Search

Article

x

留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

Quantum control of fast/slow light in atom-assisted optomechanical cavity

Gu Kai-Hui Yan Dong Zhang Meng-Long Yin Jing-Zhi Fu Chang-Bao

Citation:

Quantum control of fast/slow light in atom-assisted optomechanical cavity

Gu Kai-Hui, Yan Dong, Zhang Meng-Long, Yin Jing-Zhi, Fu Chang-Bao
PDF
HTML
Get Citation
  • In recent years, due to the rapid development of nano science and advanced semiconductor technology, one is able to observe more significant quantum optomechanical effects as optomechanical system turns smaller in size. Optomechanically induced transparency, fast and slow light, optical storage as well as other quantum optical and nonlinear optical effects have become the focus of research. On the other hand, the optomechanical systems coupled to other small subsystems (such as atoms, quantum dots, single electron transistors, etc.) also attract great attention in research. This is because the coupling system has not only provided more degrees of freedom for quantum manipulation, but also opened up more channels for classical and quantum information transfer. In this paper we study the optomechanically induced transparency and fast/slow light phase control in atom-assisted optomechanical cavity. Unlike the traditional systems, in this model the mechanical resonator is directly driven by a weak auxiliary driving field. We therefore find that with the change of amplitude ratio and phase difference between the auxiliary driving field and the probe field, the absorption and dispersion properties of the whole system and the group delay time vary accordingly. In the absence of auxiliary field, we observe the spectral features of the hybrid electromagnetically induced transparency and optomechanically induced transparency (OMIT) in an atom-cavity-oscillator tripartite optomechanical system. When there exists no phase difference between the auxiliary field and the probe field, we find that the membrane resonance absorption is enhanced with the increase of auxiliary field strength at resonance, causing the the optomechanically induced transparency to be suppressed, and therefore we can modify the amplitude of auxiliary field to control the depth of the OMIT window. When keeping amplitude ratio between the auxiliary field and the probe field unchanged, the modification of the phase difference between the auxiliary field and the probe field directly affects the we can not only realize the manipulation of OMIT window depth, but also control the transformation of tunable optical switch among "absorption", "transparent" and "gain" of the system. Therefore, through changing the phase of auxiliary field and probe field, we can not only realize the manipulation of OMIT window depth, but also control the transformation of tunable optical switch among "absorption" , "transparent" and "gain". In the meantime, we find that the system’s group delay time varies periodically with the change of phase difference. It is worth noting that by adjusting the phase difference and the atomic number, we can not only change the magnitude of the group delay, but also realize the conversion between slow light and fast light effect.
      Corresponding author: Yan Dong, ydbest@126.com ; Yin Jing-Zhi, yjz886666@163.com
    • Funds: Project supported by the “Spring Sunshine” Plan Foundation of Ministry of Education of China (Grant No. Z2017030) and the Natural Science Foundation of Jilin Province, China (Grant Nos. 2016286, GH16102).
    [1]

    Agarwal G S, Huang S M 2010 Phys. Rev. A 81 041803(R)Google Scholar

    [2]

    Safavi-Naeini A H, Mayer Alegre T P, Chan J, Eichenfield M, Winger M, Lin Q, Hill J T, Chang D E, Painter O 2011 Nature 472 69Google Scholar

    [3]

    Chang D E, Safavi-Naeini A H, Hafezi M, Painter O 2011 New J. Phys. 13 023003Google Scholar

    [4]

    Gu K H, Yan X B, Zhang Y, Fu C B, Liu Y M, Wang X, Wu J H 2015 Opt. Commun. 338 569Google Scholar

    [5]

    Chen B, Jiang C, Zhu K D 2011 Phys. Rev. A 83 055803Google Scholar

    [6]

    Jiang C, Liu H X, Cui Y S, Li X W, Chen G B, Chen B 2013 Opt. Express 21 12165Google Scholar

    [7]

    Tarhan D, Huang S, Müstecaplıoğlu Ö E 2013 Phys. Rev. A 87 013824Google Scholar

    [8]

