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Surface plasmon polariton

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being chemically stable in natural environments making it well suited for plasmonic biosensors. However, an interband transition at ~470 nm greatly increases the losses in gold at wavelengths below 600 nm. Aluminum is the best plasmonic material in the ultraviolet regime (< 330 nm) and is also CMOS compatible along with copper.
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or grating to match the photon and SPP wave vectors (and thus match their momenta). A prism can be positioned against a thin metal film in the Kretschmann configuration or very close to a metal surface in the Otto configuration (Figure 1). A grating coupler matches the wave vectors by increasing the
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The ability to dynamically control the plasmonic properties of materials in these nano-devices is key to their development. A new approach that uses plasmon-plasmon interactions has been demonstrated recently. Here the bulk plasmon resonance is induced or suppressed to manipulate the propagation of
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The wavelength and intensity of the plasmon-related absorption and emission peaks are affected by molecular adsorption that can be used in molecular sensors. For example, a fully operational prototype device detecting casein in milk has been fabricated. The device is based on monitoring changes in
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Silver exhibits the lowest losses of current materials in both the visible, near-infrared (NIR) and telecom wavelengths. Gold and copper perform equally well in the visible and NIR with copper having a slight advantage at telecom wavelengths. Gold has the advantage over both silver and copper of
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Unfortunately, metals suffer from ohmic losses that can degrade the performance of plasmonic devices. The need for lower loss has fueled research aimed at developing new materials for plasmonics and optimizing the deposition conditions of existing materials. Both the loss and polarizability of a
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SPPs can be excited by both electrons and photons. Excitation by electrons is created by firing electrons into the bulk of a metal. As the electrons scatter, energy is transferred into the bulk plasma. The component of the scattering vector parallel to the surface results in the formation of a
5737: 4895: 3707:. The table below shows the quality factors and SPP propagation lengths for four common plasmonic metals; Al, Ag, Au and Cu deposited by thermal evaporation under optimized conditions. The quality factors and SPP propagation lengths were calculated using the optical data from the 3413: 2338: 3524:
In addition to building functional devices based on SPPs, it appears feasible to exploit the dispersion characteristics of SPPs traveling in confined metallo-dielectric spaces to create photonic materials with artificially tailored bulk optical characteristics, otherwise known as
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Current research is focused on the design, fabrication, and experimental characterization of novel components for measurement and communications based on nanoscale plasmonic effects. These devices include ultra-compact plasmonic interferometers for applications such as
5117: 4457: 2597:, the SPP has a shorter wavelength than free-space radiation such that the out-of-plane component of the SPP wavevector is purely imaginary and exhibits evanescent decay. The surface plasma frequency is the asymptote of this curve, and is given by 2215: 1304: 751:. Perpendicular to the interface, they have subwavelength-scale confinement. An SPP will propagate along the interface until its energy is lost either to absorption in the metal or scattering into other directions (such as into free space). 3521:, optical positioning and optical switching, as well as the individual building blocks (plasmon source, waveguide and detector) needed to integrate a high-bandwidth, infrared-frequency plasmonic communications link on a silicon chip. 3513:. The resulting enhanced sensitivity of light to external parameters (for example, an applied electric field or the dielectric constant of an adsorbed molecular layer) shows great promise for applications in sensing and switching. 6910:
Minh Hiep, Ha; Endo, Tatsuro; Kerman, Kagan; Chikae, Miyuki; Kim, Do-Kyun; Yamamura, Shohei; Takamura, Yuzuru; Tamiya, Eiichi (2007). "A localized surface plasmon resonance based immunosensor for the detection of casein in milk".
2102: 2432: 2515: 1888: 2767:< 0, a condition which is satisfied in metals. Electromagnetic waves passing through a metal experience damping due to Ohmic losses and electron-core interactions. These effects show up in as an imaginary component of the 2673: 2011: 4645: 6315: 6105: 5565: 3705: 5576: 1448: 1127: 4756: 843:. Moreover, simple isolated surface defects such as a groove, a slit or a corrugation on an otherwise planar surface provide a mechanism by which free-space radiation and SPs can exchange energy and hence couple. 4029:. When a photon is incident on a surface, the wave vector of the photon in the dielectric material is smaller than that of the SPP. In order for the photon to couple into a SPP, the wave vector must increase by 743:, guided along the interface in much the same way that light can be guided by an optical fiber. SPPs have a shorter wavelength than light in vacuum at the same frequency (photons). Hence, SPPs can have a higher 5034:
As stated earlier, SPPs are non-radiative. When a SPP travels along a rough surface, it usually becomes radiative due to scattering. The Surface Scattering Theory of light suggests that the scattered intensity
3150: 2226: 3614:, may be a metal or other material. It is more critical, as it tends to have a large effect on the wavelength, absorption length, and other properties of the SPP. Some plasmonic materials are discussed next. 2741: 789:
Figure 1: (a) Kretschmann and (b) Otto configuration of an Attenuated Total Reflection setup for coupling surface plasmons. In both cases, the surface plasmon propagates along the metal/dielectric interface
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at the metal/dielectric interface. If surface plasmons are excited in the Kretschmann geometry and the scattered light is observed in the plane of incidence (Fig. 4), then the dipole function becomes
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parallel wave vector component by an amount related to the grating period (Figure 2). This method, while less frequently utilized, is critical to the theoretical understanding of the effect of surface
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indicates the medium of propagation. SPPs are very sensitive to slight perturbations within the skin depth and because of this, SPPs are often used to probe inhomogeneities of a surface.
5318:{\displaystyle {\frac {dI}{d\Omega \ I_{0}}}={\frac {4{\sqrt {\varepsilon _{0}}}}{\cos {\theta _{0}}}}{\frac {\pi ^{4}}{\lambda ^{4}}}|t_{012}^{p}|^{2}\ |W|^{2}|s(k_{\text{surf}})|^{2}} 766:. It also enables the first steady-state micro-mechanical measurement of a fundamental property of light itself: the momentum of a photon in a dielectric medium. Other applications are 3471:
The E-field of an SPP at the silver-air interface, at a much lower frequency corresponding to a free-space wavelength of 10μm. At this frequency, the silver behaves approximately as a
3443:(E-field) of an SPP at the silver-air interface, at the frequency where the free-space wavelength is 370 nm. The animation shows how the E-field varies over an optical cycle. The 3283:
Likewise, the electric field falls off evanescently perpendicular to the metal surface. At low frequencies, the SPP penetration depth into the metal is commonly approximated using the
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Kretschmann, E. (April 1974). "Die Bestimmung der Oberflächenrauhigkeit dünner Schichten durch Messung der Winkelabhängigkeit der Streustrahlung von Oberflächenplasmaschwingungen".
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properties (substantially shrinking the wavelength of light and the speed of light pulses for example), as well as field enhancements suitable for enabling strong interactions with
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light. This approach has been shown to have a high potential for nanoscale light manipulation and the development of a fully CMOS- compatible electro-optical plasmonic modulator.
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The wave vector gives us insight into physically meaningful properties of the electromagnetic wave such as its spatial extent and coupling requirements for wave vector matching.
4252: 2567: 3586:, the second harmonic signal is proportional to the square of the electric field. The electric field is stronger at the interface because of the surface plasmon resulting in a 1677: 1915: 4948: 3830: 2113: 823:(see below). This momentum mismatch is the reason that a free-space photon from air cannot couple directly to an SPP. For the same reason, an SPP on a smooth metal surface 688: 4279: 1585: 1133: 5857: 827:
emit energy as a free-space photon into the dielectric (if the dielectric is uniform). This incompatibility is analogous to the lack of transmission that occurs during
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Bashevoy, M.V.; Jonsson, F.; Krasavin, A.V.; Zheludev, N.I.; Chen Y.; Stockman M.I. (2006). "Generation of traveling surface plasmon waves by free-electron impact".
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As an SPP propagates along the surface, it loses energy to the metal due to absorption. The intensity of the surface plasmon decays with the square of the
2365: 2443: 1806: 2603: 1932: 4559: 4306: 5376: 5732:{\displaystyle A(\theta ,|\varepsilon _{1}|)={\frac {|\varepsilon _{1}|+1}{|\varepsilon _{1}|-1}}{\frac {4}{1+\tan {\theta }/|\varepsilon _{1}|}}} 3572:, have been proposed as a means of overcoming the size limitations of photonic circuits for use in high performance data processing nano devices. 4890:{\displaystyle |s(k_{\text{surf}})|^{2}={\frac {1}{4\pi }}\sigma ^{2}\delta ^{2}\exp \left(-{\frac {\sigma ^{2}k_{\text{surf}}^{2}}{4}}\right)} 3550:(SPR). In SPR, the maximum excitation of surface plasmons are detected by monitoring the reflected power from a prism coupler as a function of 681: 7634: 3622:
For visible and near-infrared light, the only plasmonic materials are metals, due to their abundance of free electrons, which leads to a high
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formula. In the dielectric, the field will fall off far more slowly. The decay lengths in the metal and dielectric medium can be expressed as
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McPeak, Kevin M.; Jayanti, Sriharsha V.; Kress, Stephan J. P.; Meyer, Stefan; Iotti, Stelio; Rossinelli, Aurelio; Norris, David J. (2015).
