Abstract
Optomechanical systems have long been considered in the field of precision measurement. In this work, measurement of weak magnetic field in a hybrid optomechanical system is discussed. In contrast to conventional measurements based on detecting the change of magnetic flux, our scheme presents an alternative way to measure the magnetic field with a precision of 0.1 nT. We show that the effective cavity resonance frequency will be revised due to the electromagnetic interactions. Therefore, a resonance valley in the transmission spectrum of the probe field will shift in the presence of the magnetic field, and the width of an asymmetric transparency in the optomechanically induced transparency (OMIT) shows a strong dependence on the magnetic field strength. Our results may have potential application for achieving high precision measurement of the magnetic field.
Introduction
Cavity optomechanics^{1}, combining mechanical modes with optical modes via radiation pressure, has become a rapidly developing field recently and plays an important role in many fields of physics^{2,3}, including cooling of mechanical oscillators to their motional quantum groundstate^{4,5}, strong coupling physics^{6}, gravitationalwave detectors^{7}, manipulation of light propagation^{8,9} and radiationmechanics entanglement^{10,11}. It has been shown that many effects observed in atomic systems, like electromagnetically induced transparency^{12,13}, can also occur in an optomechanical system through mechanical effects of light. A typical example is optomechanically induced transparency (OMIT) which has been demonstrated theoretically^{14,15,16} and experimentally^{17} in an optomechanical system. The process of OMIT is that the presence of a strong control field and a weak probe field induce an antiStokes field produced from the scattering of light from the control field. Destructive interference between the antiStokes field and the probe field can suppress the buildup of an intracavity probe field and then lead to a transparent window in transmission spectrum of the probe field. This physical process can also be intuitively explained by a Λ configuration picture constructed by the optical and mechanical modes. This interesting phenomenon provides a special platform for performing precision measurement^{18,19,20}, such as optical mass sensor^{21,22,23} and precision measurement of electrical charges^{24,25}.
Precision measurement is one of the most significant tasks in modern physics. The mechanical resonators hold the promise for realizing precision measurement and can be achieved by two types of systems, that is, optomechanical and electromechanical systems. Generally speaking, optomechanical measurements is considered to have higher sensitivity than electromechanical measurements^{26}. In an optomechanical system, the precision measurement were usually carried out via the transmission spectrum of the probe field in OMIT. Some previous studies^{25} have shown that resonantly enhanced feedbackbackaction arising from radiation pressure can be substantively modified by the Coulomb interactions, and the transparency window width reveals a strong dependence on the charge number, which makes measurement of the charge number possible. Additionally, a tunable doubleOMIT have been observed from the output field in an optomechanical system induced by the Coulomb interactions, which might be applied to measure the Coulomb coupling strength^{27}. However, the precision measurement of a magnetic field in an optomechanical system is still unknown.
In this paper, we focus on a hybrid optomechanical system, in which one end of a moveable mirror was passed current and the whole system was placed in a magnetic field. We find that the effective cavity resonance frequency can be modified in the presence of the magnetic field. A resonance valley in the transmission curve of the probe field therefore will shift due to the electromagnetic interactions. Furthermore, the steadystate position of the mechanical oscillator (MO) will be affected coram the electromagnetic interactions and the transparency window of the OMIT will change correspondingly. Our scheme shows that an asymmetric transparency window appears in the transmission spectrum of the probe field and also the width of this window can be tunable by the electromagnetic interactions. Additionally, the current intensity plays a crucial role in our study, which determines the relationship between the probe power transmission and the magnetic field strength. As a result, we believe that our scheme enables a potentially practical proposal for precision measurement of the magnetic field.
