Abstract

Although experimental efforts have been active for about 30 years, a direct laboratory observation of vacuum magnetic birefringence, due to vacuum fluctuations, still needs confirmation: the predicted birefringence of vacuum is Delta n = 4.0times 10^{-24} @ 1 T. Key ingredients of a polarimeter for detecting such a small birefringence are a long optical path within the magnetic field and a time dependent effect. To lengthen the optical path a Fabry–Perot is generally used with a finesse ranging from {{mathscr {F}}} approx 10^4 to {{mathscr {F}}} approx 7times 10^5. Interestingly, there is a difficulty in reaching the predicted shot noise limit of such polarimeters. We have measured the ellipticity and rotation noises along with Cotton-Mouton and Faraday effects as a function of the finesse of the cavity of the PVLAS polarimeter. The observations are consistent with the idea that the cavity mirrors generate a birefringence-dominated noise whose ellipticity is amplified by the cavity itself. The optical path difference sensitivity at 10;hbox {Hz} is S_{Delta {{mathscr {D}}}}=6times 10^{-19};hbox {m}/sqrt{mathrm{Hz}}, a value which we believe is consistent with an intrinsic thermal noise in the mirror coatings. Our findings prove that the continuous efforts to increase the finesse of the cavity to improve the sensitivity has reached a limit.

Highlights

  • ObjectivesLet us remind the reader that the aim of the present work is to study the signal-to-noise ratio in the PVLAS apparatus as a function of the finesse of the Fabry–Perot cavity

  • E2 c2 − B2 + Ae μ0 +7 E ·B c (1)which takes into account vacuum fluctuations with the creation of electron-positron pairs

  • A small Faraday effect is generated in the mirrors due to the stray field but this rotation is negligible with respect to the rotation generated in the gas

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Summary

Objectives

Let us remind the reader that the aim of the present work is to study the signal-to-noise ratio in the PVLAS apparatus as a function of the finesse of the Fabry–Perot cavity. The main goal of the present work is to show whether the noise present in the two configurations of the polarimeter is dominated by an ellipticity noise generated by a fluctuating birefringence inside the cavity, i.e. whether it is multi-

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