Whispering-gallery wave

Last updated
Snapshot of an acoustic whispering-gallery mode calculated at a frequency of 69 Hz in an enclosed cylinder of air of the same diameter (33.7 m) as the whispering gallery in St Paul's Cathedral. Red and blue represent higher and lower air pressures, respectively, and the distortions in the grid lines show the displacements. In the case of the waves travelling one way round the gallery, the air particles move in elliptical trajectories. WGMVisualized.jpg
Snapshot of an acoustic whispering-gallery mode calculated at a frequency of 69 Hz in an enclosed cylinder of air of the same diameter (33.7 m) as the whispering gallery in St Paul's Cathedral. Red and blue represent higher and lower air pressures, respectively, and the distortions in the grid lines show the displacements. In the case of the waves travelling one way round the gallery, the air particles move in elliptical trajectories.

Whispering-gallery waves, or whispering-gallery modes, are a type of wave that can travel around a concave surface. Originally discovered for sound waves in the whispering gallery of St Paul's Cathedral, they can exist for light and for other waves, with important applications in nondestructive testing, lasing, cooling and sensing, as well as in astronomy.

Contents

Introduction


Whispering-gallery waves were first explained for the case of St Paul's Cathedral circa 1878 [3] by Lord Rayleigh, who revised a previous misconception [4] [5] that whispers could be heard across the dome but not at any intermediate position. He explained the phenomenon of travelling whispers with a series of specularly reflected sound rays making up chords of the circular gallery. Clinging to the walls the sound should decay in intensity only as the inverse of the distance — rather than the inverse square as in the case of a point source of sound radiating in all directions. This accounts for the whispers being audible all round the gallery.

Rayleigh developed wave theories for St Paul's in 1910 [6] and 1914. [7] Fitting sound waves inside a cavity involves the physics of resonance based on wave interference; the sound can exist only at certain pitches as in the case of organ pipes. The sound forms patterns called modes, as shown in the diagram. [1]

Many other monuments have been shown [8] to exhibit whispering-gallery waves, such as the Gol Gumbaz in Bijapur and the Temple of Heaven in Beijing.

Acoustic waves

Whispering-gallery waves for sound exist in a wide variety of systems. Examples include the vibrations of the whole Earth [9] or stars. [10]

Such acoustic whispering-gallery waves can be used in nondestructive testing in the form of waves that creep around holes filled with liquid, [11] for example. They have also been detected in solid cylinders [12] and spheres, [13] with applications in sensing, and visualized in motion on microscopic discs . [2] [14]

Whispering gallery waves are more efficiently guided in spheres than in cylinders because the effects of acoustic diffraction (lateral wave spreading) are then completely compensated. [15]

Electromagnetic waves

Optical whispering-gallery modes in a glass sphere of diameter 300 mm experimentally imaged with a fluorescence technique. The tip of an angle-cut optical fiber, visible on the right, excites the modes in the red region of the optical spectrum. Whispering gallery modes sphere.png
Optical whispering-gallery modes in a glass sphere of diameter 300 μm experimentally imaged with a fluorescence technique. The tip of an angle-cut optical fiber, visible on the right, excites the modes in the red region of the optical spectrum.

Whispering-gallery waves exist for light waves. [17] [18] [19] They have been produced in microscopic glass spheres or tori [20] [21] and in soap bubbles, [22] for example, with applications as optical resonators for lasing, [23] optomechanical cooling, [24] frequency comb generation [25] and optical sensing. [26] The light waves are guided around almost perfectly by total internal reflection, leading to Q factors in excess of 1010 being achieved. [27] This is far greater than the best values, about 104, that can be obtained in acoustics. [28] Optical modes in a whispering gallery resonator experience some loss due to a mechanism similar to quantum tunneling, even in theoretically ideal conditions. This loss has been known from research on optical waveguide theory and is dubbed tunneling ray attenuation in the field of fiber optics. [29] The Q factor is proportional to the decay time of the waves, which in turn is inversely proportional to both the surface scattering rate and the wave absorption in the medium making up the gallery.  Whispering-gallery waves for light have been investigated in chaotic galleries, [30] [31] whose cross-sections deviate from a circle. Such waves have been used in quantum information applications. [32]

