104,395 research outputs found

    Fluctuations of the vacuum energy density of quantum fields in curved spacetime via generalized zeta functions

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    For quantum fields on a curved spacetime with an Euclidean section, we derive a general expression for the stress energy tensor two-point function in terms of the effective action. The renormalized two-point function is given in terms of the second variation of the Mellin transform of the trace of the heat kernel for the quantum fields. For systems for which a spectral decomposition of the wave opearator is possible, we give an exact expression for this two-point function. Explicit examples of the variance to the mean ratio Δ=(2)/(2)\Delta' = (-^2)/(^2) of the vacuum energy density ρ\rho of a massless scalar field are computed for the spatial topologies of Rd×S1R^d\times S^1 and S3S^3, with results of Δ(Rd×S1)=(d+1)(d+2)/2\Delta'(R^d\times S^1) =(d+1)(d+2)/2, and Δ(S3)=111\Delta'(S^3) = 111 respectively. The large variance signifies the importance of quantum fluctuations and has important implications for the validity of semiclassical gravity theories at sub-Planckian scales. The method presented here can facilitate the calculation of stress-energy fluctuations for quantum fields useful for the analysis of fluctuation effects and critical phenomena in problems ranging from atom optics and mesoscopic physics to early universe and black hole physics.Comment: Uses revte

    Nonsymmetric transverse vibrations of truncated conical shells technical report no. 3

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    Resonant frequencies and associated mode shapes of truncated conical shells over wide range of geometrical and modal parameter

    Properties of solutions of stochastic differential equations driven by the G-Brownian motion

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    In this paper, we study the differentiability of solutions of stochastic differential equations driven by the GG-Brownian motion with respect to the initial data and the parameter. In addition, the stability of solutions of stochastic differential equations driven by the GG-Brownian motion is obtained
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