首页> 外文OA文献 >QCD Compositeness as Revealed in Exclusive Vector Boson Reactions through Double-Photon Annihilation: $e^+ e^- o \gamma \gamma^\ast o \gamma V^0 $ and $e^+ e^- o \gamma^\ast \gamma^\ast o V^0 V^0$
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QCD Compositeness as Revealed in Exclusive Vector Boson Reactions through Double-Photon Annihilation: $e^+ e^- o \gamma \gamma^\ast o \gamma V^0 $ and $e^+ e^- o \gamma^\ast \gamma^\ast o V^0 V^0$

机译:独家矢量玻色子反应中显示的QCD复合度   通过双光子湮灭:$ e ^ + e ^ - \到\ gamma \ gamma ^ \ ast \ to   \ gamma V ^ 0 $和$ e ^ + e ^ - \ to \ gamma ^ \ ast \ gamma ^ \ ast \ to V ^ 0 V ^ 0 $

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摘要

We study the exclusive double-photon annihilation processes, $e^+ e^- \to\gamma \gamma^\ast\to \gamma V^0$ and $e^+ e^- \to \gamma^\ast \gamma^\ast \toV^0_a V^0_b,$ where the $V^0_i$ is a neutral vector meson produced in theforward kinematical region: $s \gg -t$ and $-t \gg \Lambda_{\rm QCD}^2$. Weshow how the differential cross sections $\frac{d\sigma}{dt}$, as predicted byQCD, have additional falloff in the momentum transfer squared $t$ due to theQCD compositeness of the hadrons, consistent with the leading-twistfixed-$\theta_{\rm CM} $ scaling laws. However, even though they are exclusivechannels and not associated with the conventional electron-positronannihilation process $e^+ e^- \to \gamma^\ast \to q \bar q,$ these total crosssections $\sigma(e^+ e^- \to \gamma V^0) $ and $\sigma(e^+ e^- \to V^0_aV^0_b),$ integrated over the dominant forward- and backward-$\theta_{\rm CM}$angular domains, scale as $1/s$, and thus contribute to the leading-twistscaling behavior of the ratio $R_{e^+ e^-}$. We generalize these results toexclusive double-electroweak vector-boson annihilation processes accompanied bythe forward production of hadrons, such as $e^+ e^- \to Z^0 V^0$ and $e^+ e^-\to W^-\rho^+$. These results can also be applied to the exclusive productionof exotic hadrons such as tetraquarks, where the cross-section scaling behaviorcan reveal their multiquark nature.
机译:我们研究了唯一的双光子an灭过程,$ e ^ + e ^-\ to \ gamma \ gamma ^ \ ast \ to \ gamma V ^ 0 $和$ e ^ + e ^-\ to \ gamma ^ \ ast \ gamma ^ \ ast \ toV ^ 0_a V ^ 0_b,$,其中$ V ^ 0_i $是在向前的运动区域产生的中性矢量介子:$ s \ gg -t $和$ -t \ gg \ Lambda _ {\ rm QCD } ^ 2 $。我们展示了QCD所预测的微分横截面$ \ frac {d \ sigma} {dt} $,由于强子的QCD复杂性,动量传递平方t $ t的附加衰减如何,与前导扭曲定点$ \ theta _ {\ rm CM} $缩放定律。但是,即使它们是互斥通道,并且与常规电子正电子ni灭过程无关,也等于这些总横截面$ \ sigma(e ^ + e ^-\ to \ gamma V ^ 0)$和$ \ sigma(e ^ + e ^-\ to V ^ 0_aV ^ 0_b),$在优势前向和后向$ \ theta _ {\ rm CM} $上积分角域,缩放为$ 1 / s $,因此有助于比率$ R_ {e ^ + e ^-} $的超前扭曲行为。我们将这些结果推广到伴随强子正向产生的排他性双电弱矢量玻色子an灭过程,例如$ e ^ + e ^-\到Z ^ 0 V ^ 0 $和$ e ^ + e ^-\到W ^ -\ rho ^ + $。这些结果也可以应用于异质强子的独占生产,例如四夸克,其截面结垢行为可以揭示它们的多夸克性质。

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