Статті в журналах з теми "Phoxonic"

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1

Zhao, Shuyi, Linlin Lei, Qin Tang, Feng Xin, and Tianbao Yu. "Dual Optical and Acoustic Negative Refraction in Phoxonic Crystals." Photonics 9, no. 12 (November 28, 2022): 908. http://dx.doi.org/10.3390/photonics9120908.

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We report dual optical and acoustic negative refraction based on a defect-free phoxonic crystal within a triangular lattice. The phoxonic negative refraction is achieved based on abnormal dispersion effect, by intentionally creating convex equal-frequency contours for both photonic and phononic modes. As a potential application, negative refraction imaging for both photonic and phononic modes is also achieved. Numerical simulations based on the finite element method demonstrate the coexistence of negative refraction and the resultant imaging for electromagnetic and acoustic waves. Compared with the defect-based bandgap effects that need low fault tolerance, phoxonic negative refraction relying on passbands has considerable advantages in realizing controllable propagation of waves. The new scheme for the simultaneous control of electromagnetic and acoustic waves provides a potential platform for designing novel phoxonic devices.
2

Alonso-Redondo, Elena, Hannah Huesmann, El-Houssaine El Boudouti, Wolfgang Tremel, Bahram Djafari-Rouhani, Hans-Juergen Butt, and George Fytas. "Phoxonic Hybrid Superlattice." ACS Applied Materials & Interfaces 7, no. 23 (April 9, 2015): 12488–95. http://dx.doi.org/10.1021/acsami.5b01247.

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3

Pennec, Yan, Vincent Laude, Nikos Papanikolaou, Bahram Djafari-Rouhani, Mourad Oudich, Said El Jallal, Jean Charles Beugnot, Jose M. Escalante, and Alejandro Martínez. "Modeling light-sound interaction in nanoscale cavities and waveguides." Nanophotonics 3, no. 6 (December 1, 2014): 413–40. http://dx.doi.org/10.1515/nanoph-2014-0004.

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AbstractThe interaction of light and sound waves at the micro and nanoscale has attracted considerable interest in recent years. The main reason is that this interaction is responsible for a wide variety of intriguing physical phenomena, ranging from the laser-induced cooling of a micromechanical resonator down to its ground state to the management of the speed of guided light pulses by exciting sound waves. A common feature of all these phenomena is the feasibility to tightly confine photons and phonons of similar wavelengths in a very small volume. Amongst the different structures that enable such confinement, optomechanical or phoxonic crystals, which are periodic structures displaying forbidden frequency band gaps for light and sound waves, have revealed themselves as the most appropriate candidates to host nanoscale structures where the light-sound interaction can be boosted. In this review, we describe the theoretical tools that allow the modeling of the interaction between photons and acoustic phonons in nanoscale structures, namely cavities and waveguides, with special emphasis in phoxonic crystal structures. First, we start by summarizing the different optomechanical or phoxonic crystal structures proposed so far and discuss their main advantages and limitations. Then, we describe the different mechanisms that make light interact with sound, and show how to treat them from a theoretical point of view. We then illustrate the different photon-phonon interaction processes with numerical simulations in realistic phoxonic cavities and waveguides. Finally, we introduce some possible applications which can take enormous benefit from the enhanced interaction between light and sound at the nanoscale.
4

Djafari-Rouhani, Bahram, Said El-Jallal, Mourad Oudich, and Yan Pennec. "Optomechanic interactions in phoxonic cavities." AIP Advances 4, no. 12 (December 2014): 124602. http://dx.doi.org/10.1063/1.4903226.

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5

Papanikolaou, N., I. E. Psarobas, N. Stefanou, B. Djafari-Rouhani, B. Bonello, and V. Laude. "Light modulation in phoxonic nanocavities." Microelectronic Engineering 90 (February 2012): 155–58. http://dx.doi.org/10.1016/j.mee.2011.04.069.

