89:
characteristics of the wave. Consequently, numerous potential applications are envisaged, including devices for integrated optics, chemical and biological surface sensing, etc. However, it is not easy to satisfy the necessary conditions for the DSW, and because of this the first proof-of-principle experimental observation of DSW was reported only 20 years after the original prediction.
331:
The extreme sensitivity of DSW to anisotropy, and thereby to stress, along with their low-loss (long-range) character render them particularly attractive for enabling high sensitivity tactile and ultrasonic sensing for next-generation high-speed transduction and read-out technologies. Moreover, the
92:
A large number of theoretical work appeared dealing with various aspects of this phenomenon, see the detailed review. In particular, DSW propagation at magnetic interfaces, in left-handed materials, in electro-optical, and chiral materials was studied. Resonant transmission due to DSW in structures
88:
In recent years, the significance and potential of the DSW have attracted the attention of many researchers: a change of the constitutive properties of one or both of the two partnering materials – due to, say, infiltration by any chemical or biological agent – could measurably change the
327:
of at least one of the constituent materials and the limited number of naturally available materials fulfilling this requirement. However, this is about to change in light of novel artificially engineered metamaterials and revolutionary material synthesis techniques.
762:
Nelatury, S. R., Polo jr., J. A., and
Lakhtakia, A. (2008). "Electrical Control of Surface-Wave Propagation at the Planar Interface of a Linear Electro-Optic Material and an Isotropic Dielectric Material".
227:
65:, and showed that under certain conditions waves localized at the interface should exist. Later, similar waves were predicted to exist at the interface between two identical uniaxial crystals with
695:
Crassovan, L. C., Takayama, D., Artigas, D., Johansen, S. K., Mihalache, D., and Torner, L. (2006). "Enhanced localization of
Dyakonov-like surface waves in left-handed materials".
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Takayama, O., Shkondin, E., Bogdanov A., Panah, M. E., Golenitskii, K., Dmitriev, P., Repän, T., Malureanu, R., Belov, P., Jensen, F., and
Lavrinenko, A. (2017).
518:
81:
of one of the materials forming the interface is negative, while the other one is positive (for example, this is the case for the air/metal interface below the
832:
Nelatury, S. R., Polo jr., J. A., and
Lakhtakia, A. (2008). "On widening the angular existence domain for Dyakonov surface waves using the Pockels effect".
133:
axis is parallel to the interface. For this configuration, the DSW can propagate along the interface within certain angular intervals with respect to the
85:). In contrast, the DSW can propagate when both materials are transparent; hence they are virtually lossless, which is their most fascinating property.
319:
A widespread experimental investigation of DSW material systems and evolution of related practical devices has been largely limited by the stringent
899:
Gao, Jun; Lakhtakia, Akhlesh; Lei, Mingkai (2009). "On
Dyakonov-Tamm waves localized to a central twist defect in a structurally chiral material".
1409:
Takayama, O.; Artigas, D., Torner, L. (2014). "Lossless directional guiding of light in dielectric nanosheets using
Dyakonov surface waves".
93:
using prisms was predicted, and combination and interaction between DSW and surface plasmons (Dyakonov plasmons) was studied and observed.
1239:
Takayama, O., Dmitriev, P., Shkondin, E., Yermakov, O., Panah, M., Golenitskii, K., Jensen, F., Bogdanov A., and
Lavrinenko, A. (2018).
1513:
179:
1303:
Takayama, O.; Crasovan, L. C., Johansen, S. K.; Mihalache, D, Artigas, D.; Torner, L. (2008). "Dyakonov
Surface Waves: A Review".
935:
419:
Averkiev, N. S. and
Dyakonov, M. I. (1990). "Electromagnetic waves localized at the interface of transparent anisotropic media".
372:
638:
Crassovan, L. C., Artigas, D., Mihalache, D., and Torner, L. (2005). "Optical
Dyakonov surface waves at magnetic interfaces".
101:
The simplest configuration considered in Ref. 1 consists of an interface between an isotropic material with permittivity
24:
74:
1240:
1518:
1352:
Takayama, O.; Bogdanov, A. A., Lavrinenko, A. V. (2017). "Photonic surface waves on metamaterial interfaces".
341:
1069:
Jacob, Z. and Narimanov, E. E. (2008). "Optical hyperspace for plasmons: Dyakonov states in metamaterials".
1184:
285:). However the physically more important group velocity interval is substantially larger (proportional to
1523:
1468:"Leaky Surface Plasmon Polariton Modes at an Interface Between Metal and Uniaxially Anisotropic Materials"
782:
589:
Takayama, O., Crassovan, L. C., Mihalache, D., and Torner, L. (2008). "Dyakonov Surface Waves: A Review".
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Takayama, O., Nikitin, A. Yu., Martin-Moreno, L., Mihalache, D., Torner, L., and Artigas, A. (2011).
908:
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is satisfied. Thus DSW are supported by interfaces with positive birefringent crystals only (
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Takayama, O., Artigas, D., and Torner, L. (2012). "Coupling plasmons and dyakonons".
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conditions necessary for successful DSW propagation, particularly the high degree of
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unique directionality of DSW can be used for the steering of optical signals.
320:
481:
920:
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Torner, L., Artigas, D., and Takayama, O. (2009). "Dyakonov Surface Waves".