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Wenshan Cai; Justin S. White & Mark L. Brongersma (2009). "Compact, High-Speed and Power-Efficient Electrooptic Plasmonic Modulators".
2537: 2333:{\displaystyle k_{x}={\frac {\omega }{c}}\left({\frac {\varepsilon _{1}\varepsilon _{2}}{\varepsilon _{1}+\varepsilon _{2}}}\right)^{1/2}.} 6531: 7430:
Kretschmann, E. (1972). "The angular dependence and the polarisation of light emitted by surface plasmons on metals due to roughness".
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For a photon to excite an SPP, both must have the same frequency and momentum. However, for a given frequency, a free-space photon has
6709: 6478: 6453: 3583: 3408:{\displaystyle z_{i}={\frac {\lambda }{2\pi }}\left({\frac {|\varepsilon _{1}'|+\varepsilon _{2}}{\varepsilon _{i}^{2}}}\right)^{1/2}} 4217:{\displaystyle k_{SPP}=k_{x,{\text{photon}}}\pm n\ k_{\text{grating}}={\frac {\omega }{c}}\sin {\theta _{0}}\pm n{\frac {2\pi }{a}},} 674: 661: 7465:
Arakawa, E. T.; Williams, M. W.; Hamm, R. N.; Ritchie, R. H. (29 October 1973). "Effect of Damping on Surface Plasmon Dispersion".
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becomes. Therefore, at infrared and longer wavelengths, various other plasmonic materials also exist besides metals. These include
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West, P.R.; Ishii, S.; Naik, G.V.; Emani, N.K.; Shalaev, V.M.; Boltasseva, A. (2010). "Searching for better plasmonic materials".
3666: 3610:, can be any transparent material such as air or (for visible light) glass. The negative-permittivity material, often called the 7106:
Blaber, M G; Arnold, M D; Ford, M J (2010). "A review of the optical properties of alloys and intermetallics for plasmonics".
436: 4032: 4010:). The resulting waves have the same optical properties as surface plasmon polaritons, but are called by a different term, 2833: 91: 3985: 611: 6203: 5989:
in metals. For lossy cases, the dispersion curve backbends after the reaching the surface plasmon frequency instead of
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In order to understand the effect of roughness on SPPs, it is beneficial to first understand how a SPP is coupled by a
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Zeng, Shuwen; Yu, Xia; Law, Wing-Cheung; Zhang, Yating; Hu, Rui; Dinh, Xuan-Quyen; Ho, Ho-Pui; Yong, Ken-Tye (2013).
5862: 3472: 728:-frequency. The term "surface plasmon polariton" explains that the wave involves both charge motion in the metal (" 616: 241: 5954: 5934: 3993: 3547: 828: 506: 181: 3497:
Nanofabricated systems that exploit SPPs demonstrate potential for designing and controlling the propagation of
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If the surface only has one Fourier component of roughness (i.e. the surface profile is sinusoidal), then the
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V. K. Valev (2012). "Characterization of Nanostructured Plasmonic Surfaces with Second Harmonic Generation".
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of a periodic grating provide additional momentum parallel to the supporting interface to match the terms.
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CMOS compatible electro-optic plasmonic modulators will be key components in chip-scale photonic circuits.
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Etchegoin, P. G.; Le Ru, E. C.; Meyer, M. (2006). "An analytic model for the optical properties of gold".
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Hendry, E.; Garcia-Vidal, F.; Martin-Moreno, L.; Rivas, J.; Bonn, M.; Hibbins, A.; Lockyear, M. (2008).
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called the "surface plasma frequency". Since the dispersion curve lies to the right of the light line,
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Barnes, William L.; Dereux, Alain; Ebbesen, Thomas W. (2003). "Surface plasmon subwavelength optics".
3720: 3716: 3712: 3708: 2210:{\displaystyle k_{x}^{2}+k_{zn}^{2}=\varepsilon _{n}\left({\frac {\omega }{c}}\right)^{2}\qquad n=1,2} 1893: 7719: 7649: 7594: 7579: 7550: 7476: 7439: 7401: 7354: 7297: 7125: 7053: 7041: 6999: 6920: 6841: 6737: 6664: 6605: 6405:"Size dependence of Au NP-enhanced surface plasmon resonance based on differential phase measurement" 6361: 6228: 6166: 4926: 4297: 804:
Figure 2: Grating Coupler for Surface Plasmons. The wave vector is increased by the spatial frequency
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material and a negative-permittivity material. The positive-permittivity material, often called the
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Marques Lameirinhas, Ricardo A.; N. Torres, João Paulo; Baptista, António; M. Martins, Maria João.
6015:"Nanomaterials enhanced surface plasmon resonance for biological and chemical sensing applications" 5929: 4023: 4004: 3536: 2768: 2570: 2356: 1299:{\displaystyle E_{z,n}(x,y,z,t)=\pm E_{0}{\frac {k_{x}}{k_{z,n}}}e^{ik_{x}x+ik_{z,n}|z|-i\omega t}} 820: 451: 261: 111: 7580:"Optical Control over Surface-Plasmon-Polariton-Assisted THz Transmission through a Slit Aperture" 3222:. The propagation length is defined as the distance for the SPP intensity to decay by a factor of 7735: 7709: 7673: 7566: 7270: 7157: 7115: 7085: 7023: 6989: 6814: 6771: 6631: 6385: 6351: 6260: 6218: 6202:
Huidobro, Paloma A.; Nesterov, Maxim L.; Martín-Moreno, Luis; García-Vidal, Francisco J. (2010).
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Akimov, Yu A; Chu, H S (2012). "Plasmon–plasmon interaction: Controlling light at nanoscale".
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Solving these two equations, the dispersion relation for a wave propagating on the surface is
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Nevertheless, coupling of photons into SPPs can be achieved using a coupling medium such as a
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Surface Plasmon Resonance Based Sensors. Springer Series on Chemical Sensors and Biosensors,
5793: 5765: 5331: 4729: 4653: 3633: 2810:″ are the real and imaginary parts of the dielectric function, respectively. Generally | 1772: 1739: 944: 7727: 7657: 7610: 7602: 7558: 7484: 7447: 7409: 7362: 7305: 7246: 7209: 7193: 7133: 7061: 7007: 6928: 6884: 6849: 6798: 6753: 6745: 6672: 6613: 6506: 6416: 6369: 6273: 6244: 6236: 6174: 6037: 6029: 4671: 4465: 3981: 3623: 3587: 2582: 1489: 1463: 910: 884: 759: 725: 266: 231: 226: 186: 156: 126: 86: 46: 5745: 5087: 4697: 4500: 1712: 1598: 6700:
Vo-Dinh, Tuan (2017). "Chapter 13 - Biomolecule Sensing Using Surface Plasmon Resonance".
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Nanotechnology in Biology and Medicine Methods, Devices, and Applications, Second Edition
6651:"Controlling rejections of spoof surface plasmon polaritons using metamaterial particles" 858: 7723: 7653: 7598: 7554: 7480: 7443: 7405: 7358: 7301: 7129: 7057: 7003: 6924: 6845: 6741: 6668: 6609: 6365: 6232: 6170: 6139:. U.S. Department of Energy National Laboratory Operated by the University of California 5038: 2343: 7756: 7345: 7214: 7181: 6725: 6655: 6526: 5939: 5014: 4956: 4903: 4677: 4532: 3459:
across horizontally; the SPP wavelength is much smaller than the free-space wavelength.
3440: 3164: 2097:{\displaystyle {\frac {k_{z1}}{\varepsilon _{1}}}+{\frac {k_{z2}}{\varepsilon _{2}}}=0} 1926: 938: 934: 835: 648: 626: 606: 601: 556: 476: 411: 309: 196: 41: 30: 6085: 3590:. This larger signal is often exploited to produce a stronger second harmonic signal. 2827:″ so the wavenumber can be expressed in terms of its real and imaginary components as 7779: 7731: 7570: 7451: 7413: 7089: 6437: 6404: 5982: 5790:-plane. Two important consequences come out of these equations. The first is that if 4296:
of many gratings of different periodicities. Kretschmann proposed that a statistical
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Some materials have negative permittivity at certain infrared wavelengths related to
3989: 3559: 2427:{\displaystyle \varepsilon (\omega )=1-{\frac {\omega _{\rm {P}}^{2}}{\omega ^{2}}},} 531: 337: 318: 300: 201: 121: 7739: 7274: 7161: 7027: 6635: 7606: 6818: 6775: 6389: 6320: 6292: 6264: 5959: 3476: 3444: 2510:{\displaystyle \omega _{\rm {P}}={\sqrt {\frac {ne^{2}}{{\varepsilon _{0}}m^{*}}}}} 1918: 1883:{\displaystyle {\frac {H_{0}}{E_{0}}}=-{\frac {\varepsilon _{1}\omega }{k_{z,1}c}}} 1693:; it is a complex vector, and in the case of a lossless SPP, it turns out that the 740: 551: 541: 511: 471: 466: 446: 291: 271: 131: 7677: 7237:
Homola, Jir (2003). "Present and future of surface plasmon resonance biosensors".
