Simultaneous unidirectional reciprocal filters of electromagnetic and elastic waves based on the modal symmetry of phoxonic crystal waveguides and cavity
Introduction
In recent years, the abilities of guiding, controlling and confining electromagnetic (EM) and elastic waves simultaneously have attracted much attention in periodic or quasiperiodic structures. These structures are termed as phoxonic crystals (PhXCs) [1], [2], [3], optomechanical crystals [4], [5], or phoxonic quasicrystals [6], [7], [8], which possess the phoxonic bandgaps (the coexistence of photonic and phononic bandgaps) [1], [6]. PhXCs provide the possibility to achieve compact on-chip solutions for various dual optical and acoustic applications. Such integrated platform has been used to realize enhancing acoustic-optical interaction [9], [10], [11], [12], [13], [14] and opto-mechanical [5], [10], [14] on a wavelength scale, phoxonic sensing [15], phoxonic cavities [16] and filters [17].
It is indispensable to develop unidirectional routing networks to realize the independent operation of optical and acoustic signals on an integrated platform. Thus unidirectional transmission components are important in optical or acoustic circuits since they can offer unidirectional propagation of optical or acoustic signals [18], [19], [20], [21]. Considerable efforts have been dedicated to independently investigate the unidirectional transmission of the light or sound. Unidirectional propagation can be achieved by breaking the time-reversal symmetry based on the magneto-optical effect for light [22], [23], [24], using macroscopic flow field for sound [25], [26], and using nonlinear effect for both light and sound [27], [28], [29], [30], [31], [32]. Alternatively, unidirectional optical or acoustic propagation has also been intensively realized by breaking the spatial-inversion symmetry with the use of the artificial structures with reciprocal materials, such as gratings [33], metasurfaces [34], and photonic or phononic crystals [35], [36], [37], [38], [39], [40]. In addition, the unidirectional transmission of elastic waves has also been realized in solid/solid phononic crystal [41], [42]. The size of those devices can be remarkably reduced since this kind of structures avoids the use of external sources (e.g. magnetic field or high-intensity sources).
The coexistence of photonic and phononic unidirectional transmission in PhXCs allows for the potential route to realize integrated management of light and sound, highly controllable photon-phonon interactions with an ultracompact footprint size, thus the concept of phoxonic unidirectional transmission was recently proposed and investigated based on hybrid structures of grating-phoxonic crystals by combining diffraction and bandgap effects [43]. The undirectional transmission proposed by Chen et al. is based on the phoxonic structures of solid rods in air, meaning that the acoustic wave is propagated in the air [43]. Acousto-optic effect stems from the elastic strain caused by the elastic wave passing through the medium [9], [13]. However, the elastic strain of acoustic wave in air is rather weak, making that the acousto-optic effect in the air will be barely noticeable. Thus those structures are not suitable for enhancing acousto-optic effect. In this letter, we achieve the dual unidirectional propagation of EM and elastic waves using a single configuration of solid/solid PhXC, which involves a relatively simpler technological process for actual fabrication compared with the composite structures. Furthermore, the proposed phoxonic structure of solid rods in solid ensures that the elastic wave is propagated in the solid, enabling that the acousto-optic effect can be possibly enhanced. The functionality is achieved by matching and mismatching modal symmetry between resonant cavity and waveguides. Although this mechanism has been used to independently achieve unidirectional filters for photons in photonic crystal [35] and phonons in phononic crystals [37], [39], the coexistence of unidirectional propagation for EM and elastic waves doesn't be easily obtained due to the different characteristics of photonic and phononic modes in a same structure. The unidirectional transmission is essentially reciprocal due to the passive and linear structure. Such an unidirectional filter allows a new potential possibility to realize integrated management of photons and phonons, and enhance photon-phonon interactions with an ultracompact footprint size.
Section snippets
Model and methods
The proposed device is based on a two-dimensional (2D) PhXC formed as a square lattice of infinite long rods (inclusions) immersed in matrix. The inclusions and matrix are tungsten and polymethyl methacrylate (PMMA), respectively. These materials have been used in the Ref. [17] due to their suitable contrasts in elastic and dielectric constants. The phoxonic structure consists of a resonant cavity and two mutually orthogonal waveguides (labeled W1 and W2), as shown in Fig. 1(a). The resonant
Simulation and analysis
To demonstrate the simultaneous unidirectional reciprocal filtering of EM and elastic waves, we calculate the transmission ( and ) and reflection ( and ) of the TM wave (Fig. 1(b)) and longitudinal elastic wave (P waves, normal harmonic vibration) (Fig. 1(c)) for the case of forward incidence and backward incidence, respectively. For forward incidence, the input EM or elastic Gaussian wave centered at the central line of the waveguide W1 is launched from the
Conclusions
In summary, we have studied the simultaneous unidirectional filtering of the EM and elastic waves in the PhXC structure composed of a resonant cavity and two mutually perpendicular waveguides. The physical mechanism is to break the spatial-reversal symmetry of the system originating from the symmetry match and mismatch of the defect and waveguide modes. Although the phoxonic one-way filtering can be achieved, the device itself is essentially reciprocal. Compared to the previously proposed
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This work was supported by the National Natural Science Foundation of China (Grant Nos. 11664024, 11704175, 11604136) and the Key Project of Natural Science Foundation of Jiangxi Province (Grant No. 20171ACB21020).
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