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1.
TCT and test beam results of irradiated magnetic Czochralski silicon (MCz-Si) detectors / Luukka, P (Helsinki Inst. of Phys.) ; Härkönen, J (Helsinki Inst. of Phys.) ; Mäenpää, T (Helsinki Inst. of Phys.) ; Betchart, B (Rochester U.) ; Czellar, S (Helsinki Inst. of Phys.) ; Demina, R (Rochester U.) ; Furgeri, A (Karlsruhe U., EKP) ; Gotra, Y (Rochester U.) ; Frey, M (Karlsruhe U., EKP) ; Hartmann, F (Karlsruhe U., EKP) et al.
Pad and strip detectors processed on high resistivity n-type magnetic Czochralski silicon (MCz-Si) were irradiated to several different fluences with protons. The pad detectors were characterized with the transient current technique (TCT) and the full-size strip detectors with a reference beam telescope and a 225GeV muon beam. [...]
FERMILAB-CONF-09-677-E.- 2009 - 4 p. - Published in : Nucl. Instrum. Methods Phys. Res., A 604 (2009) 254-257
Fulltext: PDF; External link: FERMILABCONF
In : 8th International Conference on Position Sensitive Detectors, Glasgow, UK, 01 - 05 Sep 2008, pp.254-257
2.
Bose-Einstein correlations in $pp, p\mathrm{Pb}$, and PbPb collisions at $\sqrt{{s}_{NN}}=0.9-7$ TeV / CMS Collaboration
Quantum statistical (Bose-Einstein) two-particle correlations are measured in pp collisions at $\sqrt{s}= $ 0.9, 2.76, and 7 TeV, as well as in pPb and peripheral PbPb collisions at nucleon-nucleon center-of-mass energies of 5.02 and 2.76 TeV, respectively, using the CMS detector at the LHC. Separate analyses are performed for same-sign unidentified charged particles as well as for same-sign pions and kaons identified via their energy loss in the silicon tracker. [...]
arXiv:1712.07198; CMS-FSQ-14-002; CERN-EP-2017-327; CMS-FSQ-14-002-003.- Geneva : CERN, 2018-06-15 - 42 p. - Published in : Phys. Rev. C 97 (2018) 064912 Article from SCOAP3: PDF; Fulltext: arXiv:1712.07198 - PDF; openaccess_PhysRevC.97.064912 - PDF; External links: Additional information for the analysis; CMS AuthorList
3.
Search for new long-lived particles at $\sqrt{s} =$ 13 TeV / CMS Collaboration
A search for long-lived particles was performed with data corresponding to an integrated luminosity of 2.6 fb$^{-1}$ collected at a center-of-mass energy of 13 TeV by the CMS experiment in 2015. The analysis exploits two customized topological trigger algorithms, and uses the multiplicity of displaced jets to search for the presence of a signal decay occurring at distances between 1 and 1000 mm. [...]
arXiv:1711.09120; CMS-EXO-16-003; CERN-EP-2017-264; CMS-EXO-16-003-003.- Geneva : CERN, 2018-05-10 - 23 p. - Published in : Phys. Lett. B 780 (2018) 432-454 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
4.
Measurement of the underlying event activity in inclusive Z boson production in proton-proton collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
This paper presents a measurement of the underlying event activity in proton-proton collisions at a center-of-mass energy of 13 TeV, performed using inclusive Z boson production events collected with the CMS experiment at the LHC. The analyzed data correspond to an integrated luminosity of 2.1 fb$^{-1}$. [...]
arXiv:1711.04299; CMS-FSQ-16-008; CERN-EP-2017-249; CMS-FSQ-16-008-003.- Geneva : CERN, 2018-07-05 - 38 p. - Published in : JHEP 07 (2018) 032 Article from SCOAP3: PDF; Fulltext: PDF; External link: Rivet analyses reference
5.
Measurement of the inclusive $\mathrm{t}\overline{\mathrm{t}}$ cross section in pp collisions at $\sqrt{s} =$ 5.02 TeV using final states with at least one charged lepton / CMS Collaboration
The top quark pair production cross section ($\sigma_{\mathrm{t}\overline{\mathrm{t}}}$) is measured for the first time in pp collisions at a center-of-mass energy of 5.02 TeV. The data were collected by the CMS experiment at the LHC and correspond to an integrated luminosity of 27.4 pb$^{-1}$. [...]
arXiv:1711.03143; TOP-16-023; CERN-EP-2017-258; CMS-TOP-16-023-004.- Geneva : CERN, 2018-03-20 - 42 p. - Published in : JHEP 03 (2018) 115 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
6.