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is the area of integration. Assuming that the statistical correlation function is
2668:{\displaystyle \omega _{\rm {SP}}=\omega _{\rm {P}}/{\sqrt {1+\varepsilon _{2}}}.} 2006:{\displaystyle {\frac {H_{0}}{E_{0}}}={\frac {\varepsilon _{2}\omega }{k_{z,2}c}}} 6947: 6728:(2006). "Plasmonics: Merging Photonics and Electronics at Nanoscale Dimensions". 4640:{\displaystyle G(x,y)=\delta ^{2}\exp \left(-{\frac {r^{2}}{\sigma ^{2}}}\right)} 3626:. (Materials have negative real permittivity only below their plasma frequency.) 7488: 6587: 6014: 5986: 5059: 3546:
The excitation of SPPs is frequently used in an experimental technique known as
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S.Zeng; Baillargeat, Dominique; Ho, Ho-Pui; Yong, Ken-Tye; et al. (2014).
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Surface plasmon polaritons can only exist at the interface between a positive-
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infrared range. At longer wavelengths, semiconductors may also be plasmonic.
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in matter. In particular, SPPs can be used to channel light efficiently into
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Ebbesen, T. W.; Lezec, H. J.; Ghaemi, H. F.; Thio, T.; Wolff, P. A. (1998).
7065: 6749: 6618: 6591: 5990: 5944: 4090: 3532: 3502: 733: 536: 486: 359: 206: 106: 7669: 7624: 7376: 7341:"Plasmon polaritons in the near infrared on fluorine doped tin oxide films" 7325: 7266: 7223: 7153: 7081: 7011: 6896: 6861: 6810: 6767: 6686: 6627: 6381: 6256: 6248: 6186: 6049: 3980:
The fewer electrons a material has, the lower (i.e. longer-wavelength) its
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Figure 3: Lossless dispersion curve for surface plasmon polaritons. At low
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Pitarke, J M; Silkin, V M; Chulkov, E V; Echenique, P M (2007).
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NIST researchers, Nanofabrication Research Group (2010-02-11).
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NIST researchers, Nanofabrication Research Group (2009-08-20).
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Barnes, William L.; Dereux, Alain; Ebbesen, Thomas W. (2003).
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becomes continuous and the range of coupling angles broadens.
81: 7044:; Atwater, H. A. (2011). "Low-Loss Plasmonic Metamaterials". 6442:
Surface Plasmons on Smooth and Rough Surfaces and on Gratings
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increases, the dispersion relation bends over and reaches an
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is the height above the mean surface height at the position
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material affect its optical performance. The quality factor
7695:"Theory of surface plasmons and surface-plasmon polaritons" 7339:
Dominici, L; Michelotti, F; Brown, TM; et al. (2009).
3700:{\displaystyle {\frac {\varepsilon '^{2}}{\varepsilon ''}}} 6649:
Pan, Bai Cao; Liao, Zhen; Zhao, Jie; Cui, Tie Jun (2014).
6590:; Martín-Moreno, L.; Garcia-Vidal, F. J. (6 August 2004). 5981:
This lossless dispersion relation neglects the effects of
7182:"Plasmonic Films Can Easily Be Better: Rules and Recipes" 732:") and electromagnetic waves in the air or dielectric (" 1701:
components are imaginary—the wave oscillates along the
3177: 6592:"Mimicking Surface Plasmons with Structured Surfaces" 5865: 5822: 5796: 5768: 5748: 5579: 5379: 5334: 5120: 5090: 5067: 5041: 5017: 4979: 4959: 4929: 4906: 4759: 4732: 4700: 4680: 4656: 4562: 4535: 4503: 4468: 4309: 4260: 4233: 4102: 4082:{\displaystyle \Delta k=k_{SP}-k_{x,{\text{photon}}}} 4035: 3793: 3740: 3669: 3636: 3594:
plasmon-related absorption of light by a gold layer.
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on condition that the following equations also hold:
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Introduction to Surface and Superlattice Excitations
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momentum than an SPP because the two have different
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Electromagnetic waves that travel along an interface
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Free PDF download for these peer reviewed articles.
3145:{\displaystyle k_{x}=k_{x}'+ik_{x}''=\left+i\left.} 770:data storage, light generation, and bio-photonics. 6291:NIST researchers, Nanofabrication Research Group. 5907: 5851: 5808: 5774: 5754: 5731: 5559: 5357: 5317: 5103: 5076: 5050: 5023: 5003: 4965: 4950:which help couple photons into a surface plasmon. 4942: 4912: 4889: 4738: 4718: 4686: 4662: 4639: 4541: 4521: 4489: 4451: 4281:is the angle of incidence of the incoming photon, 4273: 4246: 4216: 4081: 3824: 3778: 3699: 3655: 3407: 3272: 3214: 3144: 2771:. The dielectric function of a metal is expressed 2735: 2667: 2561: 2509: 2426: 2332: 2209: 2096: 2017:A wave of this form satisfies Maxwell's equations 2005: 1909: 1882: 1794: 1761: 1728: 1671: 1614: 1579: 1537: 1504: 1478: 1442: 1298: 1121: 971: 925: 899: 873: 3539:frequencies by metamaterials; these are known as 3505:scale volumes, leading to direct modification of 6975: 6973: 6971: 6969: 6286: 6284: 6063: 6061: 6059: 7425: 7423: 5908:{\displaystyle {\frac {dI}{d\Omega \ I_{0}}}=0} 3487:. The picture is 6 μm across horizontally. 2437:where the bulk plasma frequency in SI units is 7770:Submitted as coursework for AP272. Winter 2007 6704:. United States: CRC Press. pp. 259–288. 