Abstract
The CKM angle γ is measured for the first time from mixing-induced CP violation between {B}_s^0to {D}_s^{mp }{K}^{pm }{pi}^{pm }{pi}^{mp } and {overline{B}}_s^0to {D}_s^{pm }{K}^{mp }{pi}^{mp }{pi}^{pm } decays reconstructed in proton-proton collision data corresponding to an integrated luminosity of 9 fb−1 recorded with the LHCb detector. A time-dependent amplitude analysis is performed to extract the CP-violating weak phase γ − 2βs and, subsequently, γ by taking the {B}_s^0hbox{-} {overline{B}}_s^0 mixing phase βs as an external input. The measurement yields γ = (44 ± 12)° modulo 180°, where statistical and systematic uncertainties are combined. An alternative model-independent measurement, integrating over the five-dimensional phase space of the decay, yields gamma =left({44}_{-13}^{+20}right){}^{circ} modulo 180°. Moreover, the {B}_s^0hbox{-} {overline{B}}_s^0 oscillation frequency is measured from the flavour-specific control channel {B}_s^0to {D}_s^{-}{pi}^{+}{pi}^{+}{pi}^{-} to be ∆ms = (17.757 ± 0.007(stat) ± 0.008(syst)) ps−1, consistent with and more precise than the current world-average value.
Highlights
0 s mixing phase βs as an external input
This paper presents the first measurement of the CKM angle γ with Bs0 → Ds∓K±π±π∓
A coherence factor needs to be introduced as an additional hadronic parameter, which dilutes the observable CP asymmetry since constructive and destructive interference effects cancel when integrated over the entire phase space
Summary
Since the hadronisation process is different f and f decays, their respective amplitude coefficients are distinct (aci = aui ). To ensure that the parameters r and δ do not depend on the convention employed for the amplitude coefficients, the magnitude squared of the hadronic amplitudes is normalised to unity when integrated over the phase space (with four-body phase-space element dΦ4) and the overall strong-phase difference between Ac(x) and Au(x) is set to zero, i.e. Fic(u) ≡ aci(u) Ai(x) 2 dΦ4, Iicj(u) ≡ 2 Re[aci(u) acj(u)∗ Ai(x)A∗j (x)] dΦ4
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