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Model-independent measurement of the e [equation] e [equation] [equation] HZ cross section at a future e [equation] e [equation] linear collider using hadronic Z decays

机译:使用强子Z衰减对未来e [equation] e [equation]线性对撞机的e [equation] e [equation] [equation] HZ横截面的模型独立测量

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A future (mathrm{e}^{+} mathrm{e}^{-} ) collider, such as the ILC or CLIC, would allow the Higgs sector to be probed with a precision significantly beyond that achievable at the High-Luminosity LHC. A central part of the Higgs programme at an (mathrm{e}^{+} mathrm{e}^{-} ) collider is the model-independent determination of the absolute Higgs couplings to fermions and to gauge bosons. Here the measurement of the (mathrm{e}^{+} mathrm{e}^{-} ightarrow mathrm{H} mathrm{Z} ) Higgsstrahlung cross section, using the recoil mass technique, sets the absolute scale for all Higgs coupling measurements. Previous studies have considered (upsigma (mathrm{e}^{+} mathrm{e}^{-} ightarrow mathrm{H} mathrm{Z})) with (mathrm{Z} ightarrow {ell } ^{+} {ell } ^{-} ), where ({ell } = mathrm{e},,{upmu } ). In this paper it is shown for the first time that a near model-independent recoil mass technique can be extended to the hadronic decays of the (mathrm{Z} ) boson. Because the branching ratio for (mathrm{Z} ightarrow mathrm{q} {overline{mathrm{q}}} ) is approximately ten times greater than for (mathrm{Z} ightarrow {ell } ^{+} {ell } ^{-} ), this method is statistically more powerful than using the leptonic decays. For an integrated luminosity of 500?( ext {fb}^{-1}) at a centre-of-mass energy of (sqrt{s} =350~ ext {GeV} ) at CLIC, (upsigma (mathrm{e}^{+} mathrm{e}^{-} ightarrow mathrm{H} mathrm{Z})) can be measured to ({pm }1.8~%) using the hadronic recoil mass technique. A similar precision is found for the ILC operating at (sqrt{s} =350~ ext {GeV} ). The centre-of-mass dependence of this measurement technique is discussed, arguing for the initial operation of a future linear collider at just above the top-pair production threshold.
机译:未来的(mathrm {e} ^ {+} mathrm {e} ^ {-})对撞机,例如ILC或CLIC,将使探测Higgs扇区的精度大大超过高亮度LHC所能达到的精度。 。在(mathrm {e} ^ {+} mathrm {e} ^ {-})对撞机上,Higgs程序的中心部分是与费米子和玻色子的绝对Higgs耦合的模型无关确定。此处,使用反冲质量技术对(mathrm {e} ^ {+} mathrm {e} ^ {-} ightarrow mathrm {H} mathrm {Z})的Higgsstrahlung横截面进行测量,可设置所有Higgs耦合的绝对比例测量。先前的研究已经考虑了(mathrm {Z} ightarrow {ell} ^ {+} {ell}(upsigma(mathrm {e} ^ {+} mathrm {e} ^ {-} ightarrow mathrm {H} mathrm {Z})) } ^ {-}),其中({ell} = mathrm {e} ,, {upmu})。在本文中,首次证明可以将近乎模型无关的后坐质量技术扩展到(mathrm {Z})玻色子的强子衰变上。因为(mathrm {Z} ightarrow mathrm {q} {overline {mathrm {q}}})的分支比率大约是(mathrm {Z} ightarrow {ell} ^ {+} {ell} ^ { -}),从统计上讲,此方法比使用轻子衰变更强大。对于在CLIC处(sqrt {s} = 350〜ext {GeV})的质心能量为500?(ext {fb} ^ {-1})的综合亮度,(upsigma(mathrm {e} ^ {+} mathrm {e} ^ {-} ightarrow mathrm {H} mathrm {Z}))可使用强子反冲质量技术测量为({pm} 1.8〜%)。对于在(sqrt {s} = 350〜ext {GeV})下运行的ILC,发现了类似的精度。讨论了这种测量技术的质心相关性,并提出了未来线性对撞机的初始操作应在最高对生产阈值之上的问题。

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