Ultra-high Compton Frequency, Parity Independent, Mesoscopic Schr\"odinger Cat Atom Interferometer with Heisenberg Limited Sensitivity

TL;DR

This paper proposes a mesoscopic Schrödinger cat atom interferometer that achieves near-Heisenberg limited sensitivity at ultrahigh Compton frequencies, with parity-dependent fringe narrowing, enhancing precision in gyroscopes and clocks.

Contribution

The authors introduce a protocol for a Schrödinger cat atom interferometer that reaches near-Heisenberg limit sensitivity and exhibits parity-dependent interference effects at ultrahigh frequencies.

Findings

Achieves Heisenberg limited sensitivity within a factor of √2.

Demonstrates parity-dependent fringe narrowing in the interferometer.

Enhances effective frequency and sensitivity in accelerometers and atomic clocks.

Abstract

We present a protocol for an atomic interferometer that reaches the Heisenberg Limit (HL), within a factor of $\sim$ $\sqrt{2}$, via collective state detection and critical tuning of one-axis twist spin squeezing. It generates a Schr\"odinger cat (SC) state, as a superposition of two extremal collective states. When this SC interferometer is used as a gyroscope, the interference occurs at an ultrahigh Compton frequency, corresponding to a mesoscopic single object with a mass of $Nm$, where $N$ is the number of particles in the ensemble, and $m$ is the mass of each particle. For $^{87}$Rb atoms, with $N=10^{6}$, for example, the intereference would occur at a Compton frequency of $\sim$ $2 \times 10^{31}$ Hz. Under this scheme, the signal is found to depend critically on the parity of $N$. We present two variants of the protocol. Under Protocol A, the fringes are narrowed by a factor of $N$ for one parity, while for the other parity the signal is zero. Under Protocol B, the fringes are narrowed by a factor of $N$ for one parity, and by a factor of $\sqrt{N}$ for the other parity. Both protocols can be modified in a manner that reverses the behavior of the signals for the two parities. Over repeated measurements under which the probability of being even or odd is equal, the averaged sensitivity is smaller than the HL by a factor of $\sim$ $\sqrt{2}$ for both versions of the protocol. We show that when the SC interferometer is configured as an accelerometer, the effective two-photon wave vector is enhanced by a factor of $N$, leading to the same degree of enhancement in sensitivity. We also show that such a mesoscopic single object can be used to increase the effective base frequency of an atomic clock by a factor of $N$, with a sensitivity that is equivalent to the HL, within a factor of $\sim$ $\sqrt{2}$.