Whispering-gallery waves have also been demonstrated for other electromagnetic waves such as radio waves, [33] microwaves, [34] terahertz radiation, [35] infrared radiation, [36] ultraviolet waves [37] and x-rays. [38] More recently, with the rapid development of microfluidic technologies, many integrated whispering gallery mode sensors, by combining the portability of lab‐on‐chip devices and the high sensitivity of whispering gallery mode resonators have emerged. [39] [40] The capabilities of efficient sample handling and multiplexed analyte detection offered by these systems have led to many biological and chemical sensing applications, especially for the detection of single particle or biomolecule. [41] [42]

Other systems

Whispering-gallery waves have been seen in the form of matter waves for neutrons, [43] and electrons, [44] and they have been proposed as an explanation for vibrations of a single nucleus. [45] Whispering gallery waves have also been observed in the vibrations of soap films as well as in the vibrations of thin plates [46] Analogies of whispering-gallery waves also exist for gravitational waves at the event horizon of black holes. [1] A hybrid of waves of light and electrons known as surface plasmons has been demonstrated in the form of whispering-gallery waves, [47] and likewise for exciton-polaritons in semiconductors. [48] Galleries simultaneously containing both acoustic and optical whispering-gallery waves have also been made, [49] exhibiting very strong mode coupling and coherent effects. [50] Hybrid solid-fluid-optical whispering-gallery structures have been observed as well. [51]

See also

Related Research Articles

<span class="mw-page-title-main">Optical microcavity</span>

An optical microcavity or microresonator is a structure formed by reflecting faces on the two sides of a spacer layer or optical medium, or by wrapping a waveguide in a circular fashion to form a ring. The former type is a standing wave cavity, and the latter is a traveling wave cavity. The name microcavity stems from the fact that it is often only a few micrometers thick, the spacer layer sometimes even in the nanometer range. As with common lasers, this forms an optical cavity or optical resonator, allowing a standing wave to form inside the spacer layer or a traveling wave that goes around in the ring.

Quantum metrology is the study of making high-resolution and highly sensitive measurements of physical parameters using quantum theory to describe the physical systems, particularly exploiting quantum entanglement and quantum squeezing. This field promises to develop measurement techniques that give better precision than the same measurement performed in a classical framework. Together with quantum hypothesis testing, it represents an important theoretical model at the basis of quantum sensing.

<span class="mw-page-title-main">Nonlinear X-wave</span>

In physics, a nonlinear X-wave (NLX) is a multi-dimensional wave that can travel without distortion.

Dissipative solitons (DSs) are stable solitary localized structures that arise in nonlinear spatially extended dissipative systems due to mechanisms of self-organization. They can be considered as an extension of the classical soliton concept in conservative systems. An alternative terminology includes autosolitons, spots and pulses.

The topological entanglement entropy or topological entropy, usually denoted by , is a number characterizing many-body states that possess topological order.

Within quantum technology, a quantum sensor utilizes properties of quantum mechanics, such as quantum entanglement, quantum interference, and quantum state squeezing, which have optimized precision and beat current limits in sensor technology. The field of quantum sensing deals with the design and engineering of quantum sources and quantum measurements that are able to beat the performance of any classical strategy in a number of technological applications. This can be done with photonic systems or solid state systems.

Patrick A. Lee is a professor of physics at the Massachusetts Institute of Technology (MIT).

<span class="mw-page-title-main">Oreste Piro</span> Argentine biophysicist

Oreste Piro is a dynamical systems theorist and biophysicist. He is at the Universitat de les Illes Balears (UIB) in Palma de Mallorca.

