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[PDF] Top 20 First determination of the CP content of D → ∏+∏−∏0 and D → K +K −∏0

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First determination of the CP content of D → ∏+∏−∏0 and D → K +K −∏0

First determination of the CP content of D → ∏+∏−∏0 and D → K +K −∏0

... π 0 candidates contains a significant combinatoric back- ground from continuum e + e − → u u, ¯ d d ¯ events that hadronise to six ...two D → π + π − π 0 candidates is used to deter- ... See full document

8

First determination of the CP content of D→π+π−π+π− and updated determination of the CP   contents of D→π+π−π0 and D→K+K−π0

First determination of the CP content of D→π+π−π+π− and updated determination of the CP contents of D→π+π−π0 and D→K+K−π0

... The data set analysed consists of e + e − collisions produced by the Cornell Electron Storage Ring (CESR) at √ s = 3 . 77 GeV corre- sponding to an integrated luminosity of 818 pb − 1 and collected with the CLEO-c ... See full document

10

Measurement of the branching fraction and CP content for the decay B-0 -> D*+D*-

Measurement of the branching fraction and CP content for the decay B-0 -> D*+D*-

... T. Schietinger, 64 R. H. Schindler, 64 J. Schwiening, 64 A. Snyder, 64 A. Soha, 64 S. M. Spanier, 64 J. Stelzer, 64 D. Su, 64 M. K. Sullivan, 64 H. A. Tanaka, 64 J. Va’vra, 64 S. R. Wagner, 64 M. Weaver, 64 ... See full document

7

Measurement of the Difference of Time-Integrated CP Asymmetries in D⁰ → K⁻ K⁺ and D⁰ → π⁻ π⁺ Decays

Measurement of the Difference of Time-Integrated CP Asymmetries in D⁰ → K⁻ K⁺ and D⁰ → π⁻ π⁺ Decays

... The first (second) sample contains events that are selected when using the old (new) version of the reconstruction software and are discarded by the new (old) one, while the third sample consists of those events ... See full document

10

Limits on D-0-(D)over-bar(0) mixing and CP violation from the ratio of lifetimes for decay to K-pi(+), K-K+, and pi(-)pi(+)

Limits on D-0-(D)over-bar(0) mixing and CP violation from the ratio of lifetimes for decay to K-pi(+), K-K+, and pi(-)pi(+)

... measurements of this type [10 –13], all of which assumed CP conservation. We also obtain for the first time a measurement of Y 0:8 0:6stat: 0:2syst: %. We are grateful for the excellent ... See full document

7

Measurement of CP asymmetry in B s 0 → D s ∓ K ± decays

Measurement of CP asymmetry in B s 0 → D s ∓ K ± decays

... s 0D ∓ s K ± candidates which extract the CP violating ...The first fit, hence- forth referred to as the sFit , uses the results of the multivariate fit to obtain the so-called ... See full document

31

Measurement of the CP violation parameter A {Γ} in D^{0}→K^{+}K^{ } and D^{0}→π^{+}π^{ } decays

Measurement of the CP violation parameter A {Γ} in D^{0}→K^{+}K^{ } and D^{0}→π^{+}π^{ } decays

... the determination and correction of these residual ...the D 0K − π þ mode, where the time-dependent asymmetry is expected to be ...the D 0 decay time in the range ½0 . ... See full document

10

Measurement of time-dependent CP-violating asymmetries in B-0 ->phi K-S(0), (K+K-KS0), and eta K-'(S)0 decays

Measurement of time-dependent CP-violating asymmetries in B-0 ->phi K-S(0), (K+K-KS0), and eta K-'(S)0 decays

... two parameters, q and r, to represent the tagging infor- mation. The first, q, is already defined in Eq. (1). The parameter r is an event-by-event, flavor-tagging dilution factor determined from Monte Carlo (MC) ... See full document

6

Measurement of CP asymmetry in D 0 → K   K + and D 0 → π   π decays

Measurement of CP asymmetry in D 0 → K K + and D 0 → π π decays

... This analysis uses the data set collected by LHCb corresponding to an integrated luminosity of 3 fb −1 . The data in 2011 (1 fb −1 ) were taken at a centre-of-mass energy of 7TeV and the data in 2012 (2 fb −1 ) were ... See full document

