The observed interference phase in the Rydberg atom experiment depends on uniform motion through the inhomogeneous electric field, not on acceleration.
This distribution corre- 5 sponds to a temperature of T = mσ2/kB ≈ 1.2 K, so that λth = p 2πℏ2/(mkBT ) ≈ 0.8 nm
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Comment on "Matter-wave interferometry with helium atoms in low-$l$ Rydberg states''
The observed interference phase in the Rydberg atom experiment depends on uniform motion through the inhomogeneous electric field, not on acceleration.