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Hidden functional relation in Large-N Quark-Monopole system at finite temperature

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arxiv hep-th/0105039 v3 pith:R2F4LCUA submitted 2001-05-03 hep-th

classification hep-th
keywords relationpotentialbifurcationdefinedfinitefunctionalphysicalquark-monopole
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

The quark-monopole potential is computed at finite temperature in the context of $AdS/CFT$ correspondence. It is found that the potential is invariant under $g \to 1/g$ and $U_T \to U_T / g$. As in the quark-quark case there exists a maximum separation between quark and monopole, and $L$-dependence of the potential exhibits a bifurcation behavior. We find a functional relation $dE_{QM}^{Reg} / dL = [(1/E_{(1,0)}^{Reg}(U_0))^2 + (1/E_{(0,1)}^{Reg}(U_0))^2]^{-1/2}$ which is responsible for the bifurcation. The remarkable property of this relation is that it makes a relation between physical quantities defined at the $AdS$ boundary through a quantity defined at the bulk. The physical implication of this relation for the existence of the extra dimension is speculated.

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