Measurement of associated Z + charm production in proton-proton collisions at $\sqrt{s} = $ 8 TeV / CMS Collaboration
A study of the associated production of a Z boson and a charm quark jet (Z + c), and a comparison to production with a b quark jet (Z + b), in pp collisions at a centre-of-mass energy of 8 TeV are presented. The analysis uses a data sample corresponding to an integrated luminosity of 19.7 fb$^{-1}$, collected with the CMS detector at the CERN LHC. [...]
arXiv:1711.02143; CMS-SMP-15-009; CERN-EP-2017-257; CMS-SMP-15-009-003.- Geneva : CERN, 2018-04-09 - 50 p. - Published in : Eur. Phys. J. C 78 (2018) 287 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
7.
Measurement of quarkonium production cross sections in pp collisions at $\sqrt{s}=$ 13 TeV / CMS Collaboration
Differential production cross sections of J/$\psi$ and $\psi$(2S) charmonium and $\Upsilon$(nS) (n = 1, 2, 3) bottomonium states are measured in proton-proton collisions at $\sqrt{s} =$ 13 TeV, with data collected by the CMS detector at the LHC, corresponding to an integrated luminosity of 2.3 fb$^{-1}$ for the J/$\psi$ and 2.7 fb$^{-1}$ for the other mesons. The five quarkonium states are reconstructed in the dimuon decay channel, for dimuon rapidity $|y| <$ 1.2. [...]
arXiv:1710.11002; CMS-BPH-15-005; CERN-EP-2017-267; CMS-BPH-15-005-003.- Geneva : CERN, 2018-05-10 - 22 p. - Published in : Phys. Lett. B 780 (2018) 251 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
8.
Search for supersymmetry in events with at least three electrons or muons, jets, and missing transverse momentum in proton-proton collisions at $ \sqrt{s}=13 $ TeV / CMS Collaboration
A search for new physics is carried out in events with at least three electrons or muons in any combination, jets, and missing transverse momentum. Results are based on the sample of proton-proton collision data produced by the LHC at a center-of-mass energy of 13 TeV and collected by the CMS experiment in 2016. [...]
arXiv:1710.09154; CMS-SUS-16-041; CERN-EP-2017-243; CMS-SUS-16-041-003.- Geneva : CERN, 2018-02-12 - 44 p. Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
9.
Pseudorapidity and transverse momentum dependence of flow harmonics in pPb and PbPb collisionsDifferential flow harmonics v_n in pPb and PbPb collisions / CMS Collaboration
Measurements of azimuthal angular correlations are presented for high-multiplicity pPb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 5.02 TeV and peripheral PbPb collisions at $\sqrt{s_{\mathrm{NN}}} = $ 2.76 TeV. The data used in this work were collected with the CMS detector at the CERN LHC. [...]
arXiv:1710.07864; CMS-HIN-15-008; CERN-EP-2017-218; CMS-HIN-15-008-003.- Geneva : CERN, 2018-10-05 - 25 p. - Published in : Phys. Rev. C 98 (2018) 044902 Fulltext: openaccess_PhysRevC.98.044902 - PDF; 1710.07864 - PDF; Preprint: PDF; External link: Open Access fulltext
10.
Simulation study of signal formation in position sensitive planar p-on-n silicon detectors after short range charge injection / Peltola, Timo (Texas Tech. ; Helsinki Inst. of Phys.) ; Eremin, Vladimir (Boskovic Inst., Zagreb) ; Verbitskaya, Elena (Boskovic Inst., Zagreb) ; Härkönen, Jaakko (Helsinki Inst. of Phys. ; Helsinki U.)
Segmented silicon detectors (micropixel and microstrip) are the main type of detectors used in the inner trackers of Large Hadron Collider (LHC) experiments at CERN. Due to the high luminosity and eventual high fluence, detectors with fast response to fit the short shaping time of 20 ns and sufficient radiation hardness are required. [...]
arXiv:1704.03442.- 2017-09-27 - 23 p. - Published in : JINST Fulltext: PDF;

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