Within quantum cryptography, the Decoy state quantum key distribution (QKD) protocol is the most widely implemented QKD scheme. Practical QKD systems use multi-photon sources, in contrast to the standard BB84 protocol, making them susceptible to photon number splitting (PNS) attacks. This would significantly limit the secure transmission rate or the maximum channel length in practical QKD systems. In decoy state technique, this fundamental weakness of practical QKD systems is addressed by using multiple intensity levels at the transmitter's source, i.e. qubits are transmitted by Alice using randomly chosen intensity levels, resulting in varying photon number statistics throughout the channel. At the end of the transmission Alice announces publicly which intensity level has been used for the transmission of each qubit. A successful PNS attack requires maintaining the bit error rate (BER) at the receiver's end, which can not be accomplished with multiple photon number statistics. By monitoring BERs associated with each intensity level, the two legitimate parties will be able to detect a PNS attack, with highly increased secure transmission rates or maximum channel lengths, making QKD systems suitable for practical applications.

Searches for Lorentz violation involving photons provide one possible test of relativity. Examples range from modern versions of the classic Michelson–Morley experiment that utilize highly stable electromagnetic resonant cavities to searches for tiny deviations from c in the speed of light emitted by distant astrophysical sources. Due to the extreme distances involved, astrophysical studies have achieved sensitivities on the order of parts in 1038.

<span class="mw-page-title-main">Christopher Monroe</span> American physicist

Christopher Roy Monroe is an American physicist and engineer in the areas of atomic, molecular, and optical physics and quantum information science, especially quantum computing. He directs one of the leading research and development efforts in ion trap quantum computing. Monroe is the Gilhuly Family Presidential Distinguished Professor of Electrical and Computer Engineering and Physics at Duke University and was College Park Professor of Physics at the University of Maryland and Fellow of the Joint Quantum Institute and Joint Center for Quantum Computer Science until 2020 when he moved to Duke. He is also co-founder of IonQ, Inc.

Photonic molecules are a form of matter in which photons bind together to form "molecules". They were first predicted in 2007. Photonic molecules are formed when individual (massless) photons "interact with each other so strongly that they act as though they have mass". In an alternative definition, photons confined to two or more coupled optical cavities also reproduce the physics of interacting atomic energy levels, and have been termed as photonic molecules.

Quantum illumination is a paradigm for target detection that employs quantum entanglement between a signal electromagnetic mode and an idler electromagnetic mode, as well as joint measurement of these modes. The signal mode is propagated toward a region of space, and it is either lost or reflected, depending on whether a target is absent or present, respectively. In principle, quantum illumination can be beneficial even if the original entanglement is completely destroyed by a lossy and noisy environment.

<span class="mw-page-title-main">Roberto Morandotti</span> Italian physicist

Roberto Morandotti is a physicist and full Professor, working in the Energy Materials Telecommunications Department of the Institut National de la Recherche Scientifique. The work of his team includes the areas of integrated and quantum photonics, nonlinear and singular optics, as well as terahertz photonics.

Hyperuniform materials are characterized by an anomalous suppression of density fluctuations at large scales. More precisely, the vanishing of density fluctuations in the long-wave length limit distinguishes hyperuniform systems from typical gases, liquids, or amorphous solids. Examples of hyperuniformity include all perfect crystals, perfect quasicrystals, and exotic amorphous states of matter.

Kerr frequency combs are optical frequency combs which are generated from a continuous wave pump laser by the Kerr nonlinearity. This coherent conversion of the pump laser to a frequency comb takes place inside an optical resonator which is typically of micrometer to millimeter in size and is therefore termed a microresonator. The coherent generation of the frequency comb from a continuous wave laser with the optical nonlinearity as a gain sets Kerr frequency combs apart from today's most common optical frequency combs. These frequency combs are generated by mode-locked lasers where the dominating gain stems from a conventional laser gain medium, which is pumped incoherently. Because Kerr frequency combs only rely on the nonlinear properties of the medium inside the microresonator and do not require a broadband laser gain medium, broad Kerr frequency combs can in principle be generated around any pump frequency.