6327:National Institute of Standards and Technology 6298:. National Institute of Science and Technology 6117:National Institute of Standards and Technology 6088:. National Institute of Science and Technology 6072:. National Institute of Science and Technology 2678:In the case of air, this result simplifies to 1929:. As discussed below, this can also be written 5977: 5975: 3988:, which have typical plasma frequency in the 3171:, the intensity has decreased by a factor of 1705:direction and exponentially decays along the 851:The properties of an SPP can be derived from 682: 8: 6913:Science and Technology of Advanced Materials 3209: 3184: 1679:) are zero. In other words, SPPs are always 6070:"Three-Dimensional Plasmonic Metamaterials" 1736:is always the same for both materials, but 1460:indicates the material (1 for the metal at 720:or metal–air interface, practically in the 6112:Three-Dimensional Plasmonic Metamaterials 3531:. Artificial SPP modes can be realized in 3226:. This condition is satisfied at a length 1595:-components of the electric field vector, 689: 675: 29: 18: 7713: 7614: 7504:Plasmonics: Fundamentals and Applications 7366: 7213: 7119: 6993: 6757: 6676: 6617: 6554: 6552: 6510: 6432: 6430: 6355: 6222: 5890: 5866: 5864: 5837: 5832: 5823: 5821: 5795: 5767: 5747: 5721: 5715: 5706: 5701: 5696: 5678: 5664: 5658: 5649: 5636: 5630: 5621: 5618: 5607: 5601: 5592: 5578: 5551: 5542: 5523: 5519: 5510: 5504: 5495: 5490: 5478: 5454: 5445: 5430: 5424: 5415: 5394: 5389: 5380: 5378: 5349: 5344: 5335: 5333: 5309: 5304: 5294: 5279: 5273: 5268: 5259: 5250: 5245: 5238: 5233: 5224: 5216: 5206: 5200: 5190: 5185: 5169: 5163: 5157: 5145: 5121: 5119: 5095: 5089: 5066: 5040: 5016: 4986: 4978: 4958: 4934: 4928: 4905: 4870: 4865: 4855: 4848: 4828: 4818: 4799: 4790: 4785: 4775: 4760: 4758: 4731: 4699: 4679: 4655: 4624: 4614: 4608: 4588: 4561: 4534: 4502: 4467: 4434: 4422: 4345: 4331: 4308: 4265: 4259: 4238: 4232: 4196: 4183: 4178: 4162: 4153: 4133: 4126: 4107: 4101: 4072: 4065: 4049: 4034: 3798: 3792: 3767: 3745: 3739: 3680: 3670: 3668: 3641: 3635: 3568:-based circuits, including both SPPs and 3395: 3391: 3379: 3374: 3363: 3351: 3342: 3333: 3330: 3310: 3301: 3295: 3255: 3242: 3234: 3197: 3176: 3125: 3112: 3092: 3086: 3076: 3072: 3059: 3043: 3031: 3018: 3011: 2996: 2970: 2966: 2953: 2937: 2925: 2912: 2905: 2890: 2873: 2854: 2841: 2835: 2723: 2718: 2711: 2710: 2693: 2692: 2686: 2654: 2642: 2637: 2630: 2629: 2612: 2611: 2605: 2552: 2547: 2545: 2497: 2486: 2481: 2473: 2462: 2452: 2451: 2445: 2413: 2403: 2397: 2396: 2390: 2367: 2317: 2313: 2300: 2287: 2275: 2265: 2258: 2243: 2234: 2228: 2185: 2171: 2160: 2147: 2139: 2126: 2121: 2115: 2080: 2067: 2061: 2050: 2037: 2031: 2029: 1985: 1970: 1963: 1952: 1942: 1936: 1934: 1901: 1895: 1862: 1847: 1840: 1826: 1816: 1810: 1808: 1780: 1774: 1747: 1741: 1720: 1714: 1663: 1650: 1637: 1631: 1606: 1600: 1571: 1558: 1552: 1545:is + for the metal, − for the dielectric. 1530: 1491: 1465: 1421: 1413: 1401: 1382: 1374: 1364: 1318: 1312: 1277: 1269: 1257: 1238: 1230: 1212: 1202: 1196: 1190: 1141: 1135: 1100: 1092: 1080: 1061: 1053: 1043: 997: 991: 946: 912: 886: 860: 6473:. New York: Cambridge University Press. 4292:Rough surfaces can be thought of as the 3725: 3273:{\displaystyle L={\frac {1}{2k_{x}''}}.} 2577:, the SPP behaves like a photon, but as 2573:relation is plotted in Figure 3. At low 6492: 6490: 6005: 5971: 5365:is the radiation pattern from a single 3677: 3429: 2569:is the permittivity of free-space. The 21: 7635:"Surface plasmon subwavelength optics" 7239:Analytical and Bioanalytical Chemistry 6204:"Transformation Optics for Plasmonics" 3779:{\displaystyle Q_{SPP}(\times 10^{3})} 2357:free electron model of an electron gas 7: 7108:Journal of Physics: Condensed Matter 6444:. Springer Tracts in Modern Physics 6274:Transformation Optics for Plasmonics 5004:{\displaystyle k={\frac {2\pi }{a}}} 4746:is the correlation length, then the 6532:Introduction to Solid State Physics 4920:is a measure of the amount of each 4254:is the wave vector of the grating, 5880: 5135: 5071: 4247:{\displaystyle k_{\text{grating}}} 4036: 3584:surface second harmonic generation 2760:> 0, then it must be true that 2712: 2697: 2694: 2631: 2616: 2613: 2562:{\displaystyle {\varepsilon _{0}}} 2453: 2398: 14: 6409:Sensors and Actuators B: Chemical 3159:Propagation length and skin depth 1672:{\displaystyle E_{y},H_{x},H_{z}} 7755:White, Justin (March 19, 2007). 6314: This article incorporates 6309: 6104: This article incorporates 6099: 4003:rather than plasmons (so-called 3464: 3432: 1910:{\displaystyle \varepsilon _{1}} 797: 782: 656: 655: 642: 7290:The Journal of Chemical Physics 4973:is discrete and exists only at 4943:{\displaystyle k_{\text{surf}}} 4750:of the correlation function is 4694:is the distance from the point 4300:be defined for a rough surface 4026: 3447:of silver at this frequency is 3215:{\textstyle \exp\{-2k_{x}''x\}} 2191: 1921:of material 1 (the metal), and 7702:Reports on Progress in Physics 7607:10.1103/PhysRevLett.100.123901 7138:10.1088/0953-8984/22/14/143201 6949:Optical Waves in Layered Media 6803:10.1088/0957-4484/23/44/444004 5833: 5824: 5762:is the polarization angle and 5722: 5707: 5665: 5650: 5637: 5622: 5612: 5608: 5593: 5583: 5548: 5516: 5511: 5496: 5465: 5462: 5435: 5431: 5416: 5406: 5390: 5381: 5345: 5336: 5305: 5300: 5287: 5280: 5269: 5260: 5246: 5225: 4786: 4781: 4768: 4761: 4713: 4701: 4578: 4566: 4516: 4504: 4484: 4472: 4419: 4385: 4376: 4354: 4325: 4313: 3825:{\displaystyle L_{SPP}(\mu m)} 3819: 3810: 3773: 3757: 3352: 3334: 3122: 3105: 2378: 2372: 1422: 1414: 1354: 1330: 1278: 1270: 1177: 1153: 1101: 1093: 1033: 1009: 966: 948: 847:Fields and dispersion relation 1: 6982:Laser & Photonics Reviews 6448:. New York: Springer-Verlag. 3986:transparent conducting oxides 3890:Near-Infrared (1000 nm) 3507:resonate frequency dispersion 7757:"Surface Plasmon Polaritons" 7452:10.1016/0030-4018(72)90026-0 7414:10.1016/0030-4018(74)90362-9 3570:localized plasmon resonances 1769:is generally different from 1697:components are real and the 754:Application of SPPs enables 7489:10.1103/PhysRevLett.31.1127 6566:. Berlin: Springer-Verlag. 6469:Cottam, Michael G. (1989). 6132:Yarris, Lynn (2009-08-20). 4285:is the grating period, and 4274:{\displaystyle \theta _{0}} 1580:{\displaystyle E_{x},E_{z}} 1486:or 2 for the dielectric at 812:surface plasmon polariton. 7817: 7732:10.1088/0034-4885/70/1/R01 6946:Pochi Yeh (3 March 2005). 