    Fiore V, Yang Y, Kuzyk M C, Barbour R, Tian L, Wang H 2011 Phys. Rev. Lett. 107 133601Google Scholar

    [9]

    Tian L, Wang H L 2010 Phys. Rev. A 82 053806Google Scholar

    [10]

    Farman F, Bahrampour A R 2015 Phys. Rev. A 91 033828Google Scholar

    [11]

    McGee S A, Meiser D, Regal C A, Lehnert K W, Holland M J 2013 Phys. Rev. A 87 053818Google Scholar

    [12]

    Qu K, Agarwal G S 2013 Phys. Rev. A 87 031802(R)Google Scholar

    [13]

    Yan X B, Cui C L, Gu K H, Tian X D, Fu C B, Wu J H 2014 Opt. Express 22 4886Google Scholar

    [14]

    Barzanjeh S, Naderi M H, Soltanolkotabi M 2011 Phys. Rev. A 84 023803Google Scholar

    [15]

    Chan J, Alegr T P M, Safavi-Naeini A H, Hill J F, Krause A, Gröblacher S, Aspelmeyer M, Painter O 2011 Nature 478 89Google Scholar

    [16]

    Rabl P, Genes C, Hammerer K, Aspelmeyer M 2009 Phys. Rev. A 80 063819Google Scholar

    [17]

    Mari A, Eisert J 2009 Phys. Rev. Lett. 103 213603Google Scholar

    [18]

    Gu W J, Li G X 2013 Phys. Rev. A 88 013835Google Scholar

    [19]

    Mancini S, Giovannetti V, Vitali D, Tombesi P 2002 Phys. Rev. Lett. 88 120401Google Scholar

    [20]

    Hartmann M J, Plenio M B 2008 Phys. Rev. Lett. 101 200503Google Scholar

    [21]

    Mazzola L, Paternostro M 2011 Sci. Rep. 1 199Google Scholar

    [22]

    Yan X B 2017 Phys. Rev. A 96 053831Google Scholar

    [23]

    张秀龙, 鲍倩倩, 杨明珠, 田雪松 2018 物理学报 67 104203Google Scholar

    Zhang X L, Bao Q Q, Yang M Z, Tian X S 2018 Acta Phys. Sin. 67 104203Google Scholar

    [24]

    Stannigel K, Rabl P, Sorensen A S, Zoller P, Lukin M D 2010 Phys. Rev. Lett. 105 220501Google Scholar

    [25]

    Li J J, Zhu K D 2011 J. Appl. Phys. 110 114308Google Scholar

    [26]

    Agarwal G S, Huang S M 2014 New J. Phys. 16 033023Google Scholar

    [27]

    刘欢, 曹士英, 孟飞, 林百科, 方占军 2015 物理学报 64 094204Google Scholar

    Liu H, Cao S Y, Meng F, Lin B K, Fang Z J 2015 Acta Phys. Sin. 64 094204Google Scholar

    [28]

    Chang Y, Shi T, Liu Y X, Sun C P, Nori F 2011 Phys. Rev. A 83 063826Google Scholar

    [29]

    Fu C B, Yan X B, Gu K H, Cui C L, Wu J H, Fu T D 2013 Phys. Rev. A 87 053841Google Scholar

    [30]

    韩明, 谷开慧, 刘一谋, 张岩, 王晓畅, 田雪冬, 付长宝, 崔淬砺 2014 物理学报 63 094206Google Scholar

    Han M, Gu K H, Liu Y M, Zhang Y, Wang X C, Tian X D, Fu C B, Cui C L 2014 Acta Phys. Sin. 63 094206Google Scholar

    [31]

    Yan D, Wang Z H, Ren C N, Gao H, Li Y, Wu J H 2015 Phys. Rev. A 91 023813Google Scholar

    [32]

    He Q Y, Ficek Z 2014 Phys. Rev. A 89 022332Google Scholar

    [33]

    Genes C, Vitali D, Tombesi P 2008 Phys. Rev. A 77 050307Google Scholar

    [34]

    Genes C, Ritsch H, Drewsen M 2009 Phys. Rev. A 80 061803Google Scholar

    [35]

