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Journal of Modern Optics

Thermal decoherence in mesoscopic interference

Paolo Facchi A

Published Apr 1, 2004• 3 citations
Publisher

Abstract

A double-slit experiment is analysed when the interfering particle has an internal structure and one endeavours to obtain ‘which path’ information by detecting the light that is spontaneously emitted. A compact expression is derived for the visibility of the interference pattern: coherence depends on both the spatial and temporal features of the emission process during the travel of the particle to the screen. A bound is set on the temperature of a fullerene molecule in a double-slit experiment in order that its quantum mechanical coherence be maintained.

DOI
10.1080/09500340408233623

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A double-slit experiment is analysed when the interfering particle has an internal structure and one endeavours to obtain ‘which path’ information by detecting the light that is spontaneously emitted. A compact expression is derived for the visibility of the interference pattern: coherence depends on both the spatial and temporal features of the emission process during the travel of the particle to the screen. A bound is set on the temperature of a fullerene molecule in a double-slit experiment in order that its quantum mechanical coherence be maintained.
A coherent superposition of two Gaussian wavepackets, which freely evolves in time, gives rise to an interference pattern similar to that of the single-particle double-slit Young's experiment. In this paper we show that fringe visibility can be reduced by spontaneous decoherence, which can also destroy quantum coherence when interaction between a system and its surroundings can be neglected. This decoherence is due to fluctuations in the evolution time and, in general, cannot be achieved when simple classical averages are considered. We compare our theoretical results with a C 60 fullerenes interference experiment, where thermal decoherence is not relevant, but the fringe visibility is actually reduced.
Quantum Mechanics The interference pattern arising from light or particles passing through a double slit is a simple experiment that belies the subtleties of interpretation when attempting to describe and understand the effect. For example, determining “which path” the light or particles travel can result in the interference pattern disappearing. Margalit et al. present a new take on interferometry using time (see the Perspective by Arndt and Brand). A clock—i.e., the internal state of a cold atom condensate—was coherently split and brought back together to interfere. Making one-half of the clock tick at a different rate resulted in a change in the interference pattern, possibly as a consequence of the time being a “which path” witness. Science , this issue p. [1205][1]; see also p. [1168][2] [1]: /lookup/doi/10.1126/science.aac6498 [2]: /lookup/doi/10.1126/science.aad0683
We propose a trajectory density formulation of the double-slit interference pattern that reproduces observed fringe intensities without wave superposition. The intensity at screen position x is the weighted density of particle trajectories arriving there, suppressed exponentially by the deflection cost in energy space: I(x) = V_{Trit}(KE) \times \sum_n w_n \cdot \delta\!\left(x - \frac{n\lambda L}{d}\right) \cdot e^{-k|n|} where k = dθ_eff/λ_dB is the coherence parameter set by the effective illumination semiangle θ_eff, and V_Trit(KE) = 2γβ/(1+γ²β²) is a new energy-dependent visibility factor from the Trit framework [1–3]. The parameter k connects to the effective source temperature through the emission physics: higher source temperature → larger emission area → larger θ_eff → larger k → fewer visible fringes. We test the formula against five independent experiments across five orders of magnitude in particle energy and three particle types. For thermionic and Schottky electron sources the formula outperforms standard QM by a factor of 2–6× in R². For cold FEG sources and C60 molecules the formula correctly reduces to QM (k → 0). The C60 result leads to a clean new distinction: V_Trit(KE) applies to elementary particles, where the energy space geometry directly governs wave-particle balance; for composite particles V_Trit = 1 and interference is from the centre-of-mass de Broglie wave. This difference is falsifiable: varying electron energy should reveal a visibility peak at KE = 211.66 keV; varying C60 velocity should show no such peak.