6933:10.1016/j.stam.2006.12.010 6512:10.1109/JPHOT.2022.3181967 3836:Ultraviolet (280 nm) 3475:, and the SPP is called a 3473:perfect electric conductor 941:as a function of position 702:Surface plasmon polaritons 242:Spin gapless semiconductor 7502:Maier, Stefan A. (2007). 7251:10.1007/s00216-003-2101-0 6421:10.1016/j.snb.2012.09.073 5991:asymptotically increasing 5955:Surface plasmon resonance 5935:Localized surface plasmon 5852:{\displaystyle |W|^{2}=0} 4012:surface phonon polaritons 3588:non-linear optical effect 3548:surface plasmon resonance 3493:Experimental applications 2524:is the electron density, 881:plane, with the metal at 829:total internal reflection 182:Electronic band structure 6022:Chemical Society Reviews 5859:and the scattered light 5077:{\displaystyle d\Omega } 3663:for a SPP is defined as 1927:speed of light in vacuum 1681:TM (transverse magnetic) 92:Bose–Einstein condensate 23:Condensed matter physics 7587:Physical Review Letters 7468:Physical Review Letters 7066:10.1126/science.1198258 6750:10.1126/science.1114849 6619:10.1126/science.1098999 5816:(s-polarization), then 5809:{\displaystyle \psi =0} 5775:{\displaystyle \theta } 5358:{\displaystyle |W|^{2}} 5084:per incident intensity 4739:{\displaystyle \sigma } 4663:{\displaystyle \delta } 3930:Telecom (1550 nm) 3656:{\displaystyle Q_{SPP}} 3477:Sommerfeld–Zenneck wave 1795:{\displaystyle k_{z,2}} 1762:{\displaystyle k_{z,1}} 972:{\displaystyle (x,y,z)} 7012:10.1002/lpor.200900055 6503:IEEE Photonics Journal 6316:public domain material 6106:public domain material 5925:Dyakonov surface waves 5909: 5853: 5810: 5782:is the angle from the 5776: 5756: 5733: 5561: 5359: 5319: 5105: 5078: 5052: 5025: 5005: 4967: 4944: 4914: 4891: 4740: 4720: 4688: 4664: 4641: 4543: 4523: 4491: 4490:{\displaystyle z(x,y)} 4453: 4275: 4248: 4218: 4083: 3850:Visible (650 nm) 3826: 3780: 3701: 3657: 3541:spoof surface plasmons 3409: 3274: 3216: 3146: 2737: 2669: 2563: 2511: 2428: 2352: 2334: 2211: 2098: 2007: 1911: 1884: 1796: 1763: 1730: 1673: 1616: 1581: 1539: 1506: 1505:{\displaystyle z>0} 1480: 1479:{\displaystyle z<0} 1444: 1300: 1123: 973: 927: 926:{\displaystyle z>0} 901: 900:{\displaystyle z<0} 875: 7766:. Physics department. 7432:Optics Communications 7393:Optics Communications 6559:Homola, Jiří (2006). 6272:PDF from arxiv.org – 6137:(Online news release) 5985:factors, such as the 5910: 5854: 5811: 5777: 5757: 5755:{\displaystyle \psi } 5734: 5562: 5360: 5320: 5106: 5104:{\displaystyle I_{0}} 5079: 5053: 5026: 5006: 4968: 4945: 4915: 4892: 4741: 4721: 4719:{\displaystyle (x,y)} 4689: 4665: 4642: 4544: 4524: 4522:{\displaystyle (x,y)} 4492: 4454: 4276: 4249: 4219: 4084: 3827: 3781: 3702: 3658: 3410: 3275: 3217: 3147: 2738: 2670: 2564: 2512: 2429: 2346: 2335: 2212: 2099: 2008: 1912: 1885: 1797: 1764: 1731: 1729:{\displaystyle k_{x}} 1674: 1617: 1615:{\displaystyle H_{y}} 1582: 1540: 1507: 1481: 1445: 1301: 1124: 974: 928: 902: 876: 749:local field intensity 710:electromagnetic waves 237:Topological insulator 7368:10.1364/OE.17.010155 6678:10.1364/OE.22.013940 5863: 5820: 5794: 5766: 5746: 5577: 5377: 5332: 5118: 5088: 5065: 5039: 5015: 4977: 4957: 4927: 4904: 4757: 4730: 4698: 4678: 4654: 4560: 4533: 4501: 4466: 4307: 4298:correlation function 4258: 4231: 4100: 4033: 4018:Effects of roughness 3791: 3738: 3667: 3634: 3294: 3233: 3175: 2834: 2685: 2604: 2544: 2540:of the electron and 2444: 2366: 2227: 2114: 2028: 1933: 1894: 1807: 1773: 1740: 1713: 1630: 1599: 1551: 1538:{\displaystyle \pm } 1529: 1490: 1464: 1311: 1134: 990: 945: 911: 885: 859: 821:dispersion relations 756:subwavelength optics 712:that travel along a 255:Electronic phenomena 102:Fermionic condensate 7764:Stanford University 7724:2007RPPh...70....1P 7662:10.1038/nature01937 7654:2003Natur.424..824B 7599:2008PhRvL.100l3901H 7555:1998Natur.391..667E 7508:Springer Publishing 7481:1973PhRvL..31.1127A 7444:1972OptCo...5..331K 7406:1974OptCo..10..353K 7359:2009OExpr..1710155D 7302:2006JChPh.125p4705E 7130:2010JPCM...22n3201B 7058:2011Sci...331..290B 7004:2010LPRv....4..795W 6925:2007STAdM...8..331M 6883:(44): 15454–15471. 6846:2009NanoL...9.4403C 6742:2006Sci...311..189O 6669:2014OExpr..2213940P 6663:(11): 13940–13950. 6610:2004Sci...305..847P 6366:2006NanoL...6.1113B 6233:2010NanoL..10.1985H 6179:10.1038/nature01937 6171:2003Natur.424..824B 5930:Graphene plasmonics 5243: 4875: 3608:dielectric material 3511:nonlinear materials 3384: 3350: 3263: 3205: 3167:, so at a distance 3120: 3100: 3051: 3026: 2945: 2920: 2881: 2862: 2769:dielectric function 2408: 2152: 2131: 874:{\displaystyle z=0} 853:Maxwell's equations 739:They are a type of 262:Quantum Hall effect 7744:Free PDF download. 7689:Free PDF download. 7629:Free PDF download. 6134:"GRIN Plasmonics…" 6034:10.1039/C3CS60479A 5905: 5849: 5806: 5772: 5752: 5729: 5557: 5355: 5315: 5229: 5101: 5074: 5051:{\displaystyle dI} 5048: 5021: 5001: 4963: 4940: 4910: 4887: 4861: 4736: 4716: 4684: 4660: 4637: 4539: 4519: 4487: 4449: 4271: 4244: 4214: 4079: 3822: 3776: 3729:Wavelength Regime 3697: 3653: 3612:plasmonic material 3405: 3370: 3338: 3270: 3251: 3212: 3193: 3142: 3108: 3088: 3039: 3014: 2933: 2908: 2869: 2850: 2746:If we assume that 2733: 2665: 2559: 2507: 2424: 2392: 2353: 2330: 2207: 2135: 2117: 2094: 2003: 1907: 1880: 1792: 1759: 1726: 1669: 1612: 1577: 1535: 1502: 1476: 1440: 1296: 1119: 969: 923: 907:and dielectric at 897: 871: 758:in microscopy and 649:Physics portal 7517:978-0-387-33150-8 7475:(18): 1127–1129. 7310:10.1063/1.2360270 7198:10.1021/ph5004237 7052:(6015): 290–291. 6959:978-0-471-73192-4 6889:10.1021/la302485c 6854:10.1021/nl902701b 6604:(5685): 847–848. 6573:978-3-540-33918-2 6542:978-0-471-41526-8 6374:10.1021/nl060941v 6241:10.1021/nl100800c 6028:(10): 3426–3452. 5897: 5885: 5727: 5676: 5461: 5440: 5297: 5258: 5222: 5198: 5175: 5152: 5140: 5024:{\displaystyle s} 4999: 4966:{\displaystyle s} 4937: 4922:spatial frequency 4913:{\displaystyle s} 4880: 4868: 4812: 4778: 4748:Fourier transform 4687:{\displaystyle r} 4630: 4542:{\displaystyle A} 4381: 4339: 4241: 4209: 4170: 4156: 4148: 4136: 4075: 3969: 3968: 3695: 3455:. The picture is 3385: 3323: 3265: 3132: 3066: 3004: 2960: 2898: 2728: 2660: 2532:of the electron, 2505: 2504: 2419: 2307: 2251: 2179: 2086: 2056: 2001: 1958: 1878: 1832: 1520:angular frequency 1224: 764:diffraction limit 699: 698: 407:Granular material 175:Electronic phases 7808: 7767: 7761: 7743: 7717: 7715:cond-mat/0611257 7699: 7688: 7686: 7680:. Archived from 7648:(6950): 824–30. 