Results
Model, Hamiltonian, steady states and the probe power transmission
The physical pattern under investigation is a hybrid optomechanical system. The system consists of an optical cavity with a movable boundary, illustrated here as a highQ FabryPérot cavity in which one mirror was passed surface current, acting like a MO. The whole system was placed in a magnetic field, as sketched shown in Fig. 1. The singlemode cavity field with eigenfrequency ω _{c} couples to the MO with effective mass m and frequency Ω_{m} via radiation pressure. Now we presume that a strong driving field with frequency ω _{l} and a weak probe field with frequency ω _{p} are applied on the cavity. The Hamiltonian of the driven optomechanical system can therefore be written as^{24}:
where the first term describes the energy for the MO with \(\hat{x}\) and \(\hat{p}\) being the position and momentum operators, respectively. The second term is the free Hamiltonian for the cavity with the annihilation (creation) operator \(\hat{a}\) (\({\hat{a}}^{\dagger }\)). The third term describes the interaction Hamiltonian between the cavity and MO with a coupling strength G. The next term presents the electromagnetic interaction Hamiltonian where ξ is the Amperes coefficient which is determined by the current intensity and the effective range of action. The last two terms represent the Hamiltonian of the driving fields. The coupling parameter η _{c} is chosen to be the critical coupling value 1/2 and κ the total decay rate of the cavity. \({\varepsilon }_{{\rm{i}}}=\sqrt{{P}_{{\rm{i}}}/\hslash {\omega }_{{\rm{i}}}}\) (with i = l, p) are the amplitudes of the input fields with P _{l} the pump power of the driving field and P _{p} the power of the probe field. The HeisenbergLangevin equations can be obtain as follows:
where Δ_{c} = ω _{l} − ω _{c} and δ = ω _{p} − ω _{l}. The decay rates for the optical κ and MO γ _{m} have been introduced classically. Furthermore, the meanfield approximation is used and the quantum noise terms are dropped safely in the semiclassical approximation^{1}. We first denote \(\bar{a}\) and \(\bar{x}\) the intracavity field and mechanical displacement for the static solution for the case that the control field is much stronger than the probe field and all time derivatives vanish. From Eq. (2), it follow immediately that \(\bar{a}\) and \(\bar{x}\) must fulfill the self consistent equations:
where \(\bar{{\rm{\Delta }}}={{\rm{\Delta }}}_{{\rm{c}}}G\bar{x}\) is the effective cavity detuning, depending on the steadystate position \(\bar{x}\) of the MO. In other words, the effective cavity frequency \({\omega }_{{\rm{c}}}G\bar{x}\) can be adjusted by controlling the electromagnetic interaction ξB. It reminds us the possibility to achieve the precision measurement of the magnetic field in our scheme.
In the case of a weak probe field (compared to the driving field), the general expression of the probe power transmission, this is, the ratio of the probe power returned from the system divided by the input probe power
where \(f(\delta ,B)=\hslash {G}^{2}{\bar{a}}^{2}\chi (\delta )/[\kappa \mathrm{/2}+i(\bar{{\rm{\Delta }}}\delta )]\), with \(\chi (\delta )=\mathrm{1/}m({{\rm{\Omega }}}_{m}^{2}{\delta }^{2}i{\gamma }_{m}\delta )\) is the susceptibility of the MO. The detailed solution are described in the Methods.
In what follows, we numerically research the transmission spectrum of the probe field in our scheme. We show that the transmission curve appears a strong dependence on the electromagnetic interactions. Moreover, the measurement sensitivity can be improved by adjusting the current intensity. We believe that our study will be useful for measuring the magnetic field accurately. The parameters used in this work are analogous to those of ref.^{28} for the MO. This is m = 100 pg, G/2π = −11 MHz/nm, Ω_{m}/2π = 0.1 MHz, γ _{m}/2π = 0.2 kHz, κ = 0.2Ω_{m} and the wavelength of the driving field λ _{c} = 2πc/ω _{c} = 532 nm. We assume that the units of Amperes coefficient ξ = 2.0 × 10^{−5} A · m for the current intensity I = 1 mA.