<span class="mw-page-title-main">Hidetoshi Katori</span> Japanese physicist

Hidetoshi Katori is a Japanese physicist and professor at the University of Tokyo best known for having invented the magic wavelength technique for ultra precise optical lattice atomic clocks. Since 2011, Katori is also Chief Scientist at the Quantum Metrology Lab, RIKEN.

Photonic topological insulators are artificial electromagnetic materials that support topologically non-trivial, unidirectional states of light. Photonic topological phases are classical electromagnetic wave analogues of electronic topological phases studied in condensed matter physics. Similar to their electronic counterparts, they, can provide robust unidirectional channels for light propagation. The field that studies these phases of light is referred to as topological photonics.

Toshiki Tajima is a Japanese theoretical plasma physicist known for pioneering the laser wakefield acceleration technique with John M. Dawson in 1979. The technique is used to accelerate particles in a plasma and was experimentally realized in 1994, for which Tajima received several awards such as the Nishina Memorial Prize (2006), the Enrico Fermi Prize (2015), the Robert R. Wilson Prize (2019), the Hannes Alfvén Prize (2019) and the Charles Hard Townes Award (2020).

<span class="mw-page-title-main">John Martin Kolinski</span> American applied physicist

John Martin Kolinski is an American engineer. He is a professor at EPFL and the head of the Laboratory of Engineering Mechanics of Soft Interfaces (EMSI) at EPFL's School of Engineering.