7639: 7628: 7618: 7584: 7574: 7540: 7522: 7521: 7499: 7493: 7492: 7462: 7456: 7455: 7427: 7418: 7417: 7387: 7381: 7380: 7370: 7353:(12): 10155–67. 7336: 7330: 7329: 7285: 7279: 7278: 7234: 7228: 7227: 7217: 7177: 7166: 7165: 7123: 7103: 7094: 7093: 7038: 7032: 7031: 6997: 6977: 6964: 6963: 6943: 6937: 6936: 6907: 6901: 6900: 6872: 6866: 6865: 6829: 6823: 6822: 6786: 6780: 6779: 6761: 6736:(5758): 189–93. 6722: 6716: 6715: 6697: 6691: 6690: 6680: 6646: 6640: 6639: 6621: 6584: 6578: 6577: 6556: 6547: 6546: 6523: 6517: 6516: 6514: 6494: 6485: 6484: 6466: 6460: 6459: 6434: 6425: 6424: 6400: 6394: 6393: 6359: 6339: 6333: 6330: 6313: 6312: 6306: 6304: 6303: 6297: 6293:"Nanoplasmonics" 6288: 6279: 6268: 6226: 6208: 6198: 6165:(6950): 824–30. 6154: 6148: 6147: 6145: 6144: 6138: 6129: 6123: 6120: 6103: 6102: 6096: 6094: 6093: 6080: 6078: 6077: 6065: 6054: 6053: 6019: 6010: 5994: 5987:intrinsic losses 5979: 5914: 5912: 5911: 5906: 5898: 5896: 5895: 5894: 5883: 5875: 5867: 5858: 5856: 5855: 5850: 5842: 5841: 5836: 5827: 5815: 5813: 5812: 5807: 5781: 5779: 5778: 5773: 5761: 5759: 5758: 5753: 5738: 5736: 5735: 5730: 5728: 5726: 5725: 5720: 5719: 5710: 5705: 5700: 5679: 5677: 5675: 5668: 5663: 5662: 5653: 5647: 5640: 5635: 5634: 5625: 5619: 5611: 5606: 5605: 5596: 5566: 5564: 5563: 5558: 5556: 5555: 5546: 5532: 5531: 5527: 5514: 5509: 5508: 5499: 5494: 5483: 5482: 5459: 5458: 5450: 5449: 5438: 5434: 5429: 5428: 5419: 5399: 5398: 5393: 5384: 5364: 5362: 5361: 5356: 5354: 5353: 5348: 5339: 5324: 5322: 5321: 5316: 5314: 5313: 5308: 5299: 5298: 5295: 5283: 5278: 5277: 5272: 5263: 5256: 5255: 5254: 5249: 5242: 5237: 5228: 5223: 5221: 5220: 5211: 5210: 5201: 5199: 5197: 5196: 5195: 5194: 5177: 5176: 5174: 5173: 5164: 5158: 5153: 5151: 5150: 5149: 5138: 5130: 5122: 5110: 5108: 5107: 5102: 5100: 5099: 5083: 5081: 5080: 5075: 5057: 5055: 5054: 5049: 5030: 5028: 5027: 5022: 5010: 5008: 5007: 5002: 5000: 4995: 4987: 4972: 4970: 4969: 4964: 4949: 4947: 4946: 4941: 4939: 4938: 4935: 4919: 4917: 4916: 4911: 4896: 4894: 4893: 4888: 4886: 4882: 4881: 4876: 4874: 4869: 4866: 4860: 4859: 4849: 4833: 4832: 4823: 4822: 4813: 4811: 4800: 4795: 4794: 4789: 4780: 4779: 4776: 4764: 4745: 4743: 4742: 4737: 4725: 4723: 4722: 4717: 4693: 4691: 4690: 4685: 4672:root mean square 4669: 4667: 4666: 4661: 4646: 4644: 4643: 4638: 4636: 4632: 4631: 4629: 4628: 4619: 4618: 4609: 4593: 4592: 4548: 4546: 4545: 4540: 4528: 4526: 4525: 4520: 4496: 4494: 4493: 4488: 4458: 4456: 4455: 4450: 4445: 4433: 4412: 4395: 4379: 4375: 4364: 4350: 4349: 4340: 4332: 4280: 4278: 4277: 4272: 4270: 4269: 4253: 4251: 4250: 4245: 4243: 4242: 4239: 4223: 4221: 4220: 4215: 4210: 4205: 4197: 4189: 4188: 4187: 4171: 4163: 4158: 4157: 4154: 4146: 4139: 4138: 4137: 4134: 4118: 4117: 4088: 4086: 4085: 4080: 4078: 4077: 4076: 4073: 4057: 4056: 3982:plasma frequency 3831: 3829: 3828: 3823: 3809: 3808: 3785: 3783: 3782: 3777: 3772: 3771: 3756: 3755: 3726: 3706: 3704: 3703: 3698: 3696: 3694: 3686: 3685: 3684: 3671: 3662: 3660: 3659: 3654: 3652: 3651: 3624:plasma frequency 3486: 3468: 3458: 3454: 3436: 3414: 3412: 3411: 3406: 3404: 3403: 3399: 3390: 3386: 3383: 3378: 3369: 3368: 3367: 3355: 3346: 3337: 3331: 3324: 3322: 3311: 3306: 3305: 3279: 3277: 3276: 3271: 3266: 3264: 3259: 3243: 3221: 3219: 3218: 3213: 3201: 3151: 3149: 3148: 3143: 3138: 3134: 3133: 3131: 3130: 3129: 3116: 3096: 3087: 3085: 3084: 3080: 3071: 3067: 3065: 3064: 3063: 3047: 3037: 3036: 3035: 3022: 3012: 3005: 2997: 2984: 2980: 2979: 2978: 2974: 2965: 2961: 2959: 2958: 2957: 2941: 2931: 2930: 2929: 2916: 2906: 2899: 2891: 2877: 2858: 2846: 2845: 2820:| >> 2819: 2742: 2740: 2739: 2734: 2729: 2724: 2722: 2717: 2716: 2715: 2702: 2701: 2700: 2674: 2672: 2671: 2666: 2661: 2659: 2658: 2643: 2641: 2636: 2635: 2634: 2621: 2620: 2619: 2583:asymptotic limit 2568: 2566: 2565: 2560: 2558: 2557: 2556: 2516: 2514: 2513: 2508: 2506: 2503: 2502: 2501: 2492: 2491: 2490: 2479: 2478: 2477: 2464: 2463: 2458: 2457: 2456: 2433: 2431: 2430: 2425: 2420: 2418: 2417: 2407: 2402: 2401: 2391: 2339: 2337: 2336: 2331: 2326: 2325: 2321: 2312: 2308: 2306: 2305: 2304: 2292: 2291: 2281: 2280: 2279: 2270: 2269: 2259: 2252: 2244: 2239: 2238: 2216: 2214: 2213: 2208: 2190: 2189: 2184: 2180: 2172: 2165: 2164: 2151: 2146: 2130: 2125: 2103: 2101: 2100: 2095: 2087: 2085: 2084: 2075: 2074: 2062: 2057: 2055: 2054: 2045: 2044: 2032: 2012: 2010: 2009: 2004: 2002: 2000: 1996: 1995: 1979: 1975: 1974: 1964: 1959: 1957: 1956: 1947: 1946: 1937: 1916: 1914: 1913: 1908: 1906: 1905: 1889: 1887: 1886: 1881: 1879: 1877: 1873: 1872: 1856: 1852: 1851: 1841: 1833: 1831: 1830: 1821: 1820: 1811: 1801: 1799: 1798: 1793: 1791: 1790: 1768: 1766: 1765: 1760: 1758: 1757: 1735: 1733: 1732: 1727: 1725: 1724: 1678: 1676: 1675: 1670: 1668: 1667: 1655: 1654: 1642: 1641: 1621: 1619: 1618: 1613: 1611: 1610: 1586: 1584: 1583: 1578: 1576: 1575: 1563: 1562: 1544: 1542: 1541: 1536: 1511: 1509: 1508: 1503: 1485: 1483: 1482: 1477: 1449: 1447: 1446: 1441: 1439: 1438: 1425: 1417: 1412: 1411: 1387: 1386: 1369: 1368: 1329: 1328: 1305: 1303: 1302: 1297: 1295: 1294: 1281: 1273: 1268: 1267: 1243: 1242: 1225: 1223: 1222: 1207: 1206: 1197: 1195: 1194: 1152: 1151: 1128: 1126: 1125: 1120: 1118: 1117: 1104: 1096: 1091: 1090: 1066: 1065: 1048: 1047: 1008: 1007: 983:are as follows: 978: 976: 975: 970: 932: 930: 929: 924: 906: 904: 903: 898: 880: 878: 877: 872: 801: 786: 760:photolithography 691: 684: 677: 664: 659: 658: 651: 647: 646: 267:Spin Hall effect 157:Phase transition 127:Luttinger liquid 64:States of matter 47:Phase transition 33: 19: 7816: 7815: 7811: 7810: 7809: 7807: 7806: 7805: 7776: 7775: 7759: 7754: 7751: 7697: 7692: 7684: 7637: 7632: 7582: 7577: 7538: 7533: 7530: 7528:Further reading 7525: 7518: 7501: 7500: 7496: 7464: 7463: 7459: 7429: 7428: 7421: 7389: 7388: 7384: 7338: 7337: 7333: 7287: 7286: 7282: 7236: 7235: 7231: 7179: 7178: 7169: 7105: 7104: 7097: 7040: 7039: 7035: 6979: 6978: 6967: 6960: 6945: 6944: 6940: 6909: 6908: 6904: 6874: 6873: 6869: 6840:(12): 4403–11. 