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首页> 外文期刊>European physical journal >Updated measurement of time-dependent (CP) -violating observables in ({{B} ^0_{s}} ightarrow J/psi K^+ K^-) decays
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Updated measurement of time-dependent (CP) -violating observables in ({{B} ^0_{s}} ightarrow J/psi K^+ K^-) decays

机译:更新时间依赖于时间(cp ) - oviolating可观察到的测量({{b} ^ 0_ {s}} lightarrow j / psi k ^ + k ^ - )衰减

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The decay-time-dependent $$CP$$ CP asymmetry in $${{B} ^0_{s}} ightarrow J/psi {{K} ^+} {{K} ^-} $$ Bs0→J/ψK+K- decays is measured using proton–proton collision data, corresponding to an integrated luminosity of $$1.9,mathrm{fb}^{-1} $$ 1.9fb-1, collected with the LHCb detector at a centre-of-mass energy of $$13,mathrm {TeV}$$ 13TeV in 2015 and 2016. Using a sample of approximately 117 000 signal decays with an invariant $${{K} ^+} {{K} ^-} $$ K+K- mass in the vicinity of the $$phi (1020)$$ ?(1020) resonance, the $$CP$$ CP-violating phase $$phi _s$$ ?s is measured, along with the difference in decay widths of the light and heavy mass eigenstates of the $${{B} ^0_{s}} $$ Bs0-$${{overline{B}{}} {}^0_{s}} $$ Bˉs0 system, $$Delta Gamma _s$$ ΔΓs. The difference of the average $${{B} ^0_{s}} $$ Bs0 and $${{B} ^0} $$ B0 meson decay widths, $$Gamma _s-Gamma _d$$ Γs-Γd, is determined using in addition a sample of $${{B} ^0} ightarrow J/psi {{K} ^+} {{pi } ^-} $$ B0→J/ψK+π- decays. The values obtained are $$phi _s = -0.083pm 0.041pm 0.006mathrm { ,rad} $$ ?s=-0.083±0.041±0.006rad, $$Delta Gamma _s = 0.077 pm 0.008 pm 0.003 {mathrm { ,ps^{-1}}} $$ ΔΓs=0.077±0.008±0.003ps-1 and $$Gamma _s-Gamma _d = -0.0041 pm 0.0024 pm 0.0015{mathrm { ,ps^{-1}}} $$ Γs-Γd=-0.0041±0.0024±0.0015ps-1, where the first uncertainty is statistical and the second systematic. These are the most precise single measurements of these quantities to date and are consistent with expectations based on the Standard Model and with a previous LHCb analysis of this decay using data recorded at centre-of-mass energies 7 and 8 TeV. Finally, the results are combined with recent results from $${{B} ^0_{s}} ightarrow J/psi {{pi } ^+} {{pi } ^-} $$ Bs0→J/ψπ+π- decays obtained using the same dataset as this analysis, and with previous independent LHCb results.
机译:衰减时间依赖于$$ {{b} ^ 0_ {s}} lightarrow j / psi {{k} ^ +} {{k} ^ - } $$ bs0→使用质子 - 质子碰撞数据测量j /ψk+ k-衰减,对应于$$ 1.9 , mathrm {fb} ^ {-1} $$ 1.9fb-1的集成光度,与LHCB探测器收集2015年和2016年,13 , mathrm {Tev} $$ 13tev的质量能源。使用大约117 000个信号衰变的样本,不变$$ {{k} ^} {{k} ^ $$ phi附近的$$ k + k-质量(1020)$$?(1020)谐振,$$ CP $$ CP违规阶段$$ PHI _S $$?S正在衡量以及R $$ {{b} ^ 0_ {s}} $$ bs0 - $$ {{ overline {b} {}}}}}}} {}}}}}} {}}}}}}}}}}}}}}}}}}}}}}}}} { S}} $$bˉs0系统,$$ delta gamma _s $$Δγs。平均$$ {{b} ^ 0_ {s}} $$ bs0和$$ {{b} ^ 0} $$ b0 meson衰减宽度,$$ gamma _s- gamma _d $$γs- Γd是使用$$ {{b} ^ 0} lightarrow j / psi {{k} ^ +} {{ pi} ^ - } $$ b0→j /ψk+π-衰减。所获得的值是$$ phi _s = -0.083 pm 0.041 pm 0.006 mathrm {,rad} $$?s = -0.083±0.041±0.006rad,$$ delta gamma _s = 0.077 PM 0.008 PM 0.003 { Mathrm {,PS ^ { - 1}}} $$Δγs= 0.077±0.008±0.003ps-1和$$ gamma _s- gamma _d = -0.0041 pm 0.0024 pm 0.0015 { Mathrm {,ps ^ {-1}}} $$γs-γd= -0.0041±0.0024±0.0015ps-1,其中第一个不确定性是统计和第二系统。这些是迄今为止这些数量的最精确的单一测量值,并与基于标准模型的期望一致,并使用记录在质量中心7和8 Tev的数据进行此衰变的先前LHCB分析。最后,结果与最近的$$ {{b} ^ 0_ {s}}}} lightarrow j / psi {{ pi} ^ +} {{ pi} ^ - } $$ bs0→j /使用与此分析相同的数据集获得的ψπ+π-衰减,并使用先前的独立LHCB结果。

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