Electromagnetic interactions induced a shift of the resonance valley in the transmission spectrum of the probe field
Firstly, we investigate the shift of the resonance valley in the transmission curve of the weak probe field which results from the electromagnetic interactions. In Fig. 2, we plot the probe power transmission t _{p}^{2} vary with δ under different magnetic field strength B. It is shown that t _{p}^{2} has the reversed Lorentzianlike transmission shape and the probe field is almost completely absorbed near the resonance condition. In the absence of the magnetic field B = 0 nT, i.e., without the electromagnetic interactions, the resonance valley appears at the position δ/Ω_{m} = 1. The resonance condition will change in the present of the electromagnetic interactions which leads to the shift of the resonance valley. As shown in Fig. 2, as the magnetic field strength B increases, the shift of the resonance valley becomes larger. The ultimate physical mechanism for this interesting phenomenon is as follow: The effective cavity resonance frequency \({\omega }_{{\rm{c}}}^{^{\prime} }={\omega }_{{\rm{c}}}G\bar{x}\) shows a strong dependence on the steadystate position \(\bar{x}\) which changes when we adjust the magnetic field intensity B. The transmission spectrum of the probe field therefore shift by the term \(G\bar{x}/{{\rm{\Omega }}}_{{\rm{m}}}\) due to the electromagnetic interactions. Such electromagnetic interactions induced shift of the resonance valley might be applied to measure the magnetic field.
Asymmetry transparency window in OMIT induced by electromagnetic interactions
The probe power transmission t _{p}^{2} as a function of δ/Ω_{m} and magnetic field strength B shows an interesting feature of OMIT induced by electromagnetic interactions in our scheme. It can be see from Fig. 3 that a general transparency window (black solid line) appears at δ/Ω_{m} = 1 in the absence of the electromagnetic interactions. Different from the traditional OMIT, however, the symmetry of the transparency window is broken once the electromagnetic interactions was presented and the asymmetry window is analogous to the Fano resonance window, as red solid line shown. The asymmetric transparency window becomes wider in increasing with the intensity of the magnetic field. A previous study^{25} has shown that the window widths in some special regions of the OMIT vary sharply with the charge number, which makes precise measurement of the charge number possible. In our scheme, the width of such asymmetry transparency window also shows a strong dependence on the electromagnetic interactions, which may be used to detect the value of magnetic field.
There are two minimums in the probe power transmission shown in Fig. 3, which can be evaluated by
where δ _{−} and δ _{+} are the two points corresponding to minimums of t _{p}^{2}. Here, we define the asymmetry transparency window width d in Fig. 3 as d = δ _{−}/Ω_{m} − δ _{+}/Ω_{m}. In order to discuss the possibility of measuring the strength of magnetic field by the electromagnetic interactions, we plot the window width d as a function of magnetic field strength B in Fig. 4. It is shown that the window width d almost linearly increases with the magnetic field strength B within the regime \(B\in [0,0.6]\,{\rm{nT}}\). However, when we consider the magnetic field strength greater than 0.6 nT, the growth trend of the window width d varying with B is significantly accelerated, which almost squarely increases. Such interesting relationship reminds us of the possibility of detecting the magnetic field strength B by measuring the separation d in the probe power transmission spectrum of the output field.
Improving a measurement sensitivity of the magnetic field by adjusting the current intensity
Up to now, we have shown that electromagnetic interactions can induce a shift of the resonance valley in the transmission spectrum of the probe field as well as an asymmetric transparency window in OMIT, which may enable a potentially practical scheme for the measurement of magnetic field. In what follows, we mainly research about how to improve the measurement sensitivity by adjusting the current intensity. The probe power transmission t _{p}^{2} varying with the magnetic field strength B and the current intensity I is shown in Fig. 5. For weak electromagnetic interactions (the magnetic field strength B = 0.4 nT and the current intensity I = 1 mA), the maximal probe power transmission is quite low (about 0.1). As expected, the efficiency of the probe power transmission is enhanced when we reinforce the electromagnetic interactions in our system. The maximal t _{p}^{2} increases to about 0.3 when we consider the magnetic field strength B = 0.6 nT and the current intensity I = 1.6 mA. The maximal efficiency of the probe power transmission increases as both the magnetic field strength and the current intensity increases, and the maximum values of t _{p}^{2} are about 0.5 and 0.6 corresponding to the magnetic field strength B = 0.75, 0.8 nT and the current intensity I = 1.9, 2.0 mA, respectively. These results imply that resonantly enhanced feedbackbackaction arising from radiation pressure can be substantively modified in the presence of electromagnetic interactions. From above discussion, the effective cavity resonance frequency \({\omega }_{{\rm{c}}}^{^{\prime} }={\omega }_{{\rm{c}}}G\bar{x}\) depends on the applied magnetic field and the changes of the cavity field directly reflected in the probe power transmission t _{p}^{2}.