References

  1. 1 2 3 Wright, Oliver B. (2012). "Gallery of whispers". Physics World. 25 (2): 31–36. Bibcode:2012PhyW...25b..31W. doi:10.1088/2058-7058/25/02/36.
  2. 1 2 Oliver, Wright B.; Matsuda, Oliver. "Watching whispering-gallery waves". Laboratory of Applied Solid State Physics, Hokkaido University . Retrieved 2018-11-30.
  3. [Lord Rayleigh, Theory of Sound, vol. II, 1st edition, (London, MacMillan), 1878.]
  4. [J. Tyndall, The Science of Sound (New York, Philosophical Library), 1867, p. 20.]
  5. [G. B. Airy, On Sound and Atmospheric Vibrations, with the Mathematical Elements of Music (London, MacMillan), 1871, p. 145.]
  6. Rayleigh, Lord (1910). "CXII. The problem of the whispering gallery". The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science. 20 (120). Informa UK Limited: 1001–1004. doi:10.1080/14786441008636993. ISSN   1941-5982.
  7. Rayleigh, Lord (1914). "IX. Further applications of Bessel's functions of high order to the Whispering Gallery and allied problems". The London, Edinburgh, and Dublin Philosophical Magazine and Journal of Science. 27 (157). Informa UK Limited: 100–109. doi:10.1080/14786440108635067. ISSN   1941-5982.
  8. Raman, C. V. (1921–1922). "XV. On Whispering Galleries". Proceedings of the Indian Association for the Cultivation of Science. 7: 159.
  9. [Quantitative Seismology, K. Aki and P. G. Richards (University Science Books), 2009, Ch. 8]
  10. Reese, D. R.; MacGregor, K. B.; Jackson, S.; Skumanich, A.; Metcalfe, T. S. (1 March 2009). "Pulsation modes in rapidly rotating stellar models based on the self-consistent field method". Astronomy & Astrophysics. 506 (1). EDP Sciences: 189–201. arXiv: 0903.4854 . Bibcode:2009A&A...506..189R. doi: 10.1051/0004-6361/200811510 . ISSN   0004-6361.
  11. Nagy, Peter B.; Blodgett, Mark; Golis, Matthew (1994). "Weep hole inspection by circumferential creeping waves". NDT & E International. 27 (3). Elsevier BV: 131–142. doi:10.1016/0963-8695(94)90604-1. ISSN   0963-8695.
  12. Clorennec, D; Royer, D; Walaszek, H (2002). "Nondestructive evaluation of cylindrical parts using laser ultrasonics". Ultrasonics. 40 (1–8). Elsevier BV: 783–789. doi:10.1016/s0041-624x(02)00210-x. ISSN   0041-624X. PMID   12160045.
  13. Ishikawa, Satoru; Nakaso, Noritaka; Takeda, Nobuo; Mihara, Tsuyoshi; Tsukahara, Yusuke; Yamanaka, Kazushi (2003). "Surface acoustic waves on a sphere with divergent, focusing, and collimating beam shapes excited by an interdigital transducer". Applied Physics Letters. 83 (22). AIP Publishing: 4649–4651. Bibcode:2003ApPhL..83.4649I. doi:10.1063/1.1631061. ISSN   0003-6951.
  14. Tachizaki, Takehiro; Matsuda, Osamu; Maznev, Alex A.; Wright, Oliver B. (23 April 2010). "Acoustic whispering-gallery modes generated and dynamically imaged with ultrashort optical pulses". Physical Review B. 81 (16). American Physical Society (APS): 165434. Bibcode:2010PhRvB..81p5434T. doi:10.1103/physrevb.81.165434. hdl: 2115/43062 . ISSN   1098-0121.
  15. Ishikawa, Satoru; Cho, Hideo; Yamanaka, Kazushi; Nakaso, Noritaka; Tsukahara, Yusuke (30 May 2001). "Surface Acoustic Waves on a Sphere –Analysis of Propagation Using Laser Ultrasonics–". Japanese Journal of Applied Physics. 40 (Part 1, No. 5B). Japan Society of Applied Physics: 3623–3627. Bibcode:2001JaJAP..40.3623I. doi:10.1143/jjap.40.3623. ISSN   0021-4922. S2CID   121857533.