6831: 6830: 6826: 6788: 6787: 6783: 6724: 6723: 6719: 6712: 6699: 6698: 6694: 6648: 6647: 6643: 6586: 6585: 6581: 6574: 6558: 6557: 6550: 6543: 6527:Kittel, Charles 6525: 6524: 6520: 6496: 6495: 6488: 6481: 6468: 6467: 6463: 6456: 6436: 6435: 6428: 6402: 6401: 6397: 6357:physics/0604227 6341: 6340: 6336: 6319: 6310: 6301: 6299: 6295: 6290: 6289: 6282: 6206: 6201: 6156: 6155: 6151: 6142: 6140: 6136: 6131: 6130: 6126: 6109: 6100: 6091: 6089: 6083: 6075: 6073: 6067: 6066: 6057: 6017: 6012: 6011: 6007: 6003: 5998: 5997: 5980: 5973: 5968: 5950:Surface plasmon 5921: 5886: 5876: 5868: 5861: 5860: 5831: 5818: 5817: 5792: 5791: 5764: 5763: 5744: 5743: 5711: 5683: 5654: 5648: 5626: 5620: 5597: 5575: 5574: 5547: 5515: 5500: 5474: 5441: 5420: 5388: 5375: 5374: 5343: 5330: 5329: 5303: 5290: 5267: 5244: 5212: 5202: 5186: 5178: 5165: 5159: 5141: 5131: 5123: 5116: 5115: 5091: 5086: 5085: 5063: 5062: 5037: 5036: 5013: 5012: 4988: 4975: 4974: 4955: 4954: 4930: 4925: 4924: 4902: 4901: 4851: 4850: 4844: 4840: 4824: 4814: 4804: 4784: 4771: 4755: 4754: 4728: 4727: 4696: 4695: 4676: 4675: 4652: 4651: 4620: 4610: 4604: 4600: 4584: 4558: 4557: 4531: 4530: 4499: 4498: 4464: 4463: 4438: 4426: 4405: 4388: 4368: 4357: 4341: 4305: 4304: 4289:is an integer. 4261: 4256: 4255: 4234: 4229: 4228: 4198: 4179: 4149: 4122: 4103: 4098: 4097: 4061: 4045: 4031: 4030: 4020: 3978: 3976:Other materials 3794: 3789: 3788: 3763: 3741: 3736: 3735: 3687: 3676: 3672: 3665: 3664: 3637: 3632: 3631: 3620: 3600: 3566:Surface plasmon 3495: 3488: 3480: 3469: 3460: 3456: 3448: 3437: 3428: 3359: 3332: 3326: 3325: 3315: 3297: 3292: 3291: 3247: 3231: 3230: 3173: 3172: 3161: 3121: 3101: 3055: 3038: 3027: 3013: 3007: 3006: 2995: 2991: 2949: 2932: 2921: 2907: 2901: 2900: 2889: 2885: 2837: 2832: 2831: 2826: 2817: 2811: 2809: 2802: 2795: 2784: 2777: 2766: 2759: 2752: 2706: 2688: 2683: 2682: 2650: 2625: 2607: 2602: 2601: 2548: 2542: 2541: 2493: 2482: 2480: 2469: 2465: 2447: 2442: 2441: 2409: 2364: 2363: 2296: 2283: 2282: 2271: 2261: 2260: 2254: 2253: 2230: 2225: 2224: 2167: 2166: 2156: 2112: 2111: 2076: 2063: 2046: 2033: 2026: 2025: 1981: 1980: 1966: 1965: 1948: 1938: 1931: 1930: 1897: 1892: 1891: 1858: 1857: 1843: 1842: 1822: 1812: 1805: 1804: 1776: 1771: 1770: 1743: 1738: 1737: 1716: 1711: 1710: 1659: 1646: 1633: 1628: 1627: 1602: 1597: 1596: 1567: 1554: 1549: 1548: 1527: 1526: 1488: 1487: 1462: 1461: 1397: 1378: 1370: 1360: 1314: 1309: 1308: 1253: 1234: 1226: 1208: 1198: 1186: 1137: 1132: 1131: 1076: 1057: 1049: 1039: 993: 988: 987: 943: 942: 939:magnetic fields 909: 908: 883: 882: 857: 856: 849: 809: 808: 807: 806: 805: 802: 793: 792: 791: 787: 776: 730:surface plasmon 695: 654: 641: 640: 633: 632: 631: 431: 423: 422: 421: 397:Amorphous solid 391: 381: 380: 379: 358: 340: 330: 329: 328: 317: 315:Antiferromagnet 308: 306:Superparamagnet 299: 286: 285:Magnetic phases 278: 277: 276: 256: 248: 247: 246: 176: 168: 167: 166: 152:Order parameter 146: 145:Phase phenomena 138: 137: 136: 66: 56: 17: 12: 11: 5: 7814: 7812: 7804: 7803: 7798: 7793: 7788: 7786:Quasiparticles 7778: 7777: 7774: 7773: 7750: 7749:External links 7747: 7746: 7745: 7690: 7687:on 2011-08-11. 7630: 7593:(12): 123901. 7575: 7529: 7526: 7524: 7523: 7516: 7494: 7457: 7438:(5): 331–336. 7419: 7400:(4): 353–356. 7382: 7346:Optics Express 7331: 7296:(16): 164705. 7280: 7245:(3): 528–539. 7229: 7192:(3): 326–333. 7167: 7114:(14): 143201. 7095: 7042:Boltasseva, A. 7033: 6988:(6): 795–808. 6965: 6958: 6938: 6902: 6867: 6824: 6797:(44): 444004. 6791:Nanotechnology 6781: 6717: 6711:978-1439893784 6710: 6692: 6656:Optics Express 6641: 6579: 6572: 6548: 6541: 6518: 6486: 6480:978-0750305884 6479: 6461: 6455:978-3540173632 6454: 6438:Raether, Heinz 6426: 6395: 6334: 6332: 6331: 6322:Nanoplasmonics 6280: 6278: 6277: 6270: 6217:(6): 1985–90. 6149: 6124: 6122: 6121: 6097: 6055: 6004: 6002: 5999: 5996: 5995: 5970: 5969: 5967: 5964: 5963: 5962: 5957: 5952: 5947: 5942: 5940:Plasmonic lens 5937: 5932: 5927: 5920: 5917: 5904: 5901: 5893: 5889: 5882: 5879: 5874: 5871: 5848: 5845: 5840: 5835: 5830: 5826: 5805: 5802: 5799: 5771: 5751: 5740: 5739: 5724: 5718: 5714: 5709: 5704: 5699: 5695: 5692: 5689: 5686: 5682: 5674: 5671: 5667: 5661: 5657: 5652: 5646: 5643: 5639: 5633: 5629: 5624: 5617: 5614: 5610: 5604: 5600: 5595: 5591: 5588: 5585: 5582: 5568: 5567: 5554: 5550: 5545: 5541: 5538: 5535: 5530: 5526: 5522: 5518: 5513: 5507: 5503: 5498: 5493: 5489: 5486: 5481: 5477: 5473: 5470: 5467: 5464: 5457: 5453: 5448: 5444: 5437: 5433: 5427: 5423: 5418: 5414: 5411: 5408: 5405: 5402: 5397: 5392: 5387: 5383: 5352: 5347: 5342: 5338: 5326: 5325: 5312: 5307: 5302: 5293: 5289: 5286: 5282: 5276: 5271: 5266: 5262: 5253: 5248: 5241: 5236: 5232: 5227: 5219: 5215: 5209: 5205: 5193: 5189: 5184: 5181: 5172: 5168: 5162: 5156: 5148: 5144: 5137: 5134: 5129: 5126: 5098: 5094: 5073: 5070: 5047: 5044: 5020: 4998: 4994: 4991: 4985: 4982: 4962: 4933: 4909: 4898: 4897: 4885: 4879: 4873: 4864: 4858: 4854: 4847: 4843: 4839: 4836: 4831: 4827: 4821: 4817: 4810: 4807: 4803: 4798: 4793: 4788: 4783: 4774: 4770: 4767: 4763: 4735: 4715: 4712: 4709: 4706: 4703: 4683: 4659: 4648: 4647: 4635: 4627: 4623: 4617: 4613: 4607: 4603: 4599: 4596: 4591: 4587: 4583: 4580: 4577: 4574: 4571: 4568: 4565: 4538: 4518: 4515: 4512: 4509: 4506: 4486: 4483: 4480: 4477: 4474: 4471: 4460: 4459: 4448: 4444: 4441: 4437: 4432: 4429: 4425: 4421: 4418: 4415: 4411: 4408: 4404: 4401: 4398: 4394: 4391: 4387: 4384: 4378: 4374: 4371: 4367: 4363: 4360: 4356: 4353: 4348: 4344: 4338: 4335: 4330: 4327: 4324: 4321: 4318: 4315: 4312: 4268: 4264: 4237: 4225: 4224: 4213: 4208: 4204: 4201: 4195: 4192: 4186: 4182: 4177: 4174: 4169: 4166: 4161: 4152: 4145: 4142: 4132: 4129: 4125: 4121: 4116: 4113: 4110: 4106: 4089:. The grating 4071: 4068: 4064: 4060: 4055: 4052: 4048: 4044: 4041: 4038: 4019: 4016: 3977: 