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[PDF] Top 20 Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV

Has 10000 "Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV" found on our website. Below are the top 20 most common "Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV".

Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV

Measurement of the ratio $B(B^0_s \to J/\psi f_0(980))$ / $B(B^0_s \to J/\psi \phi(1020))$ in pp collisions at $\sqrt s$ = 7 TeV

... from the Marie-Curie programme and the European Re- search Council and EPLANET (European Union); the Leventis Foundation; the ...Foundation; the Alexander von Humboldt Foundation; ... See full document

27

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

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

28

Measurement of the production cross section for a W boson and two b jets in pp collisions at $\sqrt{s}$=7 TeV

Measurement of the production cross section for a W boson and two b jets in pp collisions at $\sqrt{s}$=7 TeV

... S. Abdullin, M. Albrow, J. Anderson, G. Apollinari, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, K. Burkett, J.N. Butler, V. Chetluru, H.W.K. Cheung, F. Chlebana, S. Cihangir, V.D. ... See full document

31

Measurement of the $\Lambda_b$ cross section and the $_{\bar{\Lambda}_b}$ to $\Lambda_b$ ratio with $J/\Psi \Lambda$ decays in $pp$ collisions at $\sqrt{s}=7$ TeV

Measurement of the $\Lambda_b$ cross section and the $_{\bar{\Lambda}_b}$ to $\Lambda_b$ ratio with $J/\Psi \Lambda$ decays in $pp$ collisions at $\sqrt{s}=7$ TeV

... D. Abbaneo, E. Auffray, G. Auzinger, P. Baillon, A.H. Ball, D. Barney, C. Bernet 5 , G. Bianchi, P. Bloch, A. Bocci, A. Bonato, H. Breuker, T. Camporesi, G. Cerminara, T. Christiansen, J.A. Coarasa Perez, D. D’Enterria, ... See full document

33

Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV

Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV

... Λ bJ=ψΛ is a rich source of information about the effect of strong interactions in hadronic ...taken to study its characteristics. Several techniques [1–10] are used ... See full document

20

Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t}  jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV

Measurement of the cross section ratio $\sigma_\mathrm{t \bar{t} b \bar{b}} / \sigma_\mathrm{t \bar{t} jj }$ in pp collisions at $\sqrt{s}$ = 8 TeV

... (PDF+α S ) [10], where the uncertainty labelled “scale” refers to the uncertainty from the factorization and renormalization scales (µ F and µ R ), and the uncertainty labelled ... 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

... D. Abbaneo, E. Auffray, G. Auzinger, M. Bachtis, P. Baillon, A.H. Ball, D. Barney, J.F. Benitez, C. Bernet 5 , G. Bianchi, P. Bloch, A. Bocci, A. Bonato, C. Botta, H. Breuker, T. Camporesi, G. Cerminara, T. Christiansen, ... See full document

35

Measurement of the CP-violating weak phase $\phi_s$ and the decay width difference $\Delta \Gamma_s$ using the B$_s^0 \to J/\psi\phi$(1020) decay channel in pp collisions at $\sqrt{s}=$ 8 TeV

Measurement of the CP-violating weak phase $\phi_s$ and the decay width difference $\Delta \Gamma_s$ using the B$_s^0 \to J/\psi\phi$(1020) decay channel in pp collisions at $\sqrt{s}=$ 8 TeV

... 4: The mistag probabilities ω, defined as the ratio of the number of wrongly tagged events divided by the total number of tagged events, as a function of ... See full document

34

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

... A.A. Talyshev 108,g , J.Y.C. Tam 175 , M.C. Tamsett 78,am , K.G. Tan 87 , J. Tanaka 156 , R. Tanaka 116 , S. Tanaka 132 , S. Tanaka 65 , A.J. Tanasijczuk 143 , K. Tani 66 , N. Tannoury 84 , S. ... See full document

44

$J/\psi$ 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

... on the type of muon chamber and the region of the detector: this rejects muon signals whose spatial separation in the muon stations is too small, in order to ... See full document

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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

... M. Aldaya Martin, T. Arndt, C. Asawatangtrakuldee, I. Babounikau, K. Beernaert, O. Behnke, U. Behrens, A. Berm ´udez Mart´ınez, D. Bertsche, A.A. Bin Anuar, K. Borras 16 , V. Botta, A. Campbell, P. Connor, C. ... See full document

28

Measurement of the production cross sections for a Z boson and one or more b jets in pp collisions at sqrt(s) = 7 TeV

Measurement of the production cross sections for a Z boson and one or more b jets in pp collisions at sqrt(s) = 7 TeV

... reported of the cross sections ats = 7 TeV for the produc- tion of a Z boson with exactly one or at least two b ...according to the ... See full document

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Measurement of the cross-section for W boson production in association with b-jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

Measurement of the cross-section for W boson production in association with b-jets in pp collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detector

... compare the NLO calculations with data, the impact of non-perturbative effects and double-parton interactions has to be ...considered. The MCFM predictions are only available at ... See full document

53

Angular analysis of the decay $B^0 \to K^{*0} \mu^+ \mu^-$ from pp collisions at $\sqrt  s = 8$ TeV

Angular analysis of the decay $B^0 \to K^{*0} \mu^+ \mu^-$ from pp collisions at $\sqrt s = 8$ TeV

... used in the analysis accommodates cases in which the kaon and pion charges are correctly and incorrectly ...Both of these contributions are treated as signal. The mistag fraction ... See full document

36

Measurement of the cross section and angular correlations for associated production of a Z boson with b hadrons in pp collisions at $\sqrt{s} =$ 7 TeV

Measurement of the cross section and angular correlations for associated production of a Z boson with b hadrons in pp collisions at $\sqrt{s} =$ 7 TeV

... From the experimental point of view, the study of b-hadron pair production using the stan- dard jet-based b-tagging methods [17] suffers from geometrical limitations due ... See full document

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Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector

Measurement of the prompt J/ $\psi $ pair production cross-section in pp collisions at $\sqrt{s} = 8$  TeV with the ATLAS detector

... resolution of the reconstructed J/ψ meson depend on p T (both varying by about 3% with p T in the studied region), but in the di-J/ψ sample there are not enough ... See full document

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Determination of the ratio of $b$-quark fragmentation fractions $f_s/f_d$ in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

Determination of the ratio of $b$-quark fragmentation fractions $f_s/f_d$ in $pp$ collisions at $\sqrt{s}=7$ TeV with the ATLAS detector

... C.J. Oram 159a , M.J. Oreglia 31 , Y. Oren 153 , D. Orestano 134a,134b , N. Orlando 154 , C. Oropeza Barrera 53 , R.S. Orr 158 , B. Osculati 50a,50b , R. Ospanov 84 , G. Otero y Garzon 27 , H. Otono 70 , M. ... See full document

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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

... Values of the discriminant greater than one indicate the presence of a secondary ...vertex. To improve the purity of the selection, only secondary vertices built ... See full document

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Measurement of the total and differential inclusive $B^+$ hadron cross sections in pp collisions at $\sqrt{s}$ = 13 TeV

Measurement of the total and differential inclusive $B^+$ hadron cross sections in pp collisions at $\sqrt{s}$ = 13 TeV

... “nonprompt” J /ψ meson decays, while rejecting almost all promptly produced J /ψ ...Also, the J /ψ meson momentum vector reconstructed at the HLT stage must point back to ... See full document

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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

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