Modes trimming and clustering in a weakly perturbed high- Q whispering gallery microresonator Botao Fu17 Renhong Gao16 Jintian Lin16 Ni Yao2 Haisu Zhang3 Min Wang3 Lingling

2025-05-06 0 0 2.46MB 19 页 10玖币
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Modes trimming and clustering in a weakly perturbed high-Q
whispering gallery microresonator
Botao Fu,1,7 Renhong Gao,1,6 Jintian Lin,1,6 Ni Yao, 2,† Haisu Zhang,3 Min Wang,3 Lingling
Qiao,1,6 Wei Fang,5 and Ya Cheng1,3,4,6,8,9,10,11,*
1State Key Laboratory of High Field Laser Physics and CAS Center for Excellence in Ultra-Intense Laser
Science, Shanghai Institute of Optics and Fine Mechanics (SIOM), Chinese Academy of Sciences (CAS),
Shanghai 201800, China
2Research Center for Humanoid Sensing, Zhejiang Lab, Hangzhou 311100, China
3The Extreme Optoelectromechanics Laboratory (XXL), School of Physics and Electronic Science, East
China Normal University, Shanghai 200241, China
4State Key Laboratory of Precision Spectroscopy, East China Normal University, Shanghai 200062,
China
5Interdisciplinary Center for Quantum Information, State Key Laboratory of Modern Optical
Instrumentation, College of Optical Science and Engineering, Zhejiang University, Hangzhou 310027,
China
6Center of Materials Science and Optoelectronics Engineering, University of Chinese Academy of
Sciences, Beijing 100049, China
7School of Physical Science and Technology, Shanghai Tech University, Shanghai 200031, China
8Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
9Collaborative Innovation Center of Light Manipulations and Applications, Shandong Normal University,
Jinan 250358, China
10Shanghai Research Center for Quantum Sciences, Shanghai 201315, China
11Hefei National Laboratory, Hefei 230088, China
Electronic address: yaoni14@zju.edu.cn
*Electronic address: ya.cheng@siom.ac.cn
Abstract
In general, a high-Q microresonator can accommodate abundant whispering gallery
modes (WGMs) with the mode number increasing with the dimensional sizes of the
microresonator. Removing the unnecessary modes while reorganizing the remaining
modes is of vital importance, which, however, has been proved challenging and usually
results in a tradeoff with the Q of the microresonator. Here, we reveal an effective and
controllable mode trimming and clustering mechanism underlying the generation of
polygon and star modes in weakly perturbed tapered fiber-coupled lithium niobate
whispering gallery microresonators. Experimentally, various polygon and star modes
are observed in sequence within a single microresonator by tuning the excitation
wavelength or varying the coupling position between a tapered fiber and the circular
microresonator, which can be well reproduced with our theoretical model. The finding
offers a ubiquitous solution for a broad range of applications requiring elaborate
selection and organization of the high-Q WGMs.
Optical dielectric microresonators, which enhance light-matter interaction by storing
optical energy in a small mode volume with ultra-low loss [1-4], are now highly
desirable not only to fundamental physics such as chaos-assisted tunnelling [5, 6] and
cavity quantum electrodynamics [7, 8] but also to practical applications from integrated
laser sources [9-12], to sensors [13-15] and modulators [16, 17]. Among the diverse
candidates, circular-shaped whispering gallery mode (WGM) microresonators have
been intensively studied due to their nearly perfect light confinement over a long period.
The isotropic characteristic in the microdisk plane is unfavourable for either intensive
interaction of the light field with the coupled device or efficient emission collection,
which is the reason behind the significant efforts spent on the deformed WGM
microdisks [18-21]. Unfortunately, the microresonator deformation usually leads to the
reduction of the mode Q factor and in turn the light-matter interaction strength. Recently,
the generation of high-Q polygon modes in tapered fiber-coupled circular microdisk
resonators with weak perturbation has been reported [22, 23], whereas the essential
physics behind the phenomena is yet to be explored and clarified.
Here, we reveal an effective and controllable mechanism to precisely conduct the mode
trimming and clustering in a weakly perturbed tapered fiber-coupled lithium niobate
WGM microresonator. Meanwhile, complete polygon and star modes sequences are
observed within the single microresonator, which are well reproduced with our
theoretical model.
To facilitate observation of mode patterns, an Er3+-doped z-cut lithium niobate circular
microdisk resonator allowing visualization of the modes is utilized taking advantage of
two-photon fluorescence excitation of the Er3+ ions. The circular microdisk resonator
was fabricated using photolithography-assisted chemo-mechanical etching, and further
details on the fabrication procedures can be found in Ref. [24-26]. The inset of Fig. 1(a)
shows the scanning-electron-microscope (SEM) image of the fabricated microdisk
resonator with a thickness of 700 nm and a diameter of 83.44 μm.
The experimental setup for investigating the polygon and star modes formation is
illustrated in Fig. 1(a), in which a narrow-linewidth tunable diode laser with a
wavelength range from 960 nm to 980 nm (Model: TLB-6719-P-D, New Focus, Inc.)
is used as the pump light source. The pump light is coupled to the microdisk via the
tapered fiber with a diameter of 2 μm [27], and the polarization state can be controlled
to be transverse-magnetically polarized by an in-line polarization controller (PC). The
input pump power can be adjusted and monitored by a variable optical attenuator (VOA)
and a power meter combined with a 10/90 beam splitter. The relative position between
the tapered fiber and microdisk resonator can be monitored and adjusted by an optical
microscope system and a high-resolution positioning stage of 5 nm resolution. A top-
view optical microscope with a 20× objective lens with a numerical aperture of 0.42,
a visible charge-coupled device (CCD), and a short-pass filter (Model: FES800,
Thorlabs, Inc.) are used to capture the mode patterns distributed on the plane of the
microdisk. Remarkably, the captured up-conversion fluorescence patterns directly
reflect the spatial distribution characterisitics of the pump mode [23].
摘要:

Modestrimmingandclusteringinaweaklyperturbedhigh-QwhisperinggallerymicroresonatorBotaoFu,1,7RenhongGao,1,6JintianLin,1,6NiYao,2,†HaisuZhang,3MinWang,3LinglingQiao,1,6WeiFang,5andYaCheng1,3,4,6,8,9,10,11,*1StateKeyLaboratoryofHighFieldLaserPhysicsandCASCenterforExcellenceinUltra-IntenseLaserScience,S...

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