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and even for the most strongly birefringent natural crystals is very narrow
54:
40:
28:
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of materials forming the interface. He considered the interface between an
35:
medium. They were theoretically predicted in 1988 by the Russian physicist
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963:
659:
709:
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282:
1185:"Midinfrared surface waves on a high aspect ratio nanotrench platform"
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863:
268:
1241:"Experimental observation of Dyakonov plasmons in the mid-infrared"
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846:
777:
517:
Takayama, O., Crassovan, L., Artigas D., and Torner, L. (2009).
251:) are different. The phase velocity interval is proportional to
47:
surface waves, the DSW's existence is due to the difference in
373:"New type of electromagnetic wave propagating at an interface"
233:
The angular intervals for the DSW phase and group velocities (
222:{\displaystyle \eta ={\frac {\epsilon _{e}}{\epsilon _{0}}}-1}
1008:
Guo, Yu.. Newman, W., Cortes, C. L. and Jacob, Z. (2012).
173:). The angular interval is defined by the parameter
69:. The previously known electromagnetic surface waves,
182:
1014:
Applications of Hyperbolic Metamaterial Substrates"
221:
27:that travel along the interface in between an
936:"Dyakonov surface wave resonant transmission"
8:
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901:Journal of the Optical Society of America B
107:and a uniaxial crystal with permittivities
1491:
1466:Liu, Hsuan-Hao; Chang, Hung-Chun (2013).
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834:Microwave and Optical Technology Letters
519:"Observation of Dyakonov Surface Waves"
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137:axis, provided that the condition of
77:, exist under the condition that the
7:
1354:Journal of Physics: Condensed Matter
14:
546:10.1103/PhysRevLett.102.043903
421:Optics and Spectroscopy (USSR)
371:Dyakonov, M. I. (April 1988).
1:
25:surface electromagnetic waves
1204:10.1021/acsphotonics.7b00924
1018:Advances in OptoElectronics
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1493:10.1109/JPHOT.2013.2288298
727:10.1103/PhysRevB.74.155120
129:respectively. The crystal
75:surface plasmon polaritons
1317:10.1080/02726340801921403
1268:10.1134/S1063782618040279
797:10.1080/02726340801921486
603:10.1080/02726340801921403
462:Optics and Photonics News
125:for the ordinary and the
1514:Condensed matter physics
1374:10.1088/1361-648X/aa8bdd
482:10.1364/OPN.20.12.000025
39:. Unlike other types of
921:10.1364/JOSAB.26.000B74
1472:IEEE Photonics Journal
223:
67:different orientations
17:Dyakonov surface waves
1431:10.1038/nnano.2014.90
1411:Nature Nanotechnology
291:). Calculations give
224:
1148:10.1364/OL.37.001983
964:10.1364/OE.19.006339
660:10.1364/OL.30.003075
180:
1484:2013IPhoJ...500806L
1423:2014NatNa...9..419T
1366:2017JPCM...29T3001T
1260:2018Semic..52..442T
1140:2012OptL...37.1983T
1083:2008ApPhL..93v1109J
1041:10.1155/2012/452502
955:2011OExpr..19.6339T
913:2009JOSAB..26B..74G
856:2008arXiv0804.4879N
719:2006PhRvB..74o5120C
652:2005OptL...30.3075C
538:2009PhRvL.102d3903T
522:(Free PDF download)
474:2009OptPN..20...25T
433:1990OptSp..68..653A
399:(Free PDF download)
392:1988JETP...67..714D
380:Soviet Physics JETP
342:Dyakonov–Voigt wave
127:extraordinary waves
97:Physical properties
61:and an anisotropic
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1198:(11): 2899–2907.
1091:10.1063/1.3037208
864:10.1002/mop.23698
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83:plasma frequency
71:surface plasmons
63:uniaxial crystal
37:Mikhail Dyakonov
31:and an uniaxial-
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1248:Semiconductors
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1134:(11): 1983–5.
1128:Optics Letters
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1077:(22): 221109.
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949:(7): 6339–47.
943:Optics Express
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771:(3): 162–174.
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403:. Retrieved
396:the original
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347:Surface wave
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315:Perspectives
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79:permittivity
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33:birefringent
20:
16:
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973:10261/47330
1508:Categories
468:(12): 25.
427:(5): 653.
405:2013-07-30
386:(4): 714.
358:References
352:Leaky mode
321:anisotropy
1325:121726611
1276:255238679
1212:126006666
1031:1211.0980
847:0804.4879
783:CiteSeerX
778:0711.1663
735:119439238
640:Opt. Lett
611:121726611
490:120465632
214:−
203:ϵ
193:ϵ
184:η
55:isotropic
29:isotropic
1439:24859812
1382:29053474
1156:22660095
1099:39395734
981:21451661
805:10301459
668:16315726
562:14540394
554:19257419
336:See also
50:symmetry
41:acoustic
1480:Bibcode
1419:Bibcode
1362:Bibcode
1256:Bibcode
1136:Bibcode
1079:Bibcode
1024:: 1–9.
951:Bibcode
909:Bibcode
872:6024041
852:Bibcode
715:Bibcode
648:Bibcode
534:Bibcode
470:Bibcode
429:Bibcode
388:Bibcode
283:calomel
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