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6

Djafari-Rouhani, Bahram, Said El-Jallal, and Yan Pennec. "Phoxonic crystals and cavity optomechanics." Comptes Rendus Physique 17, no. 5 (May 2016): 555–64. http://dx.doi.org/10.1016/j.crhy.2016.02.001.

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7

Xu, Bihang, Zhong Wang, Yixiang Tan, and Tianbao Yu. "Simultaneous localization of photons and phonons in defect-free dodecagonal phoxonic quasicrystals." Modern Physics Letters B 32, no. 07 (March 5, 2018): 1850096. http://dx.doi.org/10.1142/s0217984918500963.

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In dodecagonal phoxonic quasicrytals (PhXQCs) with a very high rotational symmetry, we demonstrate numerically large phoxonic band gaps (PhXBGs, the coexistence of photonic and phononic band gaps). By computing the existence and dependence of PhXBGs on the choice of radius of holes, we find that PhXQCs can possess simultaneous photonic and phononic band gaps over a rather wide range of geometric parameters. Furthermore, localized modes of THz photons and tens of MHz phonons may exist inside and outside band gaps in defect-free PhXQCs. The electromagnetic and elastic field can be confined simultaneously around the quasicrytals center and decay in a length scale of several basic cells. As a kind of quasiperiodic structures, 12-fold PhXQCs provide a good candidate for simultaneously tailoring electromagnetic and elastic waves. Moreover, these structures exhibit some interesting characteristics due to the very high symmetry.
8

Rosello-Mecho, Xavier, Gabriele Frigenti, Daniele Farnesi, Martina Delgado-Pinar, Miguel V. Andrés, Fulvio Ratto, Gualtiero Nunzi Conti, and Silvia Soria. "Microbubble PhoXonic resonators: Chaos transition and transfer." Chaos, Solitons & Fractals 154 (January 2022): 111614. http://dx.doi.org/10.1016/j.chaos.2021.111614.

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9

ZHOU Zhi-cheng, 周志成, 何灵娟 HE Ling-juan, 陈华英 CHEN Hua-ying, 于天宝 YU Tian-bao, and 刘念华 LIU Nian-hua. "The Sensing Characteristics of Phoxonic Crystal Microcavity." Acta Sinica Quantum Optica 24, no. 2 (2018): 198–203. http://dx.doi.org/10.3788/jqo20182402.0012.

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10

ZHOU Zhi-cheng, 周志成, 何灵娟 HE Ling-juan, 陈华英 CHEN Hua-ying, 于天宝 YU Tian-bao, and 刘念华 LIU Nian-hua. "The Sensing Characteristics of Phoxonic Crystal Microcavity." Acta Sinica Quantum Optica 24, no. 2 (2018): 198–203. http://dx.doi.org/10.3788/jqo20182402.0702.

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11

Rolland, Quentin, Samuel Dupont, Joseph Gazalet, Jean-Claude Kastelik, Yan Pennec, Bahram Djafari-Rouhani, and Vincent Laude. "Simultaneous bandgaps in LiNbO3 phoxonic crystal slab." Optics Express 22, no. 13 (June 24, 2014): 16288. http://dx.doi.org/10.1364/oe.22.016288.

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12

Xia, Baizhan, Haiyan Fan, and Tingting Liu. "Topologically protected edge states of phoxonic crystals." International Journal of Mechanical Sciences 155 (May 2019): 197–205. http://dx.doi.org/10.1016/j.ijmecsci.2019.02.037.

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13

Ma, Tian-Xue, Yue-Sheng Wang, Yan-Feng Wang, and Xiao-Xing Su. "Three-dimensional dielectric phoxonic crystals with network topology." Optics Express 21, no. 3 (January 28, 2013): 2727. http://dx.doi.org/10.1364/oe.21.002727.

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14

Almpanis, Evangelos, Nikolaos Papanikolaou, Georgios Gantzounis, and Nikolaos Stefanou. "Tuning the spontaneous light emission in phoxonic cavities." Journal of the Optical Society of America B 29, no. 9 (August 30, 2012): 2567. http://dx.doi.org/10.1364/josab.29.002567.