A high dependence of the probe power transmission t _{p}^{2} on the magnetic field strength B and current intensity I is shown in Fig. 6, where the relationship between t _{p}^{2} and magnetic field strength B fits a parabolic growth pattern. Furthermore, we find that the growth trend of t _{p}^{2} varying with magnetic field strength B is quite different for different current intensity. Such current dependent probe transmission enables an attractive device to improve the measurement accuracy in our scheme. For example, for the current intensity I = 1 mA (as the green dashdotted line shown), the efficiency of probe power transmission t _{p}^{2} changes from 0.05 to 0.27 when the magnetic field strength increasing from 0 to 1 nT. The growth trend of the probe power transmission varying with the magnetic field strength distinctly accelerate for a larger current (I = 1.5 mA, shown in the blue dashed line) and the maximal probe power transmission t _{p}^{2} increases to about 1.0 for the current intensity I = 2 mA (shown in the red dotted line). Here, we define a sensitivity coefficient \(\eta =\tfrac{{{t}_{{\rm{p}}}}_{{\rm{\max }}}^{2}{{t}_{{\rm{p}}}}_{{\rm{\min }}}^{2}}{{{t}_{{\rm{p}}}}_{{\rm{\max }}}^{2}+{{t}_{{\rm{p}}}}_{{\rm{\min }}}^{2}}\times \mathrm{100 \% }\) which is applied to distinguish each 0.1 nT of the magnetic field strength. The average sensitivity coefficient η under different current values can be calculated, and we obtain η _{green} = 9.60%, η _{blue} = 11.26% and η _{red} = 14.71% corresponding to the current intensity I = 1.0, 1.5, 2.0 mA, respectively, which offer the possibility of improving the measurement sensitivity of the magnetic field strength by controlling the current values.
Discussion
We have analyzed the transmission of the weak probe field in a hybrid optomechanical system with electromagnetic interactions. We find that the resonance valley of the probe transmission shifts obviously in the presence of the magnetic field due to modification of the effective cavity resonance frequency under the electromagnetic interactions. Furthermore, an asymmetric transparency window appears in OMIT, whose width dependents sensitively on the power of the electromagnetic interactions. Additionally, the measurement sensitivity of the magnetic field is markedly affected by current intensity. As a result, we show that our scheme provides an alternative way to measure the magnetic field with a precision of 0.1 nT.
Methods
Equation (2) are intrinsically nonlinear and hard to be solved exactly. It has been shown that bistable and chaotic behavior^{29} may occur when the pump power is high enough. Similar phenomena have also been revealed in other nonlinear system with feedback, such as nonlinear optics^{30} and economic evolution^{31,32}. In the present work, the pump power of about 1 nW is used, which is too low to reach the bistable region. In this case, the perturbation method can be used to solve Eq. (2) analytically, providing that the probe field is much weaker than the control field^{17}. By using \(a=\bar{a}+\delta a\) and \(x=\bar{x}+\delta x\), where δa and δx are corresponding to the fluctuations around the steadystate solutions of the a and x, respectively. Thus, δa and δx obey the following nonlinear matrix equation:
where \(\diamond \cdot {\rm{\Phi }}={(d\delta a/dt,\hat{{\rm{\Psi }}}\delta x)}^{T}\), Φ = (δa, δx)^{T}, ρ = (1, 0)^{T}, and
In this work, we mainly focus on the linear responding of our system and neglect the nonlinear terms −iGδaδx and −ħGδa*δa which may result in higherorder sidebands^{33,34}. Next, by using the following ansatz:
In the present work, we only focus on the probe field’s transmission at frequency ω _{l} + Ω_{m}. In this sense, the matrix equations of interest are:
where \(\mho ={({a}_{},{a}_{+},{x}_{1})}^{T}\), \(\eth={(\bar{a}{x}_{1},\bar{a}{x}_{1}^{\ast },\bar{a}{a}_{+}^{\ast }+{\bar{a}}^{\ast }{a}_{})}^{T}\), \(\eth=(\sqrt{{\eta }_{{\rm{c}}}\kappa }{\varepsilon }_{{\rm{p}}},\,\mathrm{0,}\,0)\) and
with \({\rm{\Theta }}=i{{\rm{\Delta }}}_{c}iG\bar{x}\kappa \mathrm{/2}\) and \(\Re ={{\rm{\Omega }}}_{{\rm{m}}}^{2}{\delta }^{2}i{\gamma }_{{\rm{m}}}\delta \). Therefore, the solution of interest is
with
and the mechanical susceptibility
Using the inputoutput relation^{35}, one obtains:
and the transmission of the probe beam is given by:
which defined by the ratio of the output and input field amplitudes at the probe frequency.
