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Novel coupled channel framework connecting the quark model and lattice QCD for the near-threshold $$D_s$$ states

クォーク模型と格子QCDを結びつける新しいチャネル結合方式; 閾値近傍の$$D_s$$状態の解析

Yang, Z.*; Wang, G.-J.*; Wu, J.-J.*; 岡 眞   ; Zhu, S.-L.*

Yang, Z.*; Wang, G.-J.*; Wu, J.-J.*; Oka, Makoto; Zhu, S.-L.*

閾値近傍のハドロン共鳴を有限サイズの格子QCDのデータを用いて解析する新しい手法を提案し、正パリティの$$D_s$$メソンのスペクトルに応用した。ハミルトニアン有効理論にクォーク模型,クォークペア生成,DK相互作用の情報を入れてベアな状態と散乱状態の結合を取り入れた。4個の$$D_s$$状態のうち、$$0^+$$$$1^+$$の状態は散乱状態と強く混合する。一方で、$$1^+$$$$2^+$$はほとんどベアなクォーク模型状態で記述できる。有限格子サイズでのレベル交差が再現されることを示した。

A novel framework is proposed to extract near-threshold resonant states from finite-volume energy levels of lattice QCD and is applied to elucidate structures of the positive parity $$D_s$$. The quark model, the quark-pair-creation mechanism and $$D^{(*)}K$$ interaction are incorporated into the Hamiltonian effective field theory. The bare $$1^+$$ $$cbar s$$ states are almost purely given by the states with heavy-quark spin bases. The physical $$D^*_{s0}(2317)$$ and $$D^*_{s1}(2460)$$ are the mixtures of bare $$cbar s$$ core and $$D^{(*)}K$$ component, while the $$D^*_{s1}(2536)$$ and $$D^*_{s2}(2573)$$ are almost dominated by bare $$cbar{s}$$. Furthermore, our model well reproduce the clear level crossing of the $$D^*_{s1}(2536)$$ with the scattering state at a finite volume.

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パーセンタイル:96.46

分野:Physics, Multidisciplinary

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