26

Measurement of CP asymmetries and polarisation fractions in Bs0→K∗0K¯∗0 decays

Measurement of CP asymmetries and polarisation fractions in Bs0→K∗0K¯∗0 decays

... The main systematic uncertainties considered are related to the invariant mass fit used to determine the signal and reference event yields, the angular correction, and the determination of the trigger efficiency. ... See full document

28

First observation of the decay D 0 → K − π + μ + μ − in the ρ 0 – ω region of the dimuon mass spectrum

First observation of the decay D 0 → K − π + μ + μ − in the ρ 0 – ω region of the dimuon mass spectrum

... misidentified D 0K − π + π + π − decays are categorised by the presence of candidates involving misidentified pions that did not decay in flight before reaching the most downstream tracking stations, ... See full document

10

Study of the rare decays B-0 -> D-s((*)+)pi(-) and B-0 -> Ds(*)-K+

Study of the rare decays B-0 -> D-s((*)+)pi(-) and B-0 -> Ds(*)-K+

... signals and for various sources of background. The branching fraction of the charmless background is not well measured; therefore we need to estimate the sum of the reflection and charmless background (referred to as ... See full document

7

Measurement of time-dependent CP asymmetries and the CP-odd fraction in the decay B-0 -> D*+D*-

Measurement of time-dependent CP asymmetries and the CP-odd fraction in the decay B-0 -> D*+D*-

... time-dependent CP asymmetry, obtained from a com- bined analysis of the time dependence of flavor-tagged decays and the one-dimensional angular distribution of the decay ... See full document

7

Measurement of CP asymmetries in the decays B 0 → K *0 μ + μ − and B + → K + μ + μ −

Measurement of CP asymmetries in the decays B 0 → K *0 μ + μ − and B + → K + μ + μ −

... B 0K0 (→ K + π − )µ + µ − and B + → K + µ + µ − are rare decays 1 of B mesons involving b → s quark-level transitions, and have small branching fractions, mea- sured as ...direct ... See full document

19

Search for CP violation in D+ >K K+π+ decays

Search for CP violation in D+ >K K+π+ decays

... For D þ ! K þ þ , five different sets of bins in each scheme are ...S CP values with a Gaussian fit is shown in ...the D þ and the D Dalitz plots are driven only by statistical ... See full document

14

Measurement of CP observables in B± → D(⁎)K± and B± → D(⁎)π± decays

Measurement of CP observables in B± → D(⁎)K± and B± → D(⁎)π± decays

... ] D h − decays, in which h + 1 , h − 2 and h − can each represent either a charged kaon or pion and the D-meson decay products are denoted inside square brackets, have been studied at the B factories ... See full document

15

Measurements of branching fractions and CP-violating asymmetries in B-0 ->pi(+)pi(-), K+ pi(-), K+K- decays

Measurements of branching fractions and CP-violating asymmetries in B-0 ->pi(+)pi(-), K+ pi(-), K+K- decays

... tailed description of the BABAR detector is presented in Ref. [6], and more details on the analysis technique are given in Ref. [7], which describe our previous measure- ments of these quantities. Other measurements of ... See full document

7

Construction of Strong Diophantine Quadruples and Pell Equation

Construction of Strong Diophantine Quadruples and Pell Equation

... property D(n), n  Z  { 0 } , if a i a j  n , a perfect square for all 1  i  j  m and such a set is called a Diophantine m-tuples with property ...property D(n) for any arbitrary integer n [1] ... See full document

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SIMULTANEOUS STABILITY OF D=0 AND D≠0 FOR MULTIPLICATIVE VIABILITIES AT TWO LOCI

SIMULTANEOUS STABILITY OF D=0 AND D≠0 FOR MULTIPLICATIVE VIABILITIES AT TWO LOCI

... It has generally been assumed that in the general (asymmetric) multiplicative viability model results similar to those of the previous paragraph hold, namely, that as the value o[r] ... See full document

13

First observation of the decay Bs0→K*0K*0

First observation of the decay Bs0→K*0K*0

... V. Fernandez Albor 36 , M. Ferro-Luzzi 37 , S. Filippov 32 , C. Fitzpatrick 46 , M. Fontana 10 , F. Fontanelli 19 , i , R. Forty 37 , M. Frank 37 , C. Frei 37 , M. Frosini 17 , 37 , f , S. Furcas 20 , A. Gallas Torreira ... See full document

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