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References
 1.
Aspelmeyer, M., Kippenberg, T. J. & Marquardt, F. Cavity optomechanics. Rev. Mod. Phys. 86, 1391 (2014).
 2.
Børkje, K., Nunnenkamp, A. & Teufel, J. D. et al. Signatures of nonlinear cavity optomechanics in the weak coupling regime. Phys. Rev. Lett. 111, 053603 (2013).
 3.
Xiong, H., Huang, Y. M., Wan, L. L. & Wu, Y. Vector cavity optomechanics in the parameter configuration of optomechanically induced transparency. Phys. Rev. A 94, 013816 (2016).
 4.
Chan, J., Alegre, T. P. M. & SafaviNaeini, A. H. et al. Laser cooling of a nanomechanical oscillator into its quantum ground state. Nature 478, 7367 (2011).
 5.
Teufel, J. D., Donner, T. & Li, D. et al. Sideband cooling of micromechanical motion to the quantum ground state. Nature 475, 7356 (2011).
 6.
Gröblacher, S., Hammerer, K. & Vanner, M. R. et al. Observation of strong coupling between a micromechanical resonator and an optical cavity field. Nature 460, 7256 (2009).
 7.
Braginsky, V. B. & Vyatchanin, S. P. Low quantum noise tranquilizer for FabryPerot interferometer. Phys. Lett. A 293, 228 (2002).
 8.
Xiong, H., Si, L. G., Yang, X. & Wu, Y. Asymmetric optical transmission in an optomechanical array. Appl. Phys. Lett. 107, 091116 (2015).
 9.
Xiong, H., Kong, C., Yang, X. & Wu, Y. Optical polarizer based on the mechanical effect of light. Opt. Lett. 18, 4316–4319 (2016).
 10.
Palomaki, T. A., Teufel, J. D., Simmonds, R. W. & Lehnert, K. W. Entangling mechanical motion with microwave fields. Science 342, 6159 (2013).
 11.
Lin, Q., Rosenberg, J. & Chang, D. et al. Coherent mixing of mechanical excitations in nanooptomechanical structures. Nat. Photon. 4, 236–242 (2010).
 12.
SafaviNaeini, A. H., Alegre, T. P. M. & Chan, J. et al. Electromagnetically induced transparency and slow light with optomechanics. Nature 472, 7341 (2011).
 13.
Liu, Y. C., Li, B. B. & Xiao, Y. F. Electromagnetically induced transparency in optical microcavities. Nanophotonics 10, 1515 (2017).
 14.
Hou, B. P., Wei, L. F. & Wang, S. J. Optomechically induced transparency and absorption in hybridized optomechanical systems. Phys. Rev. A. 92, 033829 (2015).
 15.
Xiong, H., Si, L. G. & Zheng, A. S. et al. Higherorder sidebands in optomechanically induced transparency. Phys. Rev. A 86, 013815 (2012).
 16.
Kronwald, A. & Marquardt, F. Optomechanically induced transparency in the nonlinear quantum regime. Phys. Rev. Lett. 111, 133601 (2013).
 17.
Weis, S., Rivire, R. & Delglise, S. et al. Optomechanically induced transparency. Science 330, 6010 (2010).
