.01824.- 2016-04-22 - 18 p. - Published in : JINST 11 (2016) P04023 Fulltext: arXiv:1505.01824 - PDF; openaccess_jinst16_04_p04023 - PDF; 10.1088_1748-0221_11_04_P04023 - PDF; IOP Open Access article: PDF; External link: Open Access fulltext
10.
Angular coefficients of Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^{+}\mu^{-}$ as a function of transverse momentum and rapidity / CMS Collaboration
Measurements of the five most significant angular coefficients, $A_{0}$ through $A_{4}$, for Z bosons produced in pp collisions at $\sqrt{s}$ = 8 TeV and decaying to $\mu^{+}\mu^{-}$ are presented as a function of the transverse momentum and rapidity of Z boson. The integrated luminosity of the dataset collected with the CMS detector at the LHC corresponds to 19.7 fb$^{-1}$. [...]
arXiv:1504.03512; CMS-SMP-13-010; CERN-PH-EP-2015-046; CMS-SMP-13-010; CERN-PH-EP-2015-046.- Geneva : CERN, 2015-09-01 - 22 p. - Published in : Phys. Lett. B 750 (2015) 154-175 Article from SCOAP3: PDF; Elsevier Open Access article: PDF; Fulltext: PDF; External link: FERMILABTODAY

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