Nonlinear multi -frequency phonon lasers with active levitated optomechanics Tengfang Kuang15 Ran Huang25 Wei Xiong1 Yunlan Zuo2 Xiang Han1

2025-04-26 0 0 1.15MB 12 页 10玖币
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Nonlinear multi-frequency phonon lasers
with active levitated optomechanics
Tengfang Kuang1,5, Ran Huang2,5, Wei Xiong1, Yunlan Zuo2, Xiang Han1,
Franco Nori3, Cheng-Wei Qiu4,*, Hui Luo1,*, Hui Jing2,*, Guangzong, Xiao1,*
1 College of Advanced Interdisciplinary Studies, NUDT, Changsha Hunan,
410073, China
2 Department of Physics and Synergetic Innovation Center for Quantum
Effects and Applications, Hunan Normal University, Changsha 410081, China
3 Theoretical Quantum Physics Laboratory, RIKEN Cluster for Pioneering
Research, Wako-shi, Saitama 351-0198, Japan
4 Department of Electrical and Computer Engineering, National University of
Singapore, 4 Engineering Drive 3, Singapore, 117576, Singapore
5 These authors contribute equally to this work
*email: chengwei.qiu@nus.edu.sg; luohui.luo@163.com; jinghui73@foxmail.com;
xiaoguangzong@nudt.edu.cn.
Phonon lasers, exploiting coherent amplifications of phonons, have been
a cornerstone for exploring nonlinear phononics, imaging nanomaterial
structures, and operating phononic devices. Very recently, by levitating a
nanosphere in an optical tweezer, a single-mode phonon laser governed
by dispersive optomechanical coupling has been demonstrated, assisted
by alternating mechanical nonlinear cooling and linear heating. Such
levitated optomechanical (LOM) devices, with minimal noises in high
vacuum, can allow flexible control of large-mass objects without any
internal discrete energy levels. However, untill now, it is still elusive to
realize phonon lasing with levitated microscale objects, due to much
stronger optical scattering losses. Here, by employing a Yb3+-doped
active system, we report the first experiment on nonlinear multi-
frequency phonon lasers with a micro-size sphere governed instead by
dissipative LOM coupling. In this work, active gain plays a key role since
not only 3-order enhancement can be achieved for the amplitude of the
fundamental-mode phonon lasing, compared with the passive device, but
also nonlinear mechanical harmonics can emerge spontaneously above
the lasing threshold. Furthermore, for the first time, coherent correlations
of phonons are observed for both the fundamental mode and its
2
harmonics. Our work drives the field of LOM technology into a new regime
where it becomes promising to engineer collective motional properties of
typical micro-size objects, such as atmospheric particulates and living
cells, for a wide range of applications in e.g., acoustic sensing, gravimetry,
and inertial navigation.
Conventional optomechanical systems rely on fixed frames to support mechanical
elements, leading to unavoidable energy dissipation and thermal loading1. LOM system,
i.e., controlling motions of levitated objects with optical forces2, have provided unique
advantages3, such as fundamental minima of damping and noises, the possibility for
levitating complex objects, as well as high degree of control over both conservative
dynamics and coupling to the environment. These advantages are of significance for
both fundamental studies of non-equilibrium physics and applications in metrology4-11.
In recent years, remarkable achievements have been witnessed in LOM systems12-14,
such as the realizations of motional ground-state cooling15,16, room-temperature strong
coupling 17, or ultrahigh-precision torque sensing18, to name only a few. In a very recent
work19, a phonon laser or coherent amplification of phonons, the quanta of vibrations,
was demonstrated for a levitated nanosphere, based on dispersive LOM coupling, in
which the optical resonance frequency is modulated by mechanical motion. This work
offers exciting opportunities of exploring the boundary of classical and quantum worlds
with levitated macroscopic object16,20,21, as well as making various levitated sensors22,23.
Nevertheless, sophisticated feedback controls based on electronic loops19 are needed to
provide both nonlinear cooling and linear heating, and only a single-mode phonon laser
