We discuss limits on the noise strength parameter in mass-proportional-coupled wave-function collapse models implied by bulk heating effects and examine the role of the noise power spectrum in comparing experiments of different types. This comparison utilizes a calculation of the rate of heating through phonon excitation implied by a general noise power spectrum lambda(omega). We find that, in the standard heating formula, the reduction rate lambda is replaced by lambda(eff) = 2/3 pi(3/2 )integral d(3) we(-(w)over-right-arrow2) (w)over-right-arrow(2)lambda (omega(L)(w)over-right-arrow/r(c))) with omega(L)(q)over-right-arrow being the longitudinal acoustic-phonon frequency as a function of wave number (q)over-right-arrow, and with r c being the noise correlation length. Hence if the noise power spectrum is cut off below omega(L)(vertical bar(q)over-right-arrow vertical bar similar to r(c)(-1)), the bulk heating rate is sharply reduced, allowing compatibility with current experimental results. We suggest possible new bulk heating experiments that can be performed subject to limits placed by natural heating from radioactivity and cosmic rays. The proposed experiments exploit the vanishing of thermal transport in the low-temperature limit.
Bulk heating effects as tests for collapse models / Adler, Stephen L.; Vinante, Andrea. - In: PHYSICAL REVIEW A. - ISSN 2469-9926. - 97:5(2018). [10.1103/PhysRevA.97.052119]
Bulk heating effects as tests for collapse models
Vinante, Andrea
2018-01-01
Abstract
We discuss limits on the noise strength parameter in mass-proportional-coupled wave-function collapse models implied by bulk heating effects and examine the role of the noise power spectrum in comparing experiments of different types. This comparison utilizes a calculation of the rate of heating through phonon excitation implied by a general noise power spectrum lambda(omega). We find that, in the standard heating formula, the reduction rate lambda is replaced by lambda(eff) = 2/3 pi(3/2 )integral d(3) we(-(w)over-right-arrow2) (w)over-right-arrow(2)lambda (omega(L)(w)over-right-arrow/r(c))) with omega(L)(q)over-right-arrow being the longitudinal acoustic-phonon frequency as a function of wave number (q)over-right-arrow, and with r c being the noise correlation length. Hence if the noise power spectrum is cut off below omega(L)(vertical bar(q)over-right-arrow vertical bar similar to r(c)(-1)), the bulk heating rate is sharply reduced, allowing compatibility with current experimental results. We suggest possible new bulk heating experiments that can be performed subject to limits placed by natural heating from radioactivity and cosmic rays. The proposed experiments exploit the vanishing of thermal transport in the low-temperature limit.File | Dimensione | Formato | |
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2018_PRA_Bulkheating.pdf
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