  16. "Delaying Trains of Short Light Pulses in WGM Resonators". Tech Briefs Media Group. 1 September 2018. Retrieved 2018-11-30.
  17. Mie, Gustav (1908). "Beiträge zur Optik trüber Medien, speziell kolloidaler Metallösungen". Annalen der Physik (in German). 330 (3). Wiley: 377–445. Bibcode:1908AnP...330..377M. doi: 10.1002/andp.19083300302 . ISSN   0003-3804.
  18. Debye, P. (1909). "Der Lichtdruck auf Kugeln von beliebigem Material". Annalen der Physik (in German). 335 (11). Wiley: 57–136. Bibcode:1909AnP...335...57D. doi:10.1002/andp.19093351103. hdl: 1908/3003 . ISSN   0003-3804.
  19. Oraevsky, Anatolii N (31 May 2002). "Whispering-gallery waves". Quantum Electronics. 32 (5). IOP Publishing: 377–400. doi:10.1070/qe2002v032n05abeh002205. ISSN   1063-7818. S2CID   250792191.
  20. Vahala, K. J. (2003). "Optical microcavities". Nature. 424 (6950): 839–846. Bibcode:2003Natur.424..839V. doi:10.1038/nature01939. PMID   12917698. S2CID   4349700.
  21. Chiasera, A.; Dumeige, Y.; Féron, P.; Ferrari, M.; Jestin, Y.; Nunzi Conti, G.; Pelli, S.; Soria, S.; Righini, G.C. (23 April 2010). "Spherical whispering-gallery-mode microresonators". Laser & Photonics Reviews. 4 (3). Wiley: 457–482. Bibcode:2010LPRv....4..457C. doi:10.1002/lpor.200910016. ISSN   1863-8880. S2CID   119484780.
  22. Miller, Johanna (1 March 2024). "Bubble lasers can be sturdy and sensitive". Physics Today. 77 (3). American Institute of Physics: 12–14. doi:10.1063/pt.xafv.lnix.
  23. Rakovich, Y.P.; Donegan, J.F. (2 June 2009). "Photonic atoms and molecules". Laser & Photonics Reviews. 4 (2). Wiley: 179–191. doi:10.1002/lpor.200910001. ISSN   1863-8880. S2CID   121561846.
  24. Kippenberg, T. J.; Vahala, K. J. (29 August 2008). "Cavity Optomechanics: Back-Action at the Mesoscale". Science. 321 (5893). American Association for the Advancement of Science (AAAS): 1172–1176. Bibcode:2008Sci...321.1172K. doi:10.1126/science.1156032. ISSN   0036-8075. PMID   18755966. S2CID   4620490.
  25. Del’Haye, P.; Schliesser, A.; Arcizet, O.; Wilken, T.; Holzwarth, R.; Kippenberg, T. J. (2007). "Optical frequency comb generation from a monolithic microresonator". Nature. 450 (7173). Springer Science and Business Media LLC: 1214–1217. arXiv: 0708.0611 . Bibcode:2007Natur.450.1214D. doi:10.1038/nature06401. ISSN   0028-0836. PMID   18097405. S2CID   4426096.
  26. Arnold, S.; Khoshsima, M.; Teraoka, I.; Holler, S.; Vollmer, F. (15 February 2003). "Shift of whispering-gallery modes in microspheres by protein adsorption". Optics Letters. 28 (4). The Optical Society: 272–4. Bibcode:2003OptL...28..272A. doi:10.1364/ol.28.000272. ISSN   0146-9592. PMID   12653369.
  27. Grudinin, Ivan S.; Ilchenko, Vladimir S.; Maleki, Lute (8 December 2006). "Ultrahigh optical Q factors of crystalline resonators in the linear regime". Physical Review A. 74 (6). American Physical Society (APS): 063806. Bibcode:2006PhRvA..74f3806G. doi:10.1103/physreva.74.063806. ISSN   1050-2947.
  28. Yamanaka, K.; Ishikawa, S.; Nakaso, N.; Takeda, N.; Sim, Dong Youn; et al. (2006). "Ultramultiple roundtrips of surface acoustic wave on sphere realizing innovation of gas sensors". IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control. 53 (4): 793–801. doi:10.1109/TUFFC.2006.1621507. PMID   16615584. S2CID   22051539.
  29. Pask, Colin (1 December 1977). "Generalized parameters for tunneling ray attenuation in optical fibers". Journal of the Optical Society of America. 68 (1). The Optical Society: 110. doi:10.1364/josa.68.000110. ISSN   0030-3941.
