2021
DOI: 10.48550/arxiv.2104.11648
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Laser cooling of a Planck mass object close to the quantum ground state

Abstract: Quantum mechanics has so far not been tested for mechanical objects at the scale of the Planck mass c/G 22 µg. We present an experiment where a 1 mm quartz micropillar resonating at 3.6 MHz with an effective mass of 30 µg is cooled to 500 mK with a dilution refrigerator, and further optomechanically sideband-cooled to an effective temperature of 3 mK, corresponding to a mode thermal occupancy of 20 phonons. This nearly 1000-fold increase in the mass of an optomechanical system with respect to previous experime… Show more

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Cited by 2 publications
(3 citation statements)
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“…Device B can operate at a higher effective temperature for both choices of σ, which is attributed to the 1/Ω 2 dependence of N max . These relatively high effective temperatures required by Device B are encouraging given recent experimental progress in cooling Planck mass objects 55 .…”
Section: Comparison To Thermal Decoherence Ratementioning
confidence: 88%
“…Device B can operate at a higher effective temperature for both choices of σ, which is attributed to the 1/Ω 2 dependence of N max . These relatively high effective temperatures required by Device B are encouraging given recent experimental progress in cooling Planck mass objects 55 .…”
Section: Comparison To Thermal Decoherence Ratementioning
confidence: 88%
“…The purity with which quantum states of tangibly massive objects can be prepared remains an open experimental challenge [1][2][3]. Although workers in the fields of atomic physics [4][5][6][7][8][9], and more recently cavity optomechanics [10][11][12][13][14][15][16][17][18], have succeeded in addressing this challenge at sub-nanogram mass scales, objects with a significantly larger mass feature a qualitatively different behavior.…”
Section: Introductionmentioning
confidence: 99%
“…decreases quadratically with frequency, in marked contrast to a velocity damped oscillator (for which the scaling is linear). This can be harnessed by stiffening the oscillator -for example by radiation pressure forces from a cavity field [30][31][32] -so as to establish an oscillator mode at the frequency Ω eff Ω 0 , whose thermal decoherence rate, Γ th [Ω eff ] = Γ th [Ω 0 ](Ω 0 /Ω eff ) 2 , can be significantly lower than that of the intrinsic mode (at frequency Ω 0 ). However, this will be counteracted by additional decoherence from quantum fluctuations of the optical field used to produce the optical spring.…”
Section: Introductionmentioning
confidence: 99%