    Yi Z, Li G X, Wu S P, Yang Y P 2014 Opt. Express 22 20060Google Scholar

    [36]

    Walls D F, Milburn G J 1944 Quantum Optics (Berlin: Springer) p296

  • 图 1  由单模FP腔以及束缚在其中的N个全同二能级87Rb冷原子系综和中间由弱辅助驱动场${\varepsilon _{\rm{f}}}$驱动的振动频率为${\omega _{\rm{m}}}$的薄膜振子构成的光力学系统, 该系统的探测场和驱动场分别为${\varepsilon _{\rm{p}}}$${\varepsilon _{\rm{d}}}$

    Figure 1.  Schematic diagram of an optomechanical cavity containing N identical two-level cold 87Rb atoms with two fixed-end mirrors of equal reflectivity, which is driven by a strong coupling field ${\varepsilon _{\rm{d}}}$, a weak auxiliary drive field ${\varepsilon _{\rm{f}}}$and probed by a weak field ${\varepsilon _{\rm{p}}}$.

    图 2  $\operatorname{Re} ({\varepsilon _{\rm{T}}})$(黑色实线)和${\rm{Im}}({\varepsilon _{\rm{T}}})$(红色虚线)随频率失谐$\delta /{\omega _{\rm{m}}}$的变化曲线 (a) $Y = 0$; $\varPhi = 0$; (b) $Y = 0.05$; $\varPhi = 0$; (c) $Y = 0.2$; $\varPhi = 0$; 其他参数值见文中第4部分

    Figure 2.  The real (black line) and the imaginary (red dotted line) parts of ${\varepsilon _{\rm{T}}}$ as a function of $\delta /{\omega _{\rm{m}}}$with (a) $Y = 0$; $\varPhi = 0$; (b) $Y = 0.05$; $\varPhi = 0$; (c) $Y = 0.2$; $\varPhi = 0$. Relevant parameters are the same as those in Sec. 4.

    图 3  $Y = 0.2$$\operatorname{Re} ({\varepsilon _{\rm{T}}})$(黑色实线)和${\rm{Im}}({\varepsilon _{\rm{T}}})$(红色虚线)随频率失谐$\delta /{\omega _{\rm{m}}}$的变化曲线 (a) $\varPhi = 0$; (b) $\varPhi = {\text{π}}/4$; (c) $\varPhi = {\text{π}}/2$; (d) $\varPhi = 3{\text{π}}/4$; (e) $\varPhi = {\text{π}}$; (f) $\varPhi = 5{\text{π}} /4$; (g) $\varPhi = 6{\text{π}}/4$; (h) $\varPhi = 7{\text{π}}/4$; 其他参数值见文中第4部分

    Figure 3.  The real (black line) and the imaginary (red dotted line) parts of ${\varepsilon _{\rm{T}}}$ as a function of $\delta /{\omega _{\rm{m}}}$with $Y = 0.2$: (a) $\varPhi = 0$; (b) $\varPhi = {\text{π}}/4$; (c) $\varPhi = {\text{π}}/2$; (d) $\varPhi = 3{\text{π}}/4$; (e) $\varPhi = {\text{π}} $; (f) $\varPhi = 5{\text{π}}/4$; (g) $\varPhi = 6{\text{π}}/4$; (h) $\varPhi = 7{\text{π}}/4$. Other parameters are the same as those in Sec. 4.

    图 4  $Y = 0.2$$\operatorname{Re} ({\varepsilon _{\rm{T}}})$(黑色实线)和${\rm{Im}}({\varepsilon _{\rm{T}}})$(红色虚线)随频率失谐$\delta /{\omega _{\rm{m}}}$的变化曲线 (a) $\varPhi = {\text{π}}/4$, $g\sqrt N = 3 \times 2{\text{π}}$ MHz; (b) $\varPhi = {\text{π}}/4$, $g\sqrt N = 6 \times 2{\text{π}}$ MHz; (c) $\varPhi = {\text{π}}/4$, $g\sqrt N = 9 \times 2{\text{π}}$ MHz; (d) $\varPhi = 6{\text{π}}/4$, $g\sqrt N = 3 \times 2{\text{π}}$ MHz; (e) $\varPhi = 6{\text{π}}/4$, $g\sqrt N = 6 \times 2{\text{π}}$ MHz; (f) $\varPhi = 6{\text{π}}/4$, $g\sqrt N = 9 \times 2{\text{π}}$ MHz; 其他参数值见文中第4部分

