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[PDF] Top 20 Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV

Has 10000 "Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV" found on our website. Below are the top 20 most common "Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV".

Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV

Measurement of the prompt $J/\psi$ and $\psi$(2S) polarizations in $pp$ collisions at $\sqrt{s}$ = 7 TeV

... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN ... See full document

49

Measurement of the $Y(1S), Y(2S)$ and $Y(3S)$ polarizations in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the $Y(1S), Y(2S)$ and $Y(3S)$ polarizations in $pp$ collisions at $\sqrt{s}=7$ TeV

... G. Cerminara, T. Christiansen, J.A. Coarasa Perez, D. D’Enterria, A. Dabrowski, A. De Roeck, S. Di Guida, M. Dobson, N. Dupont-Sagorin, A. Elliott-Peisert, B. Frisch, W. Funk, G. Georgiou, M. Giffels, D. Gigi, K. ... See full document

25

Measurement of J/ψ and ψ(2S) Prompt Double-Differential Cross Sections in pp Collisions at $\sqrt{s}$=7  TeV

Measurement of J/ψ and ψ(2S) Prompt Double-Differential Cross Sections in pp Collisions at $\sqrt{s}$=7  TeV

... into the physically observable quarkonium through a nonperturbative evolution that may change L and S, with bound-state formation probabilities proportional to long-distance matrix elements ... See full document

31

Measurement of the X(3872) production cross section via decays to J/psi pi pi in pp collisions at sqrt(s) = 7 TeV

Measurement of the X(3872) production cross section via decays to J/psi pi pi in pp collisions at sqrt(s) = 7 TeV

... The measurement is found to be stable with respect to variations of the pseudo-proper-decay- length requirement between 50 and 250 ...Application of the same method to ψ ( ... See full document

35

Measurement of Prompt $\psi(2S) \to J/\psi$ Yield Ratios in Pb-Pb and $p-p$ Collisions at $\sqrt {s_{NN}}=$ 2.76  TeV

Measurement of Prompt $\psi(2S) \to J/\psi$ Yield Ratios in Pb-Pb and $p-p$ Collisions at $\sqrt {s_{NN}}=$ 2.76  TeV

... from the fitting method are studied by varying the signal and background shapes as well as the fitted invariant-mass ...shape, the sum of two CB functions with common mean ... See full document

27

Observation of the Z$\to\psi\ell^+\ell^-$ decay in pp collisions at $\sqrt{s}=$ 13 TeV

Observation of the Z$\to\psi\ell^+\ell^-$ decay in pp collisions at $\sqrt{s}=$ 13 TeV

... from the unpolarized result. In summary, a new decay mode of the Z boson into a ψ meson, where ψ represents the con- tributions from direct Jand ψ ( 2S ) → J/ψ ... See full document

28

Measurement of the production cross-section of $\psi(2S) \to J/\psi ( \to \mu^{+} \mu^{-}) \pi^{+} \pi^{-}$ in pp collisions at $ \sqrt{s} $ = 7 TeV at ATLAS

Measurement of the production cross-section of $\psi(2S) \to J/\psi ( \to \mu^{+} \mu^{-}) \pi^{+} \pi^{-}$ in pp collisions at $ \sqrt{s} $ = 7 TeV at ATLAS

... pions in the ψ(2S) → J/ψ π + π − decay are reconstructed by taking all pairs of the remaining oppositely charged tracks with p T > ...GeV and |η| < 2.5 and assigning ... See full document

58

Measurements of $\psi(2S)$ and $X(3872) \to J/\psi\pi^+\pi^-$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

Measurements of $\psi(2S)$ and $X(3872) \to J/\psi\pi^+\pi^-$ production in $pp$ collisions at $\sqrt{s} = 8$ TeV with the ATLAS detector

... J. Del Peso 84 , T. Del Prete 125a,125b , D. Delgove 118 , F. Deliot 137 , C.M. Delitzsch 51 , A. Dell’Acqua 32 , L. Dell’Asta 24 , M. Dell’Orso 125a,125b , M. Della Pietra 105a,l , D. della Volpe 51 , M. ... See full document

42

Observation of the decay $B^+ \to \psi(2S) \phi(1020) K^+$ in pp collisions at $\sqrt s =$ 8 TeV

Observation of the decay $B^+ \to \psi(2S) \phi(1020) K^+$ in pp collisions at $\sqrt s =$ 8 TeV

... production at the CERN LHC and the high luminosity of the accelerator provide the possibility to study rare B meson ...reported the likely presence of ... See full document

