1,721,085 research outputs found

    Induced quantum gravity from heat kernel expansion

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    The asymptotic expansion of the heat kernel is employed to derive the Einstein action from the matter effective action. The advantages of this approach are discussed. We point out some problems arising when scalar fields, nonminimally coupled to the background geometry, are used as fundamental pregeometric objects

    Coleman-weinberg model in Einstein space-time

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    We study radiative, symmetry breaking, h ht ('olemav,- ~,Veinb(,r(_,, in the /eometry of a .~tatic Einstein mfivcrsc. \Vc prove that the syvmnetric gv'om,d state (oi~510 > - . r in a nouminimally coupled mass- 1,,s,~ ).r theory, can l)et'onw, u,,st al)lc at high curvature only if 0 "4 ~ )..;: 1. As far as mas.sles~ scalar (~I".I) is ('oncerned, we find lhat pha.~c transitions can already oc('m" at low cttrvature. These conchisions arc improvc(l by nwans of r,*norm:diz:alion group tcwhniques

    Symmetry restoration in conformally flat metrics

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    We study symmetry restoration in a curved-background metric. Massless scalar QED is considered in the de Sitter space-time. The radius of the cosmological-event horizon corresponding to the critical temperature turns out to be of the order of the Compton wave-length of the vector bosom Quite similarly, the Gross-Neveau model in the twodimensional Schwarzschild background shows symmetry restoration when the radius of the black-hole horizon becomes comparable with the Compton wave-length of the spinor

    Curvature and symmetry breaking: An induced-action approach

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    We recover the general form of the one-loop effective potential for a Ar 4 theory, nonminimally coupled to a constant-curvature background geometry, in the low-energy limit, i.e. for small curvature. Renormalization is carried out and the massless limit of the renormalized theory is performed. Then we study the symmetry properties of the vacuum state according to the value of the nonminimal coupling constant ~ and the sign of the curvature
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