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15

Jin, Jun, Xiaohong Wang, Lamin Zhan, and Hongping Hu. "Strong quadratic acousto-optic coupling in 1D multilayer phoxonic crystal cavity." Nanotechnology Reviews 10, no. 1 (January 1, 2021): 443–52. http://dx.doi.org/10.1515/ntrev-2021-0034.

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Abstract Four methods are applied to calculate the acousto-optic (AO) coupling in one-dimensional (1D) phoxonic crystal (PXC) cavity: transfer matrix method (TMM), finite element method (FEM), perturbation theory, and Born approximation. Two types of mechanisms, the photoelastic effect (PE) and the moving interface effect (MI), are investigated. Whether the AO coupling belongs to linear or quadratic, the results obtained by the perturbation theory are in good agreement with the numerical results. We show that the combination method of FEM and perturbation theory has some advantages over Born approximation. The dependence of linear and quadratic couplings on the symmetry of acoustic and optical modes has been discussed in detail. The linear coupling will vanish if the defect acoustic mode is even symmetry, but the quadratic effect may be enhanced. Based on second-order perturbation theory, the contribution of each optical eigenfrequency to quadratic coupling is clarified. Finally, the quadratic coupling is greatly enhanced by tuning the thickness of the defect layer, which is an order of magnitude larger than that of normal defect thickness. The enhancement mechanism of quadratic coupling is illustrated. The symmetry of the acoustic defect mode is transformed from odd to even, and two optical defect modes are modulated to be quasi-degenerated modes. This study opens up a possibility to achieve tunable phoxonic crystals on the basis of nonlinear AO effects.
16

Hsiao, Fu-Li, Ying-Pin Tsai, Wei-Shan Chang, Chien-Chang Chiu, Bor-Shyh Lin, and Chi-Tsung Chiang. "Photo-Elastic Enhanced Optomechanic One Dimensional Phoxonic Fishbone Nanobeam." Crystals 12, no. 7 (June 23, 2022): 890. http://dx.doi.org/10.3390/cryst12070890.

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We investigated the strength of acousto-optical (AO) interaction in one-dimensional fishbone silicon nanobeam computationally. The structure can generate phononic and photonic band gaps simultaneously. We use defect cavity optical mode and slow light mode to interact with acoustic defect modes. The AO coupling rates are obtained by adding the optical frequency shifts, which result from photo-elastic effect and moving-boundary effect disturbances. The AO coupling rates are strongly dependent on the overlap of acoustic and optical mode distribution. The strength of AO interaction can be enhanced by choosing certain acoustic defect modes that are formed by the stretching of wings and that overlap significantly with optical fields.
17

Lei, Linlin, Tianbao Yu, Wenxing Liu, Tongbiao Wang, and Qinghua Liao. "Dirac cones with zero refractive indices in phoxonic crystals." Optics Express 30, no. 1 (December 21, 2021): 308. http://dx.doi.org/10.1364/oe.446356.

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18

Farnesi, D., S. Berneschi, G. Frigenti, G. Nunzi Conti, S. Pelli, P. Feron, T. Murzina, M. Ferrari, and S. Soria. "Phoxonic glass cavities based on whispering gallery mode resonators." Optical Materials: X 12 (December 2021): 100120. http://dx.doi.org/10.1016/j.omx.2021.100120.

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19

Rolland, Q., M. Oudich, S. El-Jallal, S. Dupont, Y. Pennec, J. Gazalet, J. C. Kastelik, G. Lévêque, and B. Djafari-Rouhani. "Acousto-optic couplings in two-dimensional phoxonic crystal cavities." Applied Physics Letters 101, no. 6 (August 6, 2012): 061109. http://dx.doi.org/10.1063/1.4744539.

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20

Hsiao, Fu-Li, Cheng-Yi Hsieh, Hao-Yu Hsieh, and Chien-Chang Chiu. "High-efficiency acousto-optical interaction in phoxonic nanobeam waveguide." Applied Physics Letters 100, no. 17 (April 23, 2012): 171103. http://dx.doi.org/10.1063/1.4705295.