    Figure 4.  The real (black line) and the imaginary (red dotted line) parts of ${\varepsilon _{\rm{T}}}$ as a function of $\delta /{\omega _{\rm m}}$with $Y = 0.2$: (a) $\varPhi = {\text{π}}/4$, $g\sqrt N = 3 \times 2{\text{π}}$ MHz; (b) $\varPhi = {\text{π}}/4$, $g\sqrt N = 6 \times 2{\text{π}}$ MHz; (c) $\varPhi = {\text{π}}/4$, $g\sqrt N = 9 \times 2{\text{π}}$ MHz; (d) $\varPhi = 6{\text{π}}/4$, $g\sqrt N = 3 \times 2{\text{π}}$ MHz; (e) $\varPhi = 6{\text{π}}/4$, $g\sqrt N = 6 \times {{2{\text{π}} }}$ MHz; (f) $\varPhi = 6{\text{π}}/4$, $g\sqrt N = 9 \times {{2{\text{π}} }}$ MHz. Other parameters are the same as those in Sec. 4.

    图 5  ${\tau _{\rm{T}}}$(黑色实线)和${\tau _{\rm{R}}}$(红色虚线)随频率失谐$\delta /{\omega _{\rm{m}}}$的变化曲线: (a) $\varPhi = 0$; (b) $\varPhi = {\text{π}}/4$; (c) $\varPhi = {\text{π}}/2$; (d) $\varPhi = 3{\text{π}}/4$; (e) $\varPhi = {\text{π}}$; (f) $\varPhi = 5{\text{π}} /4$; (g) $\varPhi = 6{\text{π}}/4$; (h) $\varPhi = 7{{{\text{π}} }}/4$; 其他参数取值同图3

    Figure 5.  The ${\tau _{\rm{T}}}$ (black line) and the ${\tau _{\rm{R}}}$ (red dotted line) as a function of $\delta /{\omega _{\rm{m}}}$with (a) $\varPhi = 0$; (b) $\varPhi = {\text{π}}/4$; (c) $\varPhi = {\text{π}}/2$; (d) $\varPhi = 3{\text{π}}/4$; (e) $\varPhi = {\text{π}}$; (f) $\varPhi = 5{\text{π}}/4$; (g) $\varPhi = {{6{\text{π}} /}}4$; (h) $\varPhi = 7{\text{π}}/4$. Other parameters are the same as those in Fig.3.

    图 6  $\delta = {\omega _{\rm{m}}}$${\tau _{\rm{T}}}$(黑色实线)和${\tau _{\rm{R}}}$(红色虚线)随相位差$\varPhi /{\text{π}}$和振幅比$Y$的变化曲线: (a) $Y = 0.2$, $g\sqrt N = 3 \times 2{\text{π}}$ MHz; (b) $Y = 0.2$, $g\sqrt N = 6 \times 2{\text{π}}$ MHz; (c) $Y = 0.2$, $g\sqrt N = 9 \times 2{\text{π}}$ MHz; 其他参数取值见文中第4部分

    Figure 6.  The ${\tau _{\rm{T}}}$ (black line) and the ${\tau _{\rm{R}}}$ (red dotted line) as a function of $\varPhi /{\text{π}}$ and Y with $\delta = {\omega _{\rm{m}}}$: (a) $Y = 0.2$, $g\sqrt N = 3 \times 2{\text{π}}$ MHz; (b) $Y = 0.2$, $g\sqrt N = 6 \times 2{\text{π}}$ MHz; (c) $Y = 0.2$, $g\sqrt N = 9 \times 2{\text{π}}$ MHz. Other parameters are the same as those in Sec. IV.

