<p>Gravitational waves and ultralight dark matter are among the most compelling frontiers in fundamental physics, motivating proposals for very-long-baseline atom interferometerssuch as AION<sup><CitationRef CitationID="CR1">1</CitationRef></sup>, MAGIS<sup><CitationRef CitationID="CR2">2</CitationRef></sup>, AICE<sup><CitationRef CitationID="CR3">3</CitationRef></sup> and AEDGE<sup><CitationRef CitationID="CR4">4</CitationRef></sup> that aim to detect at&#xa0;frequencies at which ground-based<sup><CitationRef CitationID="CR5">5</CitationRef></sup> and space-borne<sup><CitationRef CitationID="CR6">6</CitationRef></sup> laser interferometers lose sensitivity. Very-long-baseline atom interferometers look for signals by comparing the quantum phase evolution of widely separated atomic ensembles interrogated by a common laser. However, their performance depends critically on suppressing noise sources, particularly laser phase noise. The experimental validation of such noise rejection remains an important challenge. Here we demonstrate a prototype differential atom interferometer based on the single-photon clock transition of fermionic <sup>87</sup>Sr. Thus, we obtain a gradiometer configuration with a species intrinsically suited to kilometre-scale and space-baseline operation. The instrument operates at the standard quantum limit<sup><CitationRef CitationID="CR7">7</CitationRef></sup> with no excess noise beyond atom shot noise. The differential configuration maintains quantum-limited sensitivity in the presence of several radians of artificially injected laser phase noise per shot, which emulates the conditions expected in a very-long-baseline atom interferometer. We also demonstrate the recovery of coherent oscillatory signals across a broad frequency range under fully phase-randomized conditions, a capability that is inaccessible to a single interferometer operating in the same regime. These results provide an experimental validation of the noise-immune measurement principle underlying very-long-baseline atom interferometers and mark an important step towards next-generation quantum sensors for gravitational-wave detection and searches for ultralight dark matter<sup><CitationRef CitationID="CR8">8</CitationRef>,<CitationRef CitationID="CR9">9</CitationRef></sup>.</p>

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A prototype differential atom interferometer for fundamental physics

  • C. F. A. Baynham,
  • R. Hobson,
  • O. Buchmüller,
  • D. Evans,
  • L. Hawkins,
  • L. Iannizzotto Venezze,
  • A. Josset,
  • D. Lee,
  • E. Pasatembou,
  • B. E. Sauer,
  • M. R. Tarbutt,
  • T. Walker,
  • O. Ennis,
  • U. Chauhan,
  • A. Brzakalik,
  • S. Dey,
  • S. Hedges,
  • B. Stray,
  • M. Langlois,
  • K. Bongs,
  • T. Hird,
  • S. Lellouch,
  • M. Holynski,
  • B. Bostwick,
  • J. Chen,
  • Z. Eyler,
  • V. Gibson,
  • T. L. Harte,
  • C. C. Hsu,
  • M. Karzazi,
  • C. Lu,
  • B. Millward,
  • J. Mitchell,
  • N. Mouelle,
  • B. Panchumarthi,
  • J. Scheper,
  • U. Schneider,
  • X. Su,
  • Y. Tang,
  • K. Tkalčec,
  • M. Zeuner,
  • S. Zhang,
  • Y. Zhi,
  • L. Badurina,
  • A. Beniwal,
  • D. Blas,
  • J. Carlton,
  • J. Ellis,
  • C. McCabe,
  • G. Parish,
  • D. Pathak Govardhan,
  • V. Vaskonen,
  • T. Bowcock,
  • K. Bridges,
  • A. Carroll,
  • J. Coleman,
  • G. Elertas,
  • S. Hindley,
  • C. Metelko,
  • H. Throssell,
  • J. N. Tinsley,
  • E. Bentine,
  • M. Booth,
  • D. Bortoletto,
  • N. Callaghan,
  • C. Foot,
  • C. Gómez-Monedero,
  • K. Hughes,
  • A. James,
  • T. Leese,
  • A. Lowe,
  • J. March-Russell,
  • J. Sander,
  • J. Schelfhout,
  • I. Shipsey,
  • D. Weatherill,
  • D. Wood,
  • S. N. Balashov,
  • M. G. Bason,
  • K. Hussain,
  • H. Labiad,
  • P. Majewski,
  • A. L. Marchant,
  • D. Newbold,
  • Z. Pan,
  • Z. Tam,
  • T. C. Thornton,
  • T. Valenzuela,
  • M. G. D. van der Grinten,
  • I. Wilmut,
  • K. Clarke,
  • A. Vick,
  • S. Hedges,
  • B. Stray,
  • M. Langlois,
  • K. Bongs,
  • B. Bostwick,
  • B. Panchumarthi,
  • X. Su,
  • M. Zeuner,
  • Y. Zhi,
  • L. Badurina,
  • A. Beniwal,
  • D. Blas,
  • V. Vaskonen,
  • M. G. D. van der Grinten

摘要

Gravitational waves and ultralight dark matter are among the most compelling frontiers in fundamental physics, motivating proposals for very-long-baseline atom interferometerssuch as AION1, MAGIS2, AICE3 and AEDGE4 that aim to detect at frequencies at which ground-based5 and space-borne6 laser interferometers lose sensitivity. Very-long-baseline atom interferometers look for signals by comparing the quantum phase evolution of widely separated atomic ensembles interrogated by a common laser. However, their performance depends critically on suppressing noise sources, particularly laser phase noise. The experimental validation of such noise rejection remains an important challenge. Here we demonstrate a prototype differential atom interferometer based on the single-photon clock transition of fermionic 87Sr. Thus, we obtain a gradiometer configuration with a species intrinsically suited to kilometre-scale and space-baseline operation. The instrument operates at the standard quantum limit7 with no excess noise beyond atom shot noise. The differential configuration maintains quantum-limited sensitivity in the presence of several radians of artificially injected laser phase noise per shot, which emulates the conditions expected in a very-long-baseline atom interferometer. We also demonstrate the recovery of coherent oscillatory signals across a broad frequency range under fully phase-randomized conditions, a capability that is inaccessible to a single interferometer operating in the same regime. These results provide an experimental validation of the noise-immune measurement principle underlying very-long-baseline atom interferometers and mark an important step towards next-generation quantum sensors for gravitational-wave detection and searches for ultralight dark matter8,9.