All-optical sub-Kelvin sympathetic cooling of a levitated microsphere in vacuum

2025-04-22 0 0 1.06MB 3 页 10玖币
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All-optical sub-Kelvin sympathetic cooling of a levitated microsphere in vacuum
Yoshihiko Arita,1, Graham D. Bruce,1Ewan M. Wright,2, 1 Stephen
H. Simpson,3Pavel Zem´anek,3and Kishan Dholakia1, 2, 4, 5,
1SUPA, School of Physics & Astronomy, University of St Andrews,
North Haugh, St Andrews, KY16 9SS, United Kingdom
2Wyant College of Optical Sciences, The University of Arizona,
1630 East University Boulevard, Tucson, Arizona 85721, USA
3Institute of Scientific Instruments of the Czech Academy of Science,
v.v.i., Kr´alovopolsk´a 147, 612 64 Brno, Czech Republic
4Department of Physics, College of Science, Yonsei University, Seoul 03722, South Korea
5School of Biological Sciences, The University of Adelaide, Adelaide, South Australia, Australia
We demonstrate all-optical sympathetic cooling of a laser-trapped microsphere to sub-Kelvin tem-
peratures, mediate by optical binding to a feedback-cooled adjacent particle. Our study opens
prospects for multi-particle quantum entanglement and sensing in levitated optomechanics.
This article was published by Optica Publishing Group under the terms of the Creative Commons
Attribution 4.0 License. Further distribution of this work must maintain attribution to the author(s)
and the published article’s title, journal citation, and DOI https://doi.org/10.1364/OPTICA.466337
Single, levitated mesoscopic objects are providing an ex-
cellent platform for sensing weak forces [1] and explor-
ing the classical-quantum boundary with massive objects
[2] due to their weak coupling to the environment and
the ability to cool their centre of mass (CoM) motion.
Intriguing possibilities have been proposed for interact-
ing systems comprising multiple levitated particles, in-
cluding quantum gravity measurements [3], dark matter
detection [4] and quantum friction measurement [5], al-
though there are currently few experimental demonstra-
tions trapping multiple particles [6–9].
The path to systems of interacting, massive quan-
tum objects requires simultaneous cooling of multiple
trapped particles. We take inspiration from experiments
with cold neutral atoms [10] and atomic ions [11], where
an actively cooled object can be used to sympathet-
ically cool another. Recently, sympathetic cooling of
two charged particles held in a Paul trap was shown
[8]. While Coulomb forces provide strong interactions
between particles, they also couple strongly to the envi-
ronment. Hence, an all-optical alternative is desirable,
especially for compatibility with state-of-the-art ground
state cooling methods [2].
Towards this goal, we have developed an optical tweez-
ers system (Fig. 1(a)) that can trap more than one parti-
cle, mediate inter-particle separation and perform para-
metric feedback (PFB) cooling [12] on one particle. Two
rotating microparticles confined in separate but close-
proximity traps exhibit optical binding, a light scattering
mediated interaction whose strength is dependent on the
inter-particle separation [6]. We show, for the first time,
the use of this optical binding to perform sympathetic
cooling: by applying PFB cooling to one particle, the
ya10@st-andrews.ac.uk
kd1@st-andrews.ac.uk
FIG. 1. Sympathetic cooling scheme and numerical simula-
tions. (a) Optical binding couples the centre-of-mass motion
of two microspheres (depicted as a spring between the parti-
cles). When feedback cooling is applied to the left particle,
the right particle is sympathetically cooled. (b-c) Time evolu-
tion of simulated centre-of-mass temperatures T1(solid lines)
and T2(dashed lines) for the feedback-cooled and sympathet-
ically cooled particle respectively, versus gas pressure for (b)
ξ= 0.01 and (c) ξ= 0.1. (d) Simulated steady-state
temperatures T1(blue) and T2(red) as a function of gas pres-
sure for different binding strengths.
adjacent particle is sympathetically cooled to sub-Kelvin
temperatures.
We modelled the motion of two particles, optically
bound along the x-axis and labelled j= 1,2, using a
Langevin equation for each particle [6]. The determin-
istic forces acting on the particles along the x-axis are
Fj=κxj+ξx3j. Here, κis the trap stiffness for each
individual particle, and ξdescribes the inter-particle cou-
pling due to optical binding. The ratio ξ(typically
arXiv:2210.01458v1 [physics.optics] 4 Oct 2022
摘要:

All-opticalsub-KelvinsympatheticcoolingofalevitatedmicrosphereinvacuumYoshihikoArita,1,GrahamD.Bruce,1EwanM.Wright,2,1StephenH.Simpson,3PavelZemanek,3andKishanDholakia1,2,4,5,y1SUPA,SchoolofPhysics&Astronomy,UniversityofStAndrews,NorthHaugh,StAndrews,KY169SS,UnitedKingdom2WyantCollegeofOpticalScie...

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