  • [1]

    Agarwal G S, Huang S M 2010 Phys. Rev. A 81 041803(R)Google Scholar

    [2]

    Safavi-Naeini A H, Mayer Alegre T P, Chan J, Eichenfield M, Winger M, Lin Q, Hill J T, Chang D E, Painter O 2011 Nature 472 69Google Scholar

    [3]

    Chang D E, Safavi-Naeini A H, Hafezi M, Painter O 2011 New J. Phys. 13 023003Google Scholar

    [4]

    Gu K H, Yan X B, Zhang Y, Fu C B, Liu Y M, Wang X, Wu J H 2015 Opt. Commun. 338 569Google Scholar

    [5]

    Chen B, Jiang C, Zhu K D 2011 Phys. Rev. A 83 055803Google Scholar

    [6]

    Jiang C, Liu H X, Cui Y S, Li X W, Chen G B, Chen B 2013 Opt. Express 21 12165Google Scholar

    [7]

    Tarhan D, Huang S, Müstecaplıoğlu Ö E 2013 Phys. Rev. A 87 013824Google Scholar

    [8]

    Fiore V, Yang Y, Kuzyk M C, Barbour R, Tian L, Wang H 2011 Phys. Rev. Lett. 107 133601Google Scholar

    [9]

    Tian L, Wang H L 2010 Phys. Rev. A 82 053806Google Scholar

    [10]

    Farman F, Bahrampour A R 2015 Phys. Rev. A 91 033828Google Scholar

    [11]

    McGee S A, Meiser D, Regal C A, Lehnert K W, Holland M J 2013 Phys. Rev. A 87 053818Google Scholar

    [12]

    Qu K, Agarwal G S 2013 Phys. Rev. A 87 031802(R)Google Scholar

    [13]

    Yan X B, Cui C L, Gu K H, Tian X D, Fu C B, Wu J H 2014 Opt. Express 22 4886Google Scholar

    [14]

    Barzanjeh S, Naderi M H, Soltanolkotabi M 2011 Phys. Rev. A 84 023803Google Scholar

    [15]

    Chan J, Alegr T P M, Safavi-Naeini A H, Hill J F, Krause A, Gröblacher S, Aspelmeyer M, Painter O 2011 Nature 478 89Google Scholar

    [16]

    Rabl P, Genes C, Hammerer K, Aspelmeyer M 2009 Phys. Rev. A 80 063819Google Scholar

    [17]

    Mari A, Eisert J 2009 Phys. Rev. Lett. 103 213603Google Scholar

    [18]

    Gu W J, Li G X 2013 Phys. Rev. A 88 013835Google Scholar

    [19]

    Mancini S, Giovannetti V, Vitali D, Tombesi P 2002 Phys. Rev. Lett. 88 120401Google Scholar

    [20]

    Hartmann M J, Plenio M B 2008 Phys. Rev. Lett. 101 200503Google Scholar

    [21]

    Mazzola L, Paternostro M 2011 Sci. Rep. 1 199Google Scholar

    [22]

    Yan X B 2017 Phys. Rev. A 96 053831Google Scholar

    [23]

    张秀龙, 鲍倩倩, 杨明珠, 田雪松 2018 物理学报 67 104203Google Scholar

    Zhang X L, Bao Q Q, Yang M Z, Tian X S 2018 Acta Phys. Sin. 67 104203Google Scholar

    [24]

    Stannigel K, Rabl P, Sorensen A S, Zoller P, Lukin M D 2010 Phys. Rev. Lett. 105 220501Google Scholar

    [25]

    Li J J, Zhu K D 2011 J. Appl. Phys. 110 114308Google Scholar

    [26]

    Agarwal G S, Huang S M 2014 New J. Phys. 16 033023Google Scholar

    [27]

    刘欢, 曹士英, 孟飞, 林百科, 方占军 2015 物理学报 64 094204Google Scholar

    Liu H, Cao S Y, Meng F, Lin B K, Fang Z J 2015 Acta Phys. Sin. 64 094204Google Scholar

    [28]

    Chang Y, Shi T, Liu Y X, Sun C P, Nori F 2011 Phys. Rev. A 83 063826Google Scholar

    [29]