  30. Gmachl, C. (5 June 1998). "High-Power Directional Emission from Microlasers with Chaotic Resonators". Science. 280 (5369): 1556–1564. arXiv: cond-mat/9806183 . Bibcode:1998Sci...280.1556G. doi:10.1126/science.280.5369.1556. ISSN   0036-8075. PMID   9616111. S2CID   502055.
  31. Baryshnikov, Yuliy; Heider, Pascal; Parz, Wolfgang; Zharnitsky, Vadim (22 September 2004). "Whispering Gallery Modes Inside Asymmetric Resonant Cavities". Physical Review Letters. 93 (13). American Physical Society (APS): 133902. Bibcode:2004PhRvL..93m3902B. doi:10.1103/physrevlett.93.133902. ISSN   0031-9007. PMID   15524720.
  32. Tanaka, Akira; Asai, Takeshi; Toubaru, Kiyota; Takashima, Hideaki; Fujiwara, Masazumi; Okamoto, Ryo; Takeuchi, Shigeki (24 January 2011). "Phase shift spectra of a fiber–microsphere system at the single photon level". Optics Express. 19 (3). The Optical Society: 2278–85. arXiv: 1101.5198 . Bibcode:2011OExpr..19.2278T. doi:10.1364/oe.19.002278. ISSN   1094-4087. PMID   21369045. S2CID   31604481.
  33. Budden, K. G.; Martin, H. G. (6 February 1962). "The ionosphere as a whispering gallery". Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences. 265 (1323). The Royal Society: 554–569. Bibcode:1962RSPSA.265..554B. doi:10.1098/rspa.1962.0042. ISSN   2053-9169. S2CID   120311101.
  34. Stanwix, P. L.; et al. (2005). "Test of Lorentz Invariance in Electrodynamics Using Rotating Cryogenic Sapphire Microwave Oscillators". Physical Review Letters. 95 (4): 040404. arXiv: hep-ph/0506074 . Bibcode:2005PhRvL..95d0404S. doi:10.1103/PhysRevLett.95.040404. PMID   16090785. S2CID   14255475.
  35. Mendis, R.; Mittleman, M. (2010). "Whispering-gallery-mode terahertz pulse propagation on a curved metallic plate". Applied Physics Letters. 97 (3): 031106. Bibcode:2010ApPhL..97c1106M. doi:10.1063/1.3466909.
  36. Albert, F.; Braun, T.; Heindel, T.; Schneider, C.; Reitzenstein, S.; Höfling, S.; Worschech, L.; Forchel, A. (6 September 2010). "Whispering gallery mode lasing in electrically driven quantum dot micropillars". Applied Physics Letters. 97 (10). AIP Publishing: 101108. Bibcode:2010ApPhL..97j1108A. doi:10.1063/1.3488807. ISSN   0003-6951.
  37. Hyun, J. K.; Couillard, M.; Rajendran, P.; Liddell, C. M.; Muller, D. A. (15 December 2008). "Measuring far-ultraviolet whispering gallery modes with high energy electrons". Applied Physics Letters. 93 (24). AIP Publishing: 243106. Bibcode:2008ApPhL..93x3106H. doi:10.1063/1.3046731. ISSN   0003-6951.
  38. Liu, Chien; Golovchenko, Jene A. (4 August 1997). "Surface Trapped X Rays: Whispering-Gallery Modes atλ=0.7Å". Physical Review Letters. 79 (5). American Physical Society (APS): 788–791. Bibcode:1997PhRvL..79..788L. doi:10.1103/physrevlett.79.788. ISSN   0031-9007. S2CID   121253766.
  39. M.R. Foreman (2015). "Whispering gallery mode sensors". Advances in Optics and Photonics. 7 (2): 168–240. Bibcode:2015AdOP....7..168F. doi:10.1364/AOP.7.000168. PMC   4786191 . PMID   26973759.
  40. Y. Wang (2020). "Microfluidic whispering gallery mode optical sensors for biological applications". Laser & Photonics Reviews. 14 (12): 2000135–56. Bibcode:2020LPRv...1400135W. doi:10.1002/lpor.202000135. S2CID   228850737.
  41. T. Reynolds (2017). "Fluorescent and lasing whispering gallery mode microresonators for sensing applications". Laser & Photonics Reviews. 11 (2): 1600265–76. Bibcode:2017LPRv...1100265R. doi:10.1002/lpor.201600265. hdl: 2027.42/136528 . S2CID   125481589.
