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[PDF] Top 20 Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays

Has 10000 "Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays" found on our website. Below are the top 20 most common "Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays".

Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays

Search for $B^0_s \to \mu^+ \mu^-$ and $B^0 \to \mu^+ \mu^-$ decays

... technical and administrative staff at CERN and other CMS ...Science and Research; the Belgium Fonds de la Recherche Scientifique, and Fonds voor Wetenschap- pelijk Onderzoek; the Brazilian ... See full document

35

Search for high-mass Z$\gamma$ resonances in $\mathrm{ e }^{+}\mathrm{ e }^{-}\gamma $ and $ \mu^{+}\mu^{-}\gamma$ final states in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV

Search for high-mass Z$\gamma$ resonances in $\mathrm{ e }^{+}\mathrm{ e }^{-}\gamma $ and $ \mu^{+}\mu^{-}\gamma$ final states in proton-proton collisions at $\sqrt{s} =$ 8 and 13 TeV

... boson decays, as expected in the decay of high-mass ...itself. To account for the contamination from pileup interactions, charged particles originating from additional vertices are excluded from the ... See full document

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Observation of the rare $B^0_s\to\mu^+\mu^-$ decay from the combined analysis of CMS and LHCb data

Observation of the rare $B^0_s\to\mu^+\mu^-$ decay from the combined analysis of CMS and LHCb data

... 2 to a few TeV/c 2 . Since many of these new particles would be able to decay into b quarks and many of the SM measurements also involve b quarks, the detection of b-hadron ... See full document

20

Search for Higgs bosons decaying to $aa$ in the $\mu\mu\tau\tau$ final state in $pp$ collisions at $\sqrt{s} = $ 8 TeV with the ATLAS experiment

Search for Higgs bosons decaying to $aa$ in the $\mu\mu\tau\tau$ final state in $pp$ collisions at $\sqrt{s} = $ 8 TeV with the ATLAS experiment

... weights to the energy deposits arising from the electromagnetic and hadronic components of the show- ...calorimeter to match the particle-level jet energy [ 62 , 63 ...lation and then improved ... See full document

24

Search for lepton flavour violating decays of the Higgs boson to $\mu\tau$ and e$\tau$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV

Search for lepton flavour violating decays of the Higgs boson to $\mu\tau$ and e$\tau$ in proton-proton collisions at $\sqrt{s}=$ 13 TeV

... A. Canepa, G.B. Cerati, H.W.K. Cheung, F. Chlebana, M. Cremonesi, J. Duarte, V.D. Elvira, J. Freeman, Z. Gecse, E. Gottschalk, L. Gray, D. Green, S. Gr ¨unendahl, O. Gutsche, R.M. Harris, S. Hasegawa, J. Hirschauer, Z. ... See full document

48

Angular analysis of $B^0_d \rightarrow K^{*}\mu^+\mu^-$ decays in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS detector

Angular analysis of $B^0_d \rightarrow K^{*}\mu^+\mu^-$ decays in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS detector

... level and can proceed only via loops, hence are ...a b-quark to an s µ + µ − final state mediated by electroweak box and penguin ...contribute to FCNC decay amplitudes, affecting the ... See full document

47

Search for lepton flavour violating decays of heavy resonances and quantum black holes to an e$\mu$ pair in proton-proton collisions at $\sqrt{s}$ = 8 TeV

Search for lepton flavour violating decays of heavy resonances and quantum black holes to an e$\mu$ pair in proton-proton collisions at $\sqrt{s}$ = 8 TeV

... A search for narrow resonances decaying to an electron and a muon is ...corresponding to an integrated luminosity of ...section and branching fraction for signals arising in theories ... See full document

38

Search for heavy Majorana neutrinos in $\mu^\pm \mu^\pm+$ jets events in proton-proton collisions at $\sqrt{s}$ = 8 TeV

Search for heavy Majorana neutrinos in $\mu^\pm \mu^\pm+$ jets events in proton-proton collisions at $\sqrt{s}$ = 8 TeV

... up to approximately 90 ...the search region up to about 200 GeV ...DELPHI, and LHCb allow for a finite heavy-neutrino lifetime such that it decays with a vertex displaced from the ... See full document

35

Measurement of angular parameters from the decay $\mathrm{B}^0 \to \mathrm{K}^{*0} \mu^+ \mu^-$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV

Measurement of angular parameters from the decay $\mathrm{B}^0 \to \mathrm{K}^{*0} \mu^+ \mu^-$ in proton-proton collisions at $\sqrt{s} = $ 8 TeV

... multibody B decays that might affect the low-mass sideband is addressed in Section 5 ...a B + → K + μ + μ − decay is combined with a random pion, and from events with a b0 μ + ... See full document