    Fu C B, Yan X B, Gu K H, Cui C L, Wu J H, Fu T D 2013 Phys. Rev. A 87 053841Google Scholar

    [30]

    韩明, 谷开慧, 刘一谋, 张岩, 王晓畅, 田雪冬, 付长宝, 崔淬砺 2014 物理学报 63 094206Google Scholar

    Han M, Gu K H, Liu Y M, Zhang Y, Wang X C, Tian X D, Fu C B, Cui C L 2014 Acta Phys. Sin. 63 094206Google Scholar

    [31]

    Yan D, Wang Z H, Ren C N, Gao H, Li Y, Wu J H 2015 Phys. Rev. A 91 023813Google Scholar

    [32]

    He Q Y, Ficek Z 2014 Phys. Rev. A 89 022332Google Scholar

    [33]

    Genes C, Vitali D, Tombesi P 2008 Phys. Rev. A 77 050307Google Scholar

    [34]

    Genes C, Ritsch H, Drewsen M 2009 Phys. Rev. A 80 061803Google Scholar

    [35]

    Yi Z, Li G X, Wu S P, Yang Y P 2014 Opt. Express 22 20060Google Scholar

    [36]

    Walls D F, Milburn G J 1944 Quantum Optics (Berlin: Springer) p296

  • [1] Wang Xin, Ren Fei-Fan, Han Song, Han Hai-Yan, Yan Dong. Perfect optomechanically induced transparency and slow light in an Rydberg atom-assisted optomechanical system. Acta Physica Sinica, 2023, 72(9): 094203. doi: 10.7498/aps.72.20222264
    [2] Xie Bao-Hao, Chen Hua-Jun, Sun Yi. Slow light effect caused by optomechanically induced transparency in multimode optomechanical system. Acta Physica Sinica, 2023, 72(15): 154203. doi: 10.7498/aps.72.20230663
    [3] Sun Zhan-Shuo, Wang Xin, Wang Jun-Lin, Fan Bo, Zhang Yü, Feng Yao. Sensing and slow light properties of dual-band terahertz metamaterials based on electromagnetically induced transparency-like. Acta Physica Sinica, 2022, 71(13): 138101. doi: 10.7498/aps.71.20212163
    [4] Xu Qi, Sun Xiao-Wei, Song Ting, Wen Xiao-Dong, Liu Xi-Xuan, Wang Yi-Wen, Liu Zi-Jiang. Novel one-dimensional optomechanical crystal nanobeam with high optomechanical coupling rate under different defect states. Acta Physica Sinica, 2021, 70(22): 224210. doi: 10.7498/aps.70.20210925
    [5] Zhao Jia-Dong, Zhang Hao, Yang Wen-Guang, Zhao Jing-Hua, Jing Ming-Yong, Zhang Lin-Jie. Deceleration of optical pulses based on electromagnetically induced transparency of Rydberg atoms. Acta Physica Sinica, 2021, 70(10): 103201. doi: 10.7498/aps.70.20210102
    [6] Li Sen, Li Hao-Zhen, Xu Jing-Ping, Zhu Cheng-Jie, Yang Ya-Ping. Squeezed property of optical transistor based on cavity optomechanical system. Acta Physica Sinica, 2019, 68(17): 174202. doi: 10.7498/aps.68.20190078
    [7] Zhang Xiu-Long, Bao Qian-Qian, Yang Ming-Zhu, Tian Xue-Song. Entanglement characteristics of output optical fields in double-cavity optomechanics. Acta Physica Sinica, 2018, 67(10): 104203. doi: 10.7498/aps.67.20172467
    [8] Deng Rui-Jie, Yan Zhi-Hui, Jia Xiao-Jun. Analysis of electromagnetically induced transparency based on quantum memory of squeezed state of light. Acta Physica Sinica, 2017, 66(7): 074201. doi: 10.7498/aps.66.074201
    [9] Li Gao-Fang, Ma Guo-Hong, Ma Hong, Chu Feng-Hong, Cui Hao-Yang, Liu Wei-Jing, Song Xiao-Jun, Jiang You-Hua, Huang Zhi-Ming, Chu Jun-Hao. Photocarrier dynamics in zinc selenide studied with optical-pump terahertz-probe spectroscopy. Acta Physica Sinica, 2016, 65(24): 247201. doi: 10.7498/aps.65.247201