 18.
Gavartin, E., Verlot, P. & Kippenberg, T. J. A hybrid onchip optomechanical transducer for ultrasensitive force measurements. Nat. nanotechnology 7, 509514 (2012).
 19.
Krause, A. G., Winger, M., Blasius, T. D. & Painter, O. A highresolution microchip optomechanical accelerometer. Nat. Photonics 6, 768–772 (2012).
 20.
Xiong, H., Liu, Z. X. & Wu, Y. Highly sensitive optical sensor for precision measurement of electrical charges based on optomechanically induced differencesideband generation. Opt. Lett. 42, 3630 (2017).
 21.
Li, J. J. & Zhu, K. D. Nonlinear optical mass sensor with an optomechanical microresonator. Appl. Phys. Lett. 14, 141905 (2012).
 22.
Chiu, H. Y., Hung, P., Postma, H. W. C. & Bockrath, M. Atomicscale mass sensing using carbon nanotube resonators. Nano Lett. 8, 4342 (2008).
 23.
Naik, A. K., Hanay, M. S., Hiebert, W. K. & Roukes, M. L. Towards singlemolecule nanomechanical mass spectrometry. Nat. Nanotechnol. 4, 445 (2009).
 24.
Xiong, H., Si, L. G. & Wu, Y. Precision measurement of electrical charges in an optomechanical system beyond linearized dynamics. Appl. Phys. Lett. 110, 171102 (2017).
 25.
Zhang, J. Q., Li, Y., Feng, M. & Xu, Y. Precision measurement of electrical charge with optomechanically induced transparency. Phys. Rev. A 86, 053806 (2012).
 26.
Xiong, C., Fan, L., Sun, X. et al. Cavity piezooptomechanics: Piezoelectrically excited, optically transduced optomechanical resonators. Appl. Phys. Lett. 102, 021110 (2013).
 27.
Ma, P. C., Zhang, J. Q., Xiao, Y. et al. Tunable double optomechanically induced transparency in an optomechanical system. Phys. Rev. A. 90, 043825 (2014).
 28.
Thompson, J. D., Zwickl, B. M., Jayich, A. M. et al. Strong dispersive coupling of a highfinesse cavity to a micromechanical membrane. Nature 452, 72 (2008).
 29.
Lü, X. Y., Jing, H., Ma, Y. & Wu, Y. P TSymmetryBreaking Chaos in Optomechanics. Phys. Rev. Lett. 114, 250601 (2015).
 30.
Yang, W. X. Highorder harmonics in a quantum dot and metallic nanorod complex. Opt.Lett. 40, 4903 (2015).
 31.
Shi, Y. & Pan, M. Evolutionary dynamics of social tolerance in the economic interaction model with local social cost functions. Appl. Econ. Lett. 24, 75–79 (2017).
 32.
Shi, Y., Pan, M. & Peng, D. Replicator dynamics and evolutionary game of social tolerance: The role of neutral agents. Econ. Lett. 159, 10–14 (2017).
 33.
Xiong, H., Si, L. G., Lü, X. Y. & Wu, Y. Nanosecondpulsecontrolled higherorder sideband comb in a GaAs optomechanical disk resonator in the nonperturbative regime. Ann. Phys. 349, 43–54 (2014).
 34.
Xiong, H., Si, L. G., Lü, X. Y. & Wu, Y. Carrierenvelope phasedependent effect of highorder sideband generation in ultrafast driven optomechanical system. Opt. Lett. 38, 353 (2013).
 35.
Gardiner, C. W. & Zoller, P. Quantum Noise. Springer (2004).
Acknowledgements
The work was supported by the National Science Foundation of China (Grant Nos 11405061, 11375067, and 11574104) and the National Key Research and Development Program of China (Grant No. 2016YFA0301203).
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L.Z.X. carried out the calculations, wrote the main manuscript text and prepared all figures and W.B., K.C., S.L.G., H.X. and Y.W. are participated in the discussions. All authors reviewed the manuscript and contributed to the interpretation of the work and the writing of the manuscript.
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