was observed, without any evidence of nonlinear mechanical harmonics.
Besides LOM systems, phonon lasers have also been built by using semiconductor
superlattices24, nanomagnets25, ions26, and nanomechanical27 or electromechanical28
devices. These coherent sound sources, with shorter wavelength of operation than that
of a photon laser of the same frequency, are indispensable in steering phonon chips30,
improving the resolution of motional sensors31, and exploring new effects of phonons32-
34. However, as far as we know, the ability of achieving multi-frequency phonon lasers
with micro-size levitated objects, has not been reported. This ability can be the first step
for many important applications such as multi-frequency motional sensors, exceptional
point optomechanics32,33, and topological sound-wave control35.
In this Letter, we develop a strategy to achieve nonlinear phonon lasers for a levitated
object at microscales by utilizing an active LOM system. We show that in such a system,
3
dissipative LOM coupling36-39 can be significantly enhanced by introducing an optical
gain, thus leading to not only efficient output of fundamental-mode phonon lasing, but
also spontaneous emergence of mechanical harmonics. The active gain plays a key role
in our work since for passive systems, only thermal phonons exist, and no phonon lasing
can appear. To steer this system from a chaotic regime into a phonon lasing regime, an
optical gain is used to increase the photon lifetime and thus enhance the LOM coupling;
as a result, three-order enhancement in the power spectrum of the fundamental-mode
phonons is achieved, with 40-fold narrowing in its linewidth. More importantly, above
the lasing threshold, we observe nonlinear harmonics with double and triple mechanical
frequencies, as clear evidence of gain-enhanced nonlinearity in an active LOM system.
We stress that our work is the first experiment on phonon lasing with a micro-object
which is 3 to 4 orders larger in size or mass than a nano-sphere19. This ability, never
achieved in previous works24-28, is an important step towards applications based on
coherent motional control of a wide range of typical micro-size objects. Also, our work
is the first demonstration of mechanical harmonics accompanying phonon lasing, with
evidence of threshold features and high-order correlations. The key role of active gain
in enhancing nonlinear LOM effects, as far as we know, is also the first example
reported untill now, opening up the door to engineer and utilize more nonlinear
phononic effects in LOM systems, and to achieve exciting goals well beyond the reach
of passive systems, e.g., parity-time-symmetric or gain-enhanced LOM sensing. Finally,
our work is the first example showing dissipative optomechanical coupling in LOM
architectures, and compared to dispersive ones, dissipative LOM systems are expected
to have unique advantages in acoustic metrology40.
Our experimental platform includes an active optical cavity and a dual-beam optical
tweezer for trapping a single microsphere (Fig. 1a). The active cavity works for all three
translational degrees of freedom, well tuneable along both the longitudinal and vertical
directions. Its quality factor is 106 but can be enhanced to 109 by applying a Yb3+-doped
gain fibre. The photon lifetime is thus increased to more than
1s
, enhancing coherent
vibrational amplification of the sphere. Technically, the optical gain is achieved simply
by using a Yb-doped fibre with a pumping laser at 976 nm, and no other limitation
exists. Compared to the cavity-free work19, there is no need to design and carefully
control both nonlinear cooling and linear heating of the mechanical motion with
complicated electronic loops or algorithms19 (see Supplementary Section 1 for details).
摘要:

Nonlinearmulti-frequencyphononlaserswithactivelevitatedoptomechanicsTengfangKuang1,5,RanHuang2,5,WeiXiong1,YunlanZuo2,XiangHan1,FrancoNori3,Cheng-WeiQiu4,*,HuiLuo1,*,HuiJing2,*,Guangzong,Xiao1,*1CollegeofAdvancedInterdisciplinaryStudies,NUDT,ChangshaHunan,410073,China2DepartmentofPhysicsandSynergeti...

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