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Z_b(10610)^pm and Z_b(10650)^pm as the B^*bar{B} and B^*bar{B}^(*) molecular states

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arxiv 1106.2968 v1 pith:OS27YQOB submitted 2011-06-15 hep-ph hep-exnucl-exnucl-th

$Z_b(10610)^\pm$ and $Z_b(10650)^\pm$ as the $B^*\bar{B}$ and $B^*\bar{B}^{*}$ molecular states

classification hep-ph hep-exnucl-exnucl-th
keywords molecularstatesframeworkquiteseveralalonebottomoniabound
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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abstract

In the framework of the one-boson-exchange model, we have studied the interaction of the $B^*\bar{B}$ and $B^*\bar{B}^{*}$ system. After considering the S-wave and D-wave mixing, we notice that both $Z_b(10610)^\pm$ and $Z_b(10650)^\pm$ can be interpreted as the $B^*\bar{B}$ and $B^*\bar{B}^{*}$ molecular states quite naturally. Within the same framework, there also exist several molecular charmonia including X(3872) and several other molecular bottomonia, which are the partners of $Z_b(10610)$ and $Z_b(10650)$. The long-range one-pion-exchange force alone is strong enough to form these loosely bound molecular states, which ensures the numerical results quite model-independent and robust.

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