  42. A. Bozzola (2017). "Hybrid plasmonic–photonic whispering gallery mode resonators for sensing: a critical review". Analyst. 142 (6): 883–898. Bibcode:2017Ana...142..883B. doi: 10.1039/C6AN02693A . PMID   28225100.
  43. Nesvizhevsky, Valery V.; Voronin, Alexei Yu.; Cubitt, Robert; Protasov, Konstantin V. (13 December 2009). "Neutron whispering gallery". Nature Physics. 6 (2). Springer Science and Business Media LLC: 114–117. doi: 10.1038/nphys1478 . ISSN   1745-2473.
  44. Reecht, Gaël; Bulou, Hervé; Scheurer, Fabrice; Speisser, Virginie; Carrière, Bernard; Mathevet, Fabrice; Schull, Guillaume (29 January 2013). "Oligothiophene Nanorings as Electron Resonators for Whispering Gallery Modes". Physical Review Letters. 110 (5). American Physical Society (APS): 056802. arXiv: 1301.4860 . Bibcode:2013PhRvL.110e6802R. doi:10.1103/physrevlett.110.056802. ISSN   0031-9007. PMID   23414040. S2CID   40257448.
  45. Dragún, Olga; Überall, Herbert (1980). "Nuclear Rayleigh and whispering gallery waves excited in heavy ion collisions". Physics Letters B. 94 (1). Elsevier BV: 24–27. Bibcode:1980PhLB...94...24D. doi:10.1016/0370-2693(80)90816-3. ISSN   0370-2693.
  46. Arcos, E.; Báez, G.; Cuatláyol, P. A.; Prian, M. L. H.; Méndez-Sánchez, R. A.; Hernández-Saldaña, H. (1998). "Vibrating soap films: An analog for quantum chaos on billiards". American Journal of Physics. 66 (7). American Association of Physics Teachers (AAPT): 601–607. arXiv: chao-dyn/9903002 . Bibcode:1998AmJPh..66..601A. doi:10.1119/1.18913. ISSN   0002-9505. S2CID   52106857.
  47. Min, Bumki; Ostby, Eric; Sorger, Volker; Ulin-Avila, Erick; Yang, Lan; Zhang, Xiang; Vahala, Kerry (2009). "High-Q surface-plasmon-polariton whispering-gallery microcavity". Nature. 457 (7228). Springer Science and Business Media LLC: 455–458. Bibcode:2009Natur.457..455M. doi:10.1038/nature07627. ISSN   0028-0836. PMID   19158793. S2CID   4411541.
  48. Sun, Liaoxin; Chen, Zhanghai; Ren, Qijun; Yu, Ke; Bai, Lihui; Zhou, Weihang; Xiong, Hui; Zhu, Z. Q.; Shen, Xuechu (16 April 2008). "Direct Observation of Whispering Gallery Mode Polaritons and their Dispersion in a ZnO Tapered Microcavity". Physical Review Letters. 100 (15): 156403. arXiv: 0710.5334 . Bibcode:2008PhRvL.100o6403S. doi:10.1103/physrevlett.100.156403. ISSN   0031-9007. PMID   18518134. S2CID   28537857.
  49. Tomes, Matthew; Carmon, Tal (19 March 2009). "Photonic Micro-Electromechanical Systems Vibrating atX-band (11-GHz) Rates". Physical Review Letters. 102 (11). American Physical Society (APS): 113601. Bibcode:2009PhRvL.102k3601T. doi:10.1103/physrevlett.102.113601. ISSN   0031-9007. PMID   19392199.
  50. Kim, JunHwan; Kuzyk, Mark C.; Han, Kewen; Wang, Hailin; Bahl, Gaurav (26 January 2015). "Non-reciprocal Brillouin scattering induced transparency". Nature Physics. 11 (3). Springer Science and Business Media LLC: 275–280. arXiv: 1408.1739 . Bibcode:2015NatPh..11..275K. doi:10.1038/nphys3236. ISSN   1745-2473. S2CID   119173646.
  51. Bahl, Gaurav; Kim, Kyu Hyun; Lee, Wonsuk; Liu, Jing; Fan, Xudong; Carmon, Tal (7 June 2013). "Brillouin cavity optomechanics with microfluidic devices". Nature Communications. 4 (1). Springer Science and Business Media LLC: 1994. arXiv: 1302.1949 . Bibcode:2013NatCo...4.1994B. doi: 10.1038/ncomms2994 . ISSN   2041-1723. PMID   23744103.