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Approaching the motional ground state of a 10 kg object

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arxiv 2102.12665 v2 pith:R6CKPIQK submitted 2021-02-25 quant-ph

Approaching the motional ground state of a 10 kg object

Chris Whittle , Evan D. Hall , Sheila Dwyer , Nergis Mavalvala , Vivishek Sudhir , R. Abbott , A. Ananyeva , C. Austin
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L. Barsotti J. Betzwieser C. D. Blair A. F. Brooks D. D. Brown A. Buikema C. Cahillane J. C. Driggers A. Effler A. Fernandez-Galiana P. Fritschel V. V. Frolov T. Hardwick M. Kasprzack K. Kawabe N. Kijbunchoo J. S. Kissel G. L. Mansell F. Matichard L. McCuller T. McRae A. Mullavey A. Pele R. M. S. Schofield D. Sigg M. Tse G. Vajente D. C. Vander-Hyde Hang Yu Haocun Yu C. Adams R. X. Adhikari S. Appert K. Arai J. S. Areeda Y. Asali S. M. Aston A. M. Baer M. Ball S. W. Ballmer S. Banagiri D. Barker J. Bartlett B. K. Berger D. Bhattacharjee G. Billingsley S. Biscans R. M. Blair N. Bode P. Booker R. Bork A. Bramley K. C. Cannon X. Chen A. A. Ciobanu F. Clara C. M. Compton S. J. Cooper K. R. Corley S. T. Countryman P. B. Covas D. C. Coyne L. E. H. Datrier D. Davis C. Di Fronzo K. L. Dooley P. Dupej T. Etzel M. Evans T. M. Evans J. Feicht P. Fulda M. Fyffe J. A. Giaime K. D. Giardina P. Godwin E. Goetz S. Gras C. Gray R. Gray A. C. Green E. K. Gustafson R. Gustafson J. Hanks J. Hanson R. K. Hasskew M. C. Heintze A. F. Helmling-Cornell N. A. Holland J. D. Jones S. Kandhasamy S. Karki P. J. King Rahul Kumar M. Landry B. B. Lane B. Lantz M. Laxen Y. K. Lecoeuche J. Leviton J. Liu M. Lormand A. P. Lundgren R. Macas M. MacInnis D. M. Macleod S. M\'arka Z. M\'arka D. V. Martynov K. Mason T. J. Massinger R. McCarthy D. E. McClelland S. McCormick J. McIver G. Mendell K. Merfeld E. L. Merilh F. Meylahn T. Mistry R. Mittleman G. Moreno C. M. Mow-Lowry S. Mozzon T. J. N. Nelson P. Nguyen L. K. Nuttall J. Oberling Richard J. Oram C. Osthelder D. J. Ottaway H. Overmier J. R. Palamos W. Parker E. Payne R. Penhorwood C. J. Perez M. Pirello H. Radkins K. E. Ramirez J. W. Richardson K. Riles N. A. Robertson J. G. Rollins C. L. Romel J. H. Romie M. P. Ross K. Ryan T. Sadecki E. J. Sanchez L. E. Sanchez T. R. Saravanan R. L. Savage D. Schaetzl R. Schnabel E. Schwartz D. Sellers T. Shaffer B. J. J. Slagmolen J. R. Smith S. Soni B. Sorazu A. P. Spencer K. A. Strain L. Sun M. J. Szczepa\'nczyk M. Thomas P. Thomas K. A. Thorne K. Toland C. I. Torrie G. Traylor A. L. Urban G. Valdes P. J. Veitch K. Venkateswara G. Venugopalan A. D. Viets T. Vo C. Vorvick M. Wade R. L. Ward J. Warner B. Weaver R. Weiss B. Willke C. C. Wipf L. Xiao H. Yamamoto L. Zhang M. E. Zucker J. Zweizig
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keywords quantumobjectstatemotionenvironmentgroundmasksmass
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The motion of a mechanical object -- even a human-sized object -- should be governed by the rules of quantum mechanics. Coaxing them into a quantum state is, however, difficult: the thermal environment masks any quantum signature of the object's motion. Indeed, the thermal environment also masks effects of proposed modifications of quantum mechanics at large mass scales. We prepare the center-of-mass motion of a 10 kg mechanical oscillator in a state with an average phonon occupation of 10.8. The reduction in temperature, from room temperature to 77 nK, is commensurate with an 11 orders-of-magnitude suppression of quantum back-action by feedback -- and a 13 orders-of-magnitude increase in the mass of an object prepared close to its motional ground state. This begets the possibility of probing gravity on massive quantum systems.

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