Quantum Noise Fraction and the Thermal Frontier in High-Frequency Gravitational Wave Detection

TL;DR

This paper introduces the quantum noise fraction diagnostic to assess the maximum quantum-enhanced sensitivity in high-frequency gravitational wave detectors, revealing thermal limitations and proposing a feasible resonator-based detection scheme.

Contribution

It defines the quantum noise fraction diagnostic, analyzes thermal and quantum regimes in high-frequency detectors, and proposes a resonator-based detector employing squeezed phononic states.

Findings

Resonant mass detectors are thermally limited below ~230 MHz at dilution temperatures.

Quantum regime becomes accessible above the thermal frontier at \, ext{Hz} = k_B T \, ext{ln} 3.

A proposed array of resonators with squeezing reaches sensitivity still far above the stochastic background bound.

Abstract

We introduce a diagnostic -- the quantum noise fraction $\beta$ -- that determines the maximum sensitivity improvement achievable through quantum enhancement for any gravitational wave detector. Applied to the landscape of proposed high-frequency (kHz-GHz) detectors, this diagnostic reveals that resonant mass detectors operating through tidal coupling are thermally dominated ($\beta \approx 0$) at all frequencies below ~230 MHz at dilution temperatures, rendering squeezing and entanglement limited in effectiveness. Only above this thermal frontier, defined by $\hbar \omega = k_B T \ln 3$, does the quantum regime become accessible. We identify a single concrete realization: a bulk acoustic wave resonator at 1 GHz and 10 mK ($\beta = 0.98$), and propose a gravitational wave detector employing squeezed phononic states via circuit QED readout. An array of $10^4$ such resonators with 10 dB mechanical squeezing reaches $\sqrt{S_h} = 2.1 \times 10^{-22}/\sqrt{\rm Hz}$ -- still a factor ~$10^{12}$ above the BBN bound on stochastic backgrounds at 1 GHz, indicating that the sensitivity gap remains predominantly classical in origin and that concurrent advances in classical detector parameters will be required.