28

$J/\psi$ and $\psi_{2S}$ production in $pp$ collisions at $\sqrt{s}=7$ TeV

$J/\psi$ and $\psi_{2S}$ production in $pp$ collisions at $\sqrt{s}=7$ TeV

... momentum in the Brest frame, they populate different regions of the B-decay ...sets of non- prompt charmonium MC events are generated according to the following ... See full document

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Suppression of non-prompt $J/\psi$, prompt $J/\psi$, and Y(1S) in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

Suppression of non-prompt $J/\psi$, prompt $J/\psi$, and Y(1S) in PbPb collisions at $\sqrt{s_{NN}}=2.76$ TeV

... formation of a QGP in high-energy nuclear collisions can be evidenced in a variety of ...One of its most striking expected signatures is the suppression of ... See full document

51

Inclusive search for squarks and gluinos in $pp$ collisions at $\sqrt{s}=7$ TeV

Inclusive search for squarks and gluinos in $pp$ collisions at $\sqrt{s}=7$ TeV

... description of the CMS detector can be found elsewhere ...feature of the CMS detector is its superconducting solenoid magnet, of 6 m internal diameter, provid- ing a field of ... See full document

42

Search for excited leptons in $pp$ collisions at $\sqrt{s}=7$ TeV

Search for excited leptons in $pp$ collisions at $\sqrt{s}=7$ TeV

... (SM) of particle physics, albeit very successful, provides no explanation for the three generation structure of the fermion ...explain the observed hierar- chy have led to a family ... See full document

31

Prompt and non-prompt $J/\psi $ elliptic flow in Pb+Pb collisions at $\sqrt{s_{_\text {NN}}} = 5.02$ Tev with the ATLAS detector

Prompt and non-prompt $J/\psi $ elliptic flow in Pb+Pb collisions at $\sqrt{s_{_\text {NN}}} = 5.02$ Tev with the ATLAS detector

... acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, ... See full document

34

Measurement of the Z/$\gamma$*+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV

Measurement of the Z/$\gamma$*+b-jet cross section in pp collisions at $\sqrt{s}$ = 7 TeV

... describes the measurement with the Compact Muon Solenoid (CMS) detector of the pp → Z/γ ∗ + b-jet cross section with Z/γ ∗ → `` (where `` = ee or µµ), including at least ... See full document

29

Measurement of the Rapidity and Transverse Momentum Distributions of $Z$ Bosons in $pp$ Collisions at $\sqrt{s}=7$ TeV

Measurement of the Rapidity and Transverse Momentum Distributions of $Z$ Bosons in $pp$ Collisions at $\sqrt{s}=7$ TeV

... Onderzoek; the Brazilian Funding Agencies (CNPq, CAPES, FAPERJ, and FAPESP); the Bul- garian Ministry of Education and Science; CERN; the Chinese Academy of Sciences, ... See full document

37

Measurement of the mass of the top quark in decays with a $J/\psi$ meson in pp collisions at 8 TeV

Measurement of the mass of the top quark in decays with a $J/\psi$ meson in pp collisions at 8 TeV

... combines the information from all CMS subdetectors to identify and reconstruct individual objects pro- duced in pp ...collisions. The particle candidates include muons, ... See full document

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Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS

Measurement of the differential cross-section of $B^{+}$ meson production in pp collisions at $\sqrt{s}$ = 7 TeV at ATLAS

... L. Adamczyk 38a , D.L. Adams 25 , T.N. Addy 56 , J. Adelman 177 , S. Adomeit 99 , T. Adye 130 , S. Aefsky 23 , J.A. Aguilar-Saavedra 125b,b , M. Agustoni 17 , S.P. Ahlen 22 , F. Ahles 48 , A. Ahmad ... See full document

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Measurement of the $W$-boson mass in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Measurement of the $W$-boson mass in pp collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... L. Nozka 127 , K. Ntekas 168 , E. Nurse 92 , F. Nuti 102 , F.G. Oakham 33,az , H. Oberlack 113 , T. Obermann 24 , J. Ocariz 133 , A. Ochi 80 , I. Ochoa 38 , J.P. Ochoa-Ricoux 144a , S. Oda 85 , S. ... See full document

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Measurement of b hadron lifetimes in pp collisions at $\sqrt{s} =$ 8 TeV

Measurement of b hadron lifetimes in pp collisions at $\sqrt{s} =$ 8 TeV

... on the lifetime due to uncertainties in the detector alignment [29] are in- vestigated for each decay topology using 20 different simulated samples with distorted ...expansions in ... See full document

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