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声子泵浦增强旋转光力系统中的高分辨率质量传感

陈华俊 叶文

陈华俊, 叶文. 声子泵浦增强旋转光力系统中的高分辨率质量传感[J]. 中国光学(中英文). doi: 10.37188/CO.2026-0037
引用本文: 陈华俊, 叶文. 声子泵浦增强旋转光力系统中的高分辨率质量传感[J]. 中国光学(中英文). doi: 10.37188/CO.2026-0037
CHEN Hua-jun, YE Wen. High-resolution mass sensing in a hybrid spinning optomechanical system enhanced by phonon pump[J]. Chinese Optics. doi: 10.37188/CO.2026-0037
Citation: CHEN Hua-jun, YE Wen. High-resolution mass sensing in a hybrid spinning optomechanical system enhanced by phonon pump[J]. Chinese Optics. doi: 10.37188/CO.2026-0037

声子泵浦增强旋转光力系统中的高分辨率质量传感

cstr: 32171.14.CO.2026-0037
基金项目: 国家自然科学基金(No. 11647001, No. 11804004);安徽高校自然科学研究项目(No. 2024AH050389);中国博士后基金项目(No. 2020M681973)
详细信息
    作者简介:

    陈华俊(1985—),男,安徽阜阳人,博士,讲授,2015年于上海交通大学获得博士学位,主要从事复合微纳系统中的量子光学、非线性光学、及光传播特性方面的研究。E-mail:chenphysics@126.com

  • 中图分类号: O431.2

High-resolution mass sensing in a hybrid spinning optomechanical system enhanced by phonon pump

Funds: Supported byNational Natural Science Foundation of China (No. 11647001, No. 11804004), Natural Science Research Project of Anhui Educational Committee (No. 2024AH050389), China Postdoctoral Science Foundation (No. 2020M681973)
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  • 摘要:

    为了实现对生物分子的高精度质量检测,本文提出一种基于混合旋转光力系统的高分辨率生物分子质量传感方案。该系统中,一个旋转的回音壁光力腔在声子泵浦驱动下,与另一个具有光学增益的回音壁腔发生耦合。首先,利用旋转回音壁光力腔的顺时针或逆时针旋转产生Sagnac效应,从而实现对腔场频率的非互易调控。其次,引入光学增益回音壁腔构建宇称时间对称或破缺系统,增强透射谱的振幅强度。同时,采用声子泵浦对机械呼吸模式进行相干驱动,进一步增强系统的光学响应。通过求解系统的量子朗之万方程并利用输入-输出关系,得到探测场的透射谱表达式。当生物分子(如杆状病毒或冠状病毒)沉积在回音壁光力腔表面时,通过监测透射谱中机械边带峰的共振频移,即可反演待测分子的质量。数值结果表明,Sagnac效应、光学增益腔和声子泵浦共同使透射谱振幅强度显著增强,进而提高质量传感的灵敏度。与基于单腔光力系统的传统光学质量传感方案相比,本方案的质量灵敏度提高约一个数量级,最小可检测质量达到p克量级(~1 pg)。该方案实现了超灵敏、高分辨率的生物分子质量检测,为芯片级超高分辨率传感器件提供了新的物理平台。

     

  • 图 1  混合旋转腔光力系统示意图。可旋转的回音壁腔光力腔a中的声学模式被声子泵浦驱动与另个回音壁增益光学腔c耦合。纳米颗粒沉积在回音壁光力腔a的表面。

    Figure 1.  Schematic diagram of the hybrid spinning whispering-gallery-mode cavity optomechanical system driven by a phonon pump, which includes an optomechanical cavity a spinning along the clockwise and counterclockwise direction, and an gain optical cavity c. Nanoparticles are landed on the optomechanical cavity a.

    图 2  不同参数机制下的透射谱。参数如图中所示。

    Figure 2.  The transmission spectrum under different parameters condition. The parameters are shown in the figures.

    图 3  不同参数机制下的透射谱。参数如图中所示,其它参数: $ {F}_{m}=0 $, $ {\varphi }_{m}=0 $

    Figure 3.  The transmission spectrum under different parameters condition. The parameters are shown in the figures and the other parameters are $ {F}_{m}=0 $, $ {\varphi }_{m}=0 $.

    图 4  不同参数机制下的透射谱。参数如图中所示,其它参数:$ {F}_{m}=0.1\;\text{fN} $$ {\varphi }_{m}={\text{π}} /6 $

    Figure 4.  The transmission spectrum under different parameters condition. The parameters are shown in the figures and the other parameters are $ {F}_{m}=0.1\;\text{fN} $, $ {\varphi }_{m}={\text{π}} /6 $.

    图 5  不同参数机制下的透射谱。参数如图中所示,其它参数:$ {\kappa }_{a}/{\kappa }_{c}=1 $, $ J=0.5({\kappa }_{a}+{\kappa }_{c}) $, $ {F}_{m}=0.1\;\text{fN} $, $ {F}_{m}=0 $, $ {\varphi }_{m}={\text{π}} /6 $

    Figure 5.  The transmission spectrum under different parameters condition. The parameters are shown in the figures and the other parameters are $ {\kappa }_{a}/{\kappa }_{c}=1 $, $ J=0.5({\kappa }_{a}+{\kappa }_{c}) $, $ {F}_{m}=0.1\;\text{fN} $, $ {F}_{m}=0 $, $ {\varphi }_{m}={\text{π}} /6 $.

    图 6  (a)纳米颗粒沉积在回音壁腔光力系统上之前与之后的透射谱。(b)纳米颗粒的质量与频移的线性关系。

    Figure 6.  (a) The transmission spectra before and after depositing nanoparticles on the whispering-gallery-mode resonator, and the color curves give the frequency-shifts. (b) The linear relationship between the frequency-shifts and the nanoparticles mass.

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  • 收稿日期:  2026-03-09
  • 录用日期:  2026-04-21
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