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Measurement of the background in the CMS muon detector in ${p}{p}$-collisions at $\sqrt{s} = 13$ $\,\text {Te}\hspace{-.08em}\text {V}$ / CMS Muon Collaboration
The CMS detector, including its muon system, has been operating at the CERN LHC in increasingly challenging conditions for about 15 years. The muon detector was designed to provide excellent triggering and track reconstruction for muons produced in proton–proton collisons at an instantaneous luminosity ($\mathcal {L}$) of $1 \times 10^{34}$ cm$^{-2}$s$^{-1}$. [...]
2024 - 43 p. - Published in : Eur. Phys. J. C 84 (2024) 955 Fulltext: PDF;

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Radiation monitoring of the GEM muon detectors at CMS / Dimitrov, L (Sofiya, Inst. Nucl. Res.) ; Iaydjiev, P (Sofiya, Inst. Nucl. Res.) ; Mitev, G (Sofiya, Inst. Nucl. Res.) ; Vankov, I (Sofiya, Inst. Nucl. Res.)
The higher energy and luminosity of future High Luminosity (HL) LHC, determines a significant increasing of the radiation background around the CMS subdetectors, and especially in the higher pseudorapidity region. Under such heavy conditions, the RPC (used in muon trigger) most probably could not operate effectively. [...]
Springer, 2016 - 6 p. - Published in : Phys. Part. Nucl. Lett. 13 (2016) 551-556

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Radiation Monitoring at New CERN Radiation Facility GIF++ / Dimitrov, L.P (INRNE) ; Iaydjiev, P.S (INRNE) ; Mitev, G.M (INRNE) ; Vankov, I.V (INRNE)
AIDA-SLIDE-2015-017.- Geneva : CERN, 2015 Fulltext: PDF;

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A New Boson with a Mass of 125 GeV Observed with the CMS Experiment at the Large Hadron Collider / CMS Collaboration
The Higgs boson was postulated nearly five decades ago within the framework of the standard model of particle physics and has been the subject of numerous searches at accelerators around the world. Its discovery would verify the existence of a complex scalar field thought to give mass to three of the carriers of the electroweak force—the W+, W–, and Z0 bosons—as well as to the fundamental quarks and leptons. [...]
Geneva : CERN, 2012 - 16 p. - Published in : Science 338 (2012) 1569-1575 Preprint: PDF; External link: Supplementary material
In : Breakthrough of the year

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Test a prototype of a Micro Controller Unit (μCU) for the control and reading of the RADMON radiation detectors – LAAS 1600 and REM 250 / Iaydjiev, Plamen (INRNE, Sofia and Bulgarian Science Fund – MEYS, Bulgaria) ; Vankov, Ivan (INRNE, Sofia and Bulgarian Science Fund – MEYS, Bulgaria) ; Dimitrov, Liubomir (INRNE, Sofia and Bulgarian Science Fund – MEYS, Bulgaria) ; Mitev, Georgi (INRNE, Sofia and Bulgarian Science Fund – MEYS, Bulgaria)
AIDA-NOTE-2012-004.- Geneva : CERN, 2012 Fulltext: AIDA_Tech_Note_RADMONs - PDF; AIDA-NOTE-2012-004 - DOCX;

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Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC / CMS Collaboration
Results are presented from searches for the standard model Higgs boson in proton-proton collisions at $\sqrt{s}$=7 and 8 TeV in the CMS experiment at the LHC, using data samples corresponding to integrated luminosities of up to 5.1 inverse femtobarns at 7 TeV and 5.3 inverse femtobarns at 8 TeV. The search is performed in five decay modes: $\gamma\gamma$, ZZ, WW, $\tau^+ \tau^-$, and $b\bar{b}$. [...]
arXiv:1207.7235; CMS-HIG-12-028; CERN-PH-EP-2012-220; CMS-HIG-12-028; CERN-PH-EP-2012-220.- Geneva : CERN, 2012-08-17 - 32 p. - Published in : Phys. Lett. B 716 (2012) 30-61 Elsevier Open Access article: PDF; Fulltext: PDF; External links: Press Release; Interactions.org article; DOE Science Highlight
In : Higgs booklet, pp.30

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Missing transverse energy performance of the CMS detector / CMS Collaboration
During 2010 the LHC delivered pp collisions with a centre-of-mass energy of 7 TeV. In this paper, the results of comprehensive studies of missing transverse energy as measured by the CMS detector are presented. [...]
arXiv:1106.5048; CERN-PH-EP-2011-051; CMS-JME-10-009; CMS-JME-10-009; CERN-PH-EP-2011-051.- Geneva : CERN, 2011 - 56 p. - Published in : JINST 6 (2011) P09001 Fulltext: PDF; IOP Open Access article: PDF;

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Measurement of the Ratio of the 3-jet to 2-jet Cross Sections in pp Collisions at $\sqrt{s}$ = 7 TeV / CMS Collaboration
A measurement of the ratio of the inclusive 3-jet to 2-jet cross sections as a function of the total jet transverse momentum, HT, in the range 0.2 < HT < 2.5 TeV is presented. The data have been collected at a proton-proton centre-of-mass energy of 7 TeV with the CMS detector at the LHC, and correspond to an integrated luminosity of 36 inverse picobarns. [...]
arXiv:1106.0647; CERN-PH-EP-2011-044; CMS-QCD-10-012; CMS-QCD-10-012; CERN-PH-EP-2011-044.- Geneva : CERN, 2013-07-16 - 19 p. - Published in : Phys. Lett. B 702 (2011) 336-354 Elsevier Open Access article: PDF; Fulltext: PDF; External link: Rivet analyses reference

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Measurement of the Inclusive Jet Cross Section in pp Collisions at $\sqrt{s}$ = 7 TeV / CMS Collaboration
The inclusive jet cross section is measured in pp collisions with a center-of-mass energy of 7 TeV at the LHC using the CMS experiment. The data sample corresponds to an integrated luminosity of 34 inverse picobarns. [...]
arXiv:1106.0208; CERN-PH-EP-2011-053; CMS-QCD-10-011; CMS-QCD-10-011; CERN-PH-EP-2011-053.- Geneva : CERN, 2011 - 24 p. - Published in : Phys. Rev. Lett. 107 (2011) 132001 APS Open Access article: PDF; Fulltext: PDF; External link: Rivet analyses reference

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10.

Measurement of W$\gamma$ and Z$\gamma$ production in pp collisions at $\sqrt{s}$ = 7 TeV / CMS Collaboration
A measurement of W-gamma and Z-gamma production in proton-proton collisions at sqrt(s) = 7 TeV, based on a data sample recorded by the CMS experiment at the LHC, and corresponding to an integrated luminosity of 36 inverse picobarns, is presented. The electron and muon decay channels of the W and Z are used. [...]
arXiv:1105.2758; CERN-PH-EP-2011-045; CMS-EWK-10-008; CMS-EWK-10-008; CERN-PH-EP-2011-045.- Geneva : CERN, 2013-07-16 - 21 p. - Published in : Phys. Lett. B 701 (2011) 535-555 Elsevier Open Access article: PDF; Fulltext: PDF; External link: FERMILABTODAY

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Vedi anche: autori con nomi simili
1	Dimitrov, L.
1	Dimitrov, L.P
1	Dimitrov, Liubomir
68	Dimitrov, Lubomir

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