25

Search for lepton flavour violating decays of the Higgs boson to $e \tau$ and $e \mu$ in proton–proton collisions at $\sqrt s=$ 8 TeV

Search for lepton flavour violating decays of the Higgs boson to $e \tau$ and $e \mu$ in proton–proton collisions at $\sqrt s=$ 8 TeV

... S. Abdullin, M. Albrow, G. Apollinari, S. Banerjee, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, G. Bolla, K. Burkett, J.N. Butler, H.W.K. Cheung, F. Chlebana, S. Cihangir, V.D. Elvira, I. Fisk, J. Freeman, E. ... See full document

44

Angular analysis and branching fraction measurement of the decay B-0 -> K*(0)mu(+)mu(-)

Angular analysis and branching fraction measurement of the decay B-0 -> K*(0)mu(+)mu(-)

... average B 0 mass resolution of 44 ...corresponding to an inte- grated luminosity of 2 . 7 fb − 1 , requiring 1 . 0 < q 2 < 7 ...2 to avoid J /ψ and ψ ′ ...required ... See full document

24

Angular analysis and branching fraction measurement of the decay $B^0 \to K^{*0} \mu^+\mu^-$

Angular analysis and branching fraction measurement of the decay $B^0 \to K^{*0} \mu^+\mu^-$

... programme and the European Re- search Council and EPLANET (European Union); the Leventis Foundation; the ...Youth and Sports (MEYS) of Czech Republic; the Council of Science and ... See full document

35

Measurement of the B(s) to mu+ mu- branching fraction and search for B0 to mu+ mu- with the CMS Experiment

Measurement of the B(s) to mu+ mu- branching fraction and search for B0 to mu+ mu- with the CMS Experiment

... trained to distinguish between signal and back- ground event ...training, B 0 s → µ + µ − MC simulation samples are used for the signal, and candidates from the data dimuon mass ... See full document

31

Search for a heavy narrow resonance decaying to $e \mu$, $e \tau$, or $\mu \tau$ with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC

Search for a heavy narrow resonance decaying to $e \mu$, $e \tau$, or $\mu \tau$ with the ATLAS detector in $\sqrt{s}=7$ TeV $pp$ collisions at the LHC

... 0.1 and ∆R = 0.4, and the invariant mass associated with the energy ...ττ decays, while accepting 1 of 20 to 1 of 50 ordinary hadronic jets misidenti- fied as tau ...tau decays with ... See full document

33

Search for the decay $B_s^0 \to \mu \mu$ with the ATLAS detector

Search for the decay $B_s^0 \to \mu \mu$ with the ATLAS detector

... input to the multivariate classifier, the tuning of the simulation for the determination of the signal efficiency, the data samples used to estimate the background rejection and the opti- mization ... See full document

25

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

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

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

29

Characterisation of Strongly Normalising lambda-mu-Terms

Characterisation of Strongly Normalising lambda-mu-Terms

... completely. To solve this problem, we first restrict types to those having ω only as the final part of a product type; we then suitably modify the standard interpretation of intersection types, adapting ... See full document

17

Search for heavy Majorana neutrinos in $\mu^{\pm}\mu^{\pm} +$ jets and $e^{\pm}e^{\pm} +$ jets events in pp collisions at $\sqrt{s} =$ 7 TeV

Search for heavy Majorana neutrinos in $\mu^{\pm}\mu^{\pm} +$ jets and $e^{\pm}e^{\pm} +$ jets events in pp collisions at $\sqrt{s} =$ 7 TeV

... Electron and muon candidates must be isolated from other activity in the event by requiring their relative isolation (I rel ) to be less than ...momenta and transverse calorimeter energy depositions ... See full document

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Modelling $Z\rightarrow\tau\tau$ processes in ATLAS with $\tau$-embedded $Z\rightarrow\mu\mu$ data

Modelling $Z\rightarrow\tau\tau$ processes in ATLAS with $\tau$-embedded $Z\rightarrow\mu\mu$ data

... A. Andreazza 91a,91b , V. Andrei 58a , S. Angelidakis 9 , I. Angelozzi 107 , P. Anger 44 , A. Angerami 35 , F. Anghinolfi 30 , A.V. Anisenkov 109,c , N. Anjos 12 , A. Annovi 124a,124b , M. Antonelli 47 , A. Antonov 98 , ... See full document

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Desempenho em redes WLAN MU-MIMO com seleção de usuário e diversidade

Desempenho em redes WLAN MU-MIMO com seleção de usuário e diversidade

... 14 Em casos em que o canal possui um tempo de coerência menor, quando o cliente é móvel ou a quantização do canal é imprecisa, (BEJARANO et al., 2016) apresenta o CHRoME (CHannel Resilient Multi-User bEamforming). A ... See full document

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