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21

Wang, Zhong, Tianbao Yu, Tongbiao Wang, Wenxing Liu, Nianhua Liu, and Qinghua Liao. "Acousto-optic interactions for terahertz waves using phoxonic quasicrystals." Journal of Physics D: Applied Physics 51, no. 10 (February 19, 2018): 105110. http://dx.doi.org/10.1088/1361-6463/aaa98c.

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22

Ma, Xingfu, Hang Xiang, Xiane Yang, and Jiawei Xiang. "Dual band gaps optimization for a two-dimensional phoxonic crystal." Physics Letters A 391 (March 2021): 127137. http://dx.doi.org/10.1016/j.physleta.2021.127137.

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23

Aly, Arafa H., Samar M. Shaban, and Ahmed Mehaney. "High-performance phoxonic cavity designs for enhanced acousto-optical interaction." Applied Optics 60, no. 11 (April 9, 2021): 3224. http://dx.doi.org/10.1364/ao.420294.

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24

Aram, Mohammad Hasan, and Sina Khorasani. "Efficient Analysis of Confined Guided Modes in Phoxonic Crystal Slabs." Journal of Lightwave Technology 35, no. 17 (September 1, 2017): 3734–42. http://dx.doi.org/10.1109/jlt.2017.2721999.

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25

Rolland, Quentin, Samuel Dupont, Joseph Gazalet, and Jean-Claude Kastelik. "Acousto-optic couplings in two-dimensional Lithium Niobate phoXonic crystal." IOP Conference Series: Materials Science and Engineering 68 (November 26, 2014): 012006. http://dx.doi.org/10.1088/1757-899x/68/1/012006.

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26

Dupont, S., Q. Rolland, J. Gazalet, and J. C. Kastelik. "Acousto-optic couplings in a phoXonic crystal slab L1 cavity." Journal of Physics: Conference Series 490 (March 11, 2014): 012175. http://dx.doi.org/10.1088/1742-6596/490/1/012175.

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27

El-jallal, S., M. Oudich, Y. Pennec, B. Djafari-Rouhani, A. Makhoute, Q. Rolland, S. Dupont, and J. Gazalet. "Optomechanical interactions in two-dimensional Si and GaAs phoXonic cavities." Journal of Physics: Condensed Matter 26, no. 1 (November 25, 2013): 015005. http://dx.doi.org/10.1088/0953-8984/26/1/015005.

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28

Aram, Mohammad Hasan, and Sina Khorasani. "Optomechanical coupling strength in various triangular phoxonic crystal slab cavities." Journal of the Optical Society of America B 35, no. 6 (May 29, 2018): 1390. http://dx.doi.org/10.1364/josab.35.001390.

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29

Lucklum, Ralf, Mikhail Zubtsov, and Aleksandr Oseev. "Phoxonic crystals—a new platform for chemical and biochemical sensors." Analytical and Bioanalytical Chemistry 405, no. 20 (June 12, 2013): 6497–509. http://dx.doi.org/10.1007/s00216-013-7093-9.

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30

Korovin, Alexander V., Yan Pennec, and Bahram Djafari-Rouhani. "Unidirectional Coherent Phonon Emission in an Optomechanic Nanobeam Containing Coupled Cavities." Photonics 9, no. 9 (August 28, 2022): 610. http://dx.doi.org/10.3390/photonics9090610.

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Анотація:
Nonreciprocal phonon emission is predicted theoretically from the coherent excitation of two coupled optomechanical cavities arranged along a phoxonic crystal nanobeam. The latter consists of a periodic array of holes and stubs and exhibits simultaneous photonic and phononic bandgaps. It is shown that nonreciprocal phonon emission arises from a combined effect of the spatial symmetry of the cavities and their underlying coupled phononic modes and the temporal phase shift between the excitation sources. This demonstration paves the way for the development of advanced integrated phonon networks and circuits, in which mechanical waves connect different elements in phononic and optomechanical structures.
31

Almpanis, Evangelos, Nikolaos Papanikolaou, and Nikolaos Stefanou. "Breakdown of the linear acousto-optic interaction regime in phoxonic cavities." Optics Express 22, no. 26 (December 15, 2014): 31595. http://dx.doi.org/10.1364/oe.22.031595.