    [10] Chen Xue, Liu Xiao-Wei, Zhang Ke-Ye, Yuan Chun-Hua, Zhang Wei-Ping. Quantum measurement with cavity optomechanical systems. Acta Physica Sinica, 2015, 64(16): 164211. doi: 10.7498/aps.64.164211
    [11] Lin Jian-Xiao, Wu Jiu-Hui, Liu Ai-Qun, Chen Zhe, Lei Hao. A nano-silicon-photonic switch driven by an optical gradient force. Acta Physica Sinica, 2015, 64(15): 154209. doi: 10.7498/aps.64.154209
    [12] Wang Fu, Wang Zhi, Wu Chong-Qing, Liu Guo-Dong, Mao Ya-Ya, Sun Zhen-Chao, Li Qiang. Superluminal and slow light of high-order harmonic for rectangle signal in erbium-doped fiber. Acta Physica Sinica, 2015, 64(24): 244205. doi: 10.7498/aps.64.244205
    [13] Liu Yan, Zhang Wen-Ming, Zhong Zuo-Yang, Peng Zhi-Ke, Meng Guang. Nonlinear dynamic analysis of nano-resonator driven by optical gradient force. Acta Physica Sinica, 2014, 63(2): 026201. doi: 10.7498/aps.63.026201
    [14] Zhao Jian-Peng, Luo Bin, Pan Wei, Yan Lian-Shan, Zhu Hong-Na, Zou Xi-Hua, Ye Jia. Characteristics of the slow and fast light in the band-edge of gain spectrum of the fiber-optic parametric amplification. Acta Physica Sinica, 2014, 63(4): 044203. doi: 10.7498/aps.63.044203
    [15] Yan Xiao-Bo, Yang Liu, Tian Xue-Dong, Liu Yi-Mou, Zhang Yan. Optomechanically induced transparency and normal mode splitting in an optical parametric amplifier cavity. Acta Physica Sinica, 2014, 63(20): 204201. doi: 10.7498/aps.63.204201
    [16] Fu Jing, Liu Wan-Fang, Zhao Yu-Jie. Wigner-Yanse skew information of the system with the electromagnetically induced transparency. Acta Physica Sinica, 2013, 62(17): 170302. doi: 10.7498/aps.62.170302
    [17] Ren Zhi-Jun, Wu Qiong, Zhou Wei-Dong, Wu Gen-Zhu, Shi Yi-Le. Spatially induced Airy-Bessel light bullets. Acta Physica Sinica, 2012, 61(17): 174207. doi: 10.7498/aps.61.174207
    [18] Zhu Qi, Pan Bai-Liang, Chen Li, Wang Ya-Juan, Zhang Xun-Yi. A kinetic model for optically pumped cesium vapor laser. Acta Physica Sinica, 2010, 59(3): 1797-1801. doi: 10.7498/aps.59.1797
    [19] Zhang Peng-Fei, Li Gang, Zhang Yu-Chi, Yang Rong-Can, Guo Yan-Qiang, Wang Jun-Min, Zhang Tian-Cai. Investigation of dynamics of magneto-optical trap loading by light-induced atom desorption. Acta Physica Sinica, 2010, 59(9): 6423-6429. doi: 10.7498/aps.59.6423
    [20] Zheng Di, Pan Wei, Yan Lian-Shan, Luo Bin, Zou Xi-Hua, Jiang Ning, Ma Ya-Nan. Zero-broadening slow and fast light using an optimized Brillouin comb gain for arbitrary periodic signals. Acta Physica Sinica, 2010, 59(2): 1040-1046. doi: 10.7498/aps.59.1040
Metrics
  • Abstract views:  8386
  • PDF Downloads:  93
  • Cited By: 0
Publishing process
  • Received Date:  25 July 2018
  • Accepted Date:  23 October 2018
  • Available Online:  01 March 2019
  • Published Online:  05 March 2019

/

返回文章
返回