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[PDF] Top 20 Search for B-s(0)->mu(+)mu(-) decays at D0

Has 10000 "Search for B-s(0)->mu(+)mu(-) decays at D0" found on our website. Below are the top 20 most common "Search for B-s(0)->mu(+)mu(-) decays at D0".

Search for B-s(0)->mu(+)mu(-) decays at D0

Search for B-s(0)->mu(+)mu(-) decays at D0

... The expected number of background events in the final candidate sample was estimated using events from the data in the low and high sidebands, together with the assump- tion that the background consists of same-b ... See full document

9

Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

Search For High-mass Z Gamma Resonances In E(+)e(-)gamma And Mu(+)mu(-)gamma Final States In Proton-proton Collisions At Root S=8 And 13 Tev

... This ensures high lepton identification efficiency even for highly-boosted Z boson decays, as expected in the decay of high-mass resonances. The relative isolation of the lepton is quantified by summing the ... See full document

34

Search for anomalous production of highly boosted $Z$ bosons decaying to $\mu^+ \mu^-$ in proton-proton collisions at $\sqrt{s}=7$ TeV

Search for anomalous production of highly boosted $Z$ bosons decaying to $\mu^+ \mu^-$ in proton-proton collisions at $\sqrt{s}=7$ TeV

... S. Abdullin, M. Albrow, J. Anderson, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, I. Bloch, K. Burkett, J.N. Butler, V. Chetluru, H.W.K. Cheung, F. Chlebana, V.D. Elvira, I. Fisk, J. Freeman, Y. Gao, D. ... See full document

31

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

... J. Cummings 176 , M. Curatolo 47 , C. Cuthbert 150 , H. Czirr 141 , P. Czodrowski 3 , S. D’Auria 53 , M. D’Onofrio 74 , M.J. Da Cunha Sargedas De Sousa 126a,126b , C. Da Via 84 , W. Dabrowski 38a , A. Dafinca 120 ... See full document

24

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

... 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, ... 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 b → 0 μ + μ − decay, ... See full document

25

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

... We congratulate our colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their ... See full document

38

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

... (FCNC) decays are particularly sensitive to the effect of new physics, since such decays are highly suppressed in the ...decay, B 0 → K ∗ 0 µ + µ − (K ∗ 0 indicates the K ∗ ( 892 ) 0 , and ... See full document

36

Search For Lepton Flavour Violating Decays Of Heavy Resonances And Quantum Black Holes To An E Mu Pair In Proton-proton Collisions At Root 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 Root S=8 Tev

... the impact of additional pp interactions in the same bunch crossing (pileup) on the selection efficiency, the calorimeter isolation is corrected for the average energy density in the event [41]. Further reduction of ... See full document

26

Search for neutral MSSM Higgs bosons decaying to mu(+) mu(-) in pp collisions at root s=7 and 8 TeV

Search for neutral MSSM Higgs bosons decaying to mu(+) mu(-) in pp collisions at root s=7 and 8 TeV

... A search for neutral Higgs bosons predicted in the minimal supersymmetric standard model (MSSM) for μ + μ − decay channels is ...experiment at the LHC in proton–proton collisions at centre-of-mass ... See full document

27

Search for neutral MSSM Higgs bosons decaying to $\mu^{+} \mu^{-}$ in pp collisions at $ \sqrt{s} =$ 7 and 8 TeV

Search for neutral MSSM Higgs bosons decaying to $\mu^{+} \mu^{-}$ in pp collisions at $ \sqrt{s} =$ 7 and 8 TeV

... Additional corrections are applied to the signal efficiency to take into account differences be- tween data and simulation in the muon trigger, reconstruction, and isolation efficiencies. A correction is also applied to ... See full document

38

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

... RAS and RFBR (Russia); MESTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand); TUBITAK and TAEK (Turkey); NASU and SFFR (Ukraine); STFC ... See full document

30

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

... flavour violation (LFV) has not been ob- served in the charged lepton sector, where neutrino-induced LFV is predicted to be ex- tremely small in the Standard Model (SM). The study of possible LFV processes involv- ing ... See full document

33

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

... S. Abdullin, M. Albrow, J. Anderson, L.A.T. Bauerdick, A. Beretvas, J. Berryhill, P.C. Bhat, I. Bloch, K. Burkett, J.N. Butler, V. Chetluru, H.W.K. Cheung, F. Chlebana, V.D. Elvira, I. Fisk, J. Freeman, Y. Gao, D. ... See full document

27

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

... trees discriminator trained to distinguish the signal from backgrounds. The results are cross- checked with an alternate analysis that fits the collinear mass distribution after applying selec- tion criteria on kinematic ... See full document

48

Search for an L-mu - L-tau gauge boson using Z -gt; 4 mu events in proton-proton collisions at root s=13 TeV

Search for an L-mu - L-tau gauge boson using Z -gt; 4 mu events in proton-proton collisions at root s=13 TeV

... sought at the CERN ...μ decays further reduces the background con- ...the search comes from resonant Z production and de- cay to 4 μ from the annihilation diagram in ... See full document

25

Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

Search for a Heavy Neutral Particle Decaying to $e\mu$, $e\tau$, or $\mu\tau$ in $pp$ Collisions at $\sqrt{s}=8$ TeV with the ATLAS Detector

... G.N. Hamity 146c , P.G. Hamnett 42 , L. Han 33b , K. Hanagaki 118 , K. Hanawa 156 , M. Hance 15 , P. Hanke 58a , R. Hanna 137 , J.B. Hansen 36 , J.D. Hansen 36 , M.C. Hansen 21 , P.H. Hansen 36 , K. Hara 161 , A.S. Hard ... 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

... The discovery of the Higgs boson [1–3] has generated great interest in exploring its prop- erties. In the standard model (SM), lepton flavour violating (LFV) decays of the Higgs bo- son are forbidden. Such ... See full document

44

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

... and B( B 0 → µ + µ − ) = ( ...[13], D0 [14], ATLAS [15], CMS [16], and LHCb [17] experiments have all published limits on these ...decay B 0 s → µ + µ − with B( B 0 ... See full document

31

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

... C. Doglioni 94 , J. Dolejsi 139 , Z. Dolezal 139 , M. Donadelli 78d , S. Donati 69a,69b , P. Dondero 68a,68b , J. Donini 37 , M. D’Onofrio 88 , J. Dopke 141 , A. Doria 67a , M.T. Dova 86 , A.T. Doyle 55 , E. ... See full document

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