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32

Hsu, Jin-Chen, Tsung-Yi Lu, and Tzy-Rong Lin. "Acousto-optic coupling in phoxonic crystal nanobeam cavities with plasmonic behavior." Optics Express 23, no. 20 (September 23, 2015): 25814. http://dx.doi.org/10.1364/oe.23.025814.

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33

Lin, Tzy-Rong, Yin-Chen Huang, and Jin-Chen Hsu. "Optomechanical coupling in phoxonic–plasmonic slab cavities with periodic metal strips." Journal of Applied Physics 117, no. 17 (May 7, 2015): 173105. http://dx.doi.org/10.1063/1.4919754.

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34

Moradi, Pedram, and Ali Bahrami. "Design of an optomechanical filter based on solid/solid phoxonic crystals." Journal of Applied Physics 123, no. 11 (March 21, 2018): 115113. http://dx.doi.org/10.1063/1.5018840.

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35

Kipfstuhl, Laura, Felix Guldner, Janine Riedrich-Möller, and Christoph Becher. "Modeling of optomechanical coupling in a phoxonic crystal cavity in diamond." Optics Express 22, no. 10 (May 14, 2014): 12410. http://dx.doi.org/10.1364/oe.22.012410.

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36

El-Jallal, S., A. Mrabti, G. Lévêque, A. Akjouj, Y. Pennec, and B. Djafari-Rouhani. "Phonon interaction with coupled photonic-plasmonic modes in a phoxonic cavity." AIP Advances 6, no. 12 (December 2016): 122001. http://dx.doi.org/10.1063/1.4968615.

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37

Yu, Zejie, and Xiankai Sun. "Giant enhancement of stimulated Brillouin scattering with engineered phoxonic crystal waveguides." Optics Express 26, no. 2 (January 11, 2018): 1255. http://dx.doi.org/10.1364/oe.26.001255.

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38

Hsiao, Fu-Li, Hao-Yu Hsieh, Cheng-Yi Hsieh, and Chien-Chang Chiu. "Acousto–optical interaction in fishbone-like one-dimensional phoxonic crystal nanobeam." Applied Physics A 116, no. 3 (May 18, 2014): 873–78. http://dx.doi.org/10.1007/s00339-014-8456-6.

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39

Lei, Lin-Lin, Ling-Juan He, Wen-Xing Liu, Qing-Hua Liao, and Tian-Bao Yu. "Coexistence of photonic and phononic corner states in a second-order topological phoxonic crystal." Applied Physics Letters 121, no. 19 (November 7, 2022): 193103. http://dx.doi.org/10.1063/5.0127301.

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Recently, higher-order topological insulators (HOTIs) have been extended from the electronic system to classical wave systems. Beyond the conventional bulk-boundary correspondence, HOTIs can host zero-dimensional topologically protected corner states, which show the strong field localization and robustness against fabrication flaws. Here, we propose a second-order topological phoxonic crystal (PXC) based on a two-dimensional (2D) square lattice, of which different unit cell choices can show either a topologically trivial or non-trivial band structure characterized by the 2D Zak phase. The proposed PXC supports the coexistence of photonic and phononic topological corner states, and their robustness to disorders and defects is numerically demonstrated. Our work opens a venue for achieving simultaneous confinement of photons and phonons, which is potentially useful for exploring the interaction of photonic and phononic second-order topological states and for designing novel topological optomechanical devices.
40

Zhang, S., J. Yin, H. W. Zhang, and B. S. Chen. "Multi-objective optimization of two-dimensional phoxonic crystals with multi-level substructure scheme." International Journal of Modern Physics B 30, no. 09 (April 10, 2016): 1650046. http://dx.doi.org/10.1142/s0217979216500466.

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Phoxonic crystal (PXC) is a promising artificial periodic material for optomechanical systems and acousto-optical devices. The multi-objective topology optimization of dual phononic and photonic max relative bandgaps in a kind of two-dimensional (2D) PXC is investigated to find the regular pattern of topological configurations. In order to improve the efficiency, a multi-level substructure scheme is proposed to analyze phononic and photonic band structures, which is stable, efficient and less memory-consuming. The efficient and reliable numerical algorithm provides a powerful tool to optimize and design crystal devices. The results show that with the reduction of the relative phononic bandgap (PTBG), the central dielectric scatterer becomes smaller and the dielectric veins of cross-connections between different dielectric scatterers turn into the horizontal and vertical shape gradually. These characteristics can be of great value to the design and synthesis of new materials with different topological configurations for applications of the PXC.
41

Ma, Tian-Xue, Yue-Sheng Wang, and Chuanzeng Zhang. "Simultaneous Guidance of Surface Acoustic and Surface Optical Waves in Phoxonic Crystal Slabs." Crystals 7, no. 11 (November 19, 2017): 350. http://dx.doi.org/10.3390/cryst7110350.

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42

Dong, Hao-Wen, Yue-Sheng Wang, and Chuanzeng Zhang. "Topology Optimization of Chiral Phoxonic Crystals With Simultaneously Large Phononic and Photonic Bandgaps." IEEE Photonics Journal 9, no. 2 (April 2017): 1–16. http://dx.doi.org/10.1109/jphot.2017.2665700.

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43

Lin, Tzy-Rong, Chiang-Hsin Lin, and Jin-Chen Hsu. "Enhanced acousto-optic interaction in two-dimensional phoxonic crystals with a line defect." Journal of Applied Physics 113, no. 5 (February 7, 2013): 053508. http://dx.doi.org/10.1063/1.4790288.

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44

Dong, Hao-Wen, Yue-Sheng Wang, Tian-Xue Ma, and Xiao-Xing Su. "Topology optimization of simultaneous photonic and phononic bandgaps and highly effective phoxonic cavity." Journal of the Optical Society of America B 31, no. 12 (November 4, 2014): 2946. http://dx.doi.org/10.1364/josab.31.002946.

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45

Forzani, L., C. G. Mendez, R. Urteaga, and A. E. Huespe. "Design and optimization of an opto-acoustic sensor based on porous silicon phoxonic crystals." Sensors and Actuators A: Physical 331 (November 2021): 112915. http://dx.doi.org/10.1016/j.sna.2021.112915.

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46

Jin, Jun, Shan Jiang, Hongping Hu, Lamin Zhan, Xiaohong Wang, and Vincent Laude. "Acousto-optic cavity coupling in 2D phoxonic crystal with combined convex and concave holes." Journal of Applied Physics 130, no. 12 (September 28, 2021): 123104. http://dx.doi.org/10.1063/5.0060412.

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Moctezuma-Enriquez, D., P. Castro-Garay, Y. Rodriguez-Viveros, J. Manzanares-Martinez, and B. Manzanares-Martinez. "Phoxonic band gaps in porous silicon multilayers at frequencies of the visible and hypersound." Advanced Studies in Theoretical Physics 7 (2013): 907–14. http://dx.doi.org/10.12988/astp.2013.3666.

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Zhang, Ruiwen, and Junqiang Sun. "Design of Silicon Phoxonic Crystal Waveguides for Slow Light Enhanced Forward Stimulated Brillouin Scattering." Journal of Lightwave Technology 35, no. 14 (July 15, 2017): 2917–25. http://dx.doi.org/10.1109/jlt.2017.2704615.

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Laude, Vincent, Jean-Charles Beugnot, Sarah Benchabane, Yan Pennec, Bahram Djafari-Rouhani, Nikos Papanikolaou, Jose M. Escalante, and Alejandro Martinez. "Simultaneous guidance of slow photons and slow acoustic phonons in silicon phoxonic crystal slabs." Optics Express 19, no. 10 (May 3, 2011): 9690. http://dx.doi.org/10.1364/oe.19.009690.

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