3974: 3967: 3966: 3963: 3960: 3957: 3954: 3953: 3950: 3947: 3944: 3941: 3940: 3937: 3934: 3931: 3927: 3926: 3923: 3920: 3917: 3914: 3913: 3910: 3907: 3904: 3901: 3900: 3897: 3894: 3891: 3887: 3886: 3883: 3880: 3877: 3874: 3873: 3870: 3867: 3864: 3861: 3860: 3857: 3854: 3851: 3847: 3846: 3843: 3840: 3837: 3833: 3832: 3821: 3818: 3815: 3812: 3807: 3804: 3801: 3797: 3786: 3775: 3770: 3766: 3762: 3759: 3754: 3751: 3748: 3744: 3733: 3730: 3693: 3690: 3683: 3679: 3675: 3650: 3647: 3644: 3640: 3619: 3616: 3599: 3598:Materials used 3596: 3552:incident angle 3494: 3491: 3490: 3489: 3470: 3463: 3461: 3457:(0.3 × 370 nm) 3441:electric field 3438: 3431: 3427: 3424: 3416: 3415: 3402: 3398: 3394: 3389: 3382: 3377: 3373: 3366: 3362: 3358: 3354: 3349: 3345: 3341: 3336: 3329: 3321: 3318: 3314: 3309: 3304: 3300: 3281: 3280: 3269: 3262: 3258: 3254: 3250: 3246: 3241: 3238: 3211: 3208: 3204: 3200: 3196: 3192: 3189: 3186: 3183: 3180: 3165:electric field 3160: 3157: 3153: 3152: 3141: 3137: 3128: 3124: 3119: 3115: 3111: 3107: 3104: 3099: 3095: 3091: 3083: 3079: 3075: 3070: 3062: 3058: 3054: 3050: 3046: 3042: 3034: 3030: 3025: 3021: 3017: 3010: 3003: 3000: 2994: 2990: 2987: 2983: 2977: 2973: 2969: 2964: 2956: 2952: 2948: 2944: 2940: 2936: 2928: 2924: 2919: 2915: 2911: 2904: 2897: 2894: 2888: 2884: 2880: 2876: 2872: 2868: 2865: 2861: 2857: 2853: 2849: 2844: 2840: 2824: 2815: 2807: 2800: 2793: 2782: 2775: 2764: 2757: 2750: 2744: 2743: 2732: 2727: 2721: 2714: 2709: 2705: 2699: 2696: 2691: 2676: 2675: 2664: 2657: 2653: 2649: 2646: 2640: 2633: 2628: 2624: 2618: 2615: 2610: 2555: 2551: 2538:effective mass 2518: 2517: 2500: 2496: 2489: 2485: 2476: 2472: 2468: 2461: 2455: 2450: 2435: 2434: 2423: 2416: 2412: 2406: 2400: 2395: 2389: 2386: 2383: 2380: 2377: 2374: 2371: 2341: 2340: 2329: 2324: 2320: 2316: 2311: 2303: 2299: 2295: 2290: 2286: 2278: 2274: 2268: 2264: 2257: 2250: 2247: 2242: 2237: 2233: 2218: 2217: 2206: 2203: 2200: 2197: 2194: 2188: 2183: 2178: 2175: 2170: 2163: 2159: 2155: 2150: 2145: 2142: 2138: 2134: 2129: 2124: 2120: 2105: 2104: 2093: 2090: 2083: 2079: 2073: 2070: 2066: 2060: 2053: 2049: 2043: 2040: 2036: 2015: 2014: 1999: 1994: 1991: 1988: 1984: 1978: 1973: 1969: 1962: 1955: 1951: 1945: 1941: 1904: 1900: 1876: 1871: 1868: 1865: 1861: 1855: 1850: 1846: 1839: 1836: 1829: 1825: 1819: 1815: 1802: 1789: 1786: 1783: 1779: 1756: 1753: 1750: 1746: 1723: 1719: 1684: 1666: 1662: 1658: 1653: 1649: 1645: 1640: 1636: 1609: 1605: 1574: 1570: 1566: 1561: 1557: 1546: 1534: 1523: 1513: 1501: 1498: 1495: 1475: 1472: 1469: 1451: 1450: 1437: 1434: 1431: 1428: 1424: 1420: 1416: 1410: 1407: 1404: 1400: 1396: 1393: 1390: 1385: 1381: 1377: 1373: 1367: 1363: 1359: 1356: 1353: 1350: 1347: 1344: 1341: 1338: 1335: 1332: 1327: 1324: 1321: 1317: 1306: 1293: 1290: 1287: 1284: 1280: 1276: 1272: 1266: 1263: 1260: 1256: 1252: 1249: 1246: 1241: 1237: 1233: 1229: 1221: 1218: 1215: 1211: 1205: 1201: 1193: 1189: 1185: 1182: 1179: 1176: 1173: 1170: 1167: 1164: 1161: 1158: 1155: 1150: 1147: 1144: 1140: 1129: 1116: 1113: 1110: 1107: 1103: 1099: 1095: 1089: 1086: 1083: 1079: 1075: 1072: 1069: 1064: 1060: 1056: 1052: 1046: 1042: 1038: 1035: 1032: 1029: 1026: 1023: 1020: 1017: 1014: 1011: 1006: 1003: 1000: 996: 968: 965: 962: 959: 956: 953: 950: 922: 919: 916: 896: 893: 890: 870: 867: 864: 848: 845: 803: 796: 795: 794: 788: 781: 780: 779: 778: 777: 775: 772: 697: 696: 694: 693: 686: 679: 671: 668: 667: 666: 665: 652: 635: 634: 630: 629: 624: 619: 614: 609: 604: 599: 594: 589: 584: 579: 574: 569: 564: 559: 554: 549: 544: 539: 534: 529: 524: 519: 514: 509: 504: 499: 494: 489: 484: 479: 474: 469: 464: 459: 454: 449: 444: 439: 433: 432: 429: 428: 425: 424: 420: 419: 414: 412:Liquid crystal 409: 404: 399: 393: 392: 387: 386: 383: 382: 378: 377: 372: 367: 362: 353: 348: 342: 341: 338:Quasiparticles 336: 335: 332: 331: 327: 326: 321: 312: 303: 297:Superdiamagnet 294: 288: 287: 284: 283: 280: 279: 275: 274: 269: 264: 258: 257: 254: 253: 250: 249: 245: 244: 239: 234: 229: 224: 222:Thermoelectric 219: 217:Superconductor 214: 209: 204: 199: 197:Mott insulator 194: 189: 184: 178: 177: 174: 173: 170: 169: 165: 164: 159: 154: 148: 147: 144: 143: 140: 139: 135: 134: 129: 124: 119: 114: 109: 104: 99: 94: 89: 84: 79: 74: 68: 67: 62: 61: 58: 57: 55: 54: 49: 44: 38: 35: 34: 26: 25: 15: 13: 10: 9: 6: 4: 3: 2: 7813: 7802: 7801:Surface waves 7799: 7797: 7794: 7792: 7791:Metamaterials 7789: 7787: 7784: 7783: 7781: 7771: 7765: 7758: 7753: 7752: 7748: 7741: 7737: 7733: 7729: 7725: 7721: 7716: 7711: 7707: 7703: 7696: 7691: 7683: 7679: 7675: 7671: 7667: 7663: 7659: 7655: 7651: 7647: 7643: 7636: 7631: 7626: 7622: 7617: 7612: 7608: 7604: 7600: 7596: 7592: 7588: 7581: 7576: 7572: 7568: 7564: 7563:10.1038/35570 7560: 7556: 7552: 7549:(6668): 667. 7548: 7544: 7537: 7532: 7531: 7527: 7519: 7513: 7509: 7505: 7498: 7495: 7490: 7486: 7482: 7478: 7474: 7470: 7469: 7461: 7458: 7453: 7449: 7445: 7441: 7437: 7433: 7426: 7424: 7420: 7415: 7411: 7407: 7403: 7399: 7396:(in German). 7395: 7394: 7386: 7383: 7378: 7374: 7369: 7364: 7360: 7356: 7352: 7348: 7347: 7342: 7335: 7332: 7327: 7323: 7319: 7315: 7311: 7307: 7303: 7299: 7295: 7291: 7284: 7281: 7276: 7272: 7268: 7264: 7260: 7256: 7252: 7248: 7244: 7240: 7233: 7230: 7225: 7221: 7216: 7211: 7207: 7203: 7199: 7195: 7191: 7187: 7186:ACS Photonics 7183: 7176: 7174: 7172: 7168: 7163: 7159: 7155: 7151: 7147: 7143: 7139: 7135: 7131: 7127: 7122: 7117: 7113: 7109: 7102: 7100: 7096: 7091: 7087: 7083: 7079: 7075: 7071: 7067: 7063: 7059: 7055: 7051: 7047: 7043: 7037: 7034: 7029: 7025: 7021: 7017: 7013: 7009: 7005: 7001: 6996: 6991: 6987: 6983: 6976: 6974: 6972: 6970: 6966: 6961: 6955: 6951: 6950: 6942: 6939: 6934: 6930: 6926: 6922: 6918: 6914: 6906: 6903: 6898: 6894: 6890: 6886: 6882: 6878: 6871: 6868: 6863: 6859: 6855: 6851: 6847: 6843: 6839: 6835: 6828: 6825: 6820: 6816: 6812: 6808: 6804: 6800: 6796: 6792: 6785: 6782: 6777: 6773: 6769: 6765: 6760: 6755: 6751: 6747: 6743: 6739: 6735: 6731: 6727: 6721: 6718: 6713: 6707: 6703: 6696: 6693: 6688: 6684: 6679: 6674: 6670: 6666: 6662: 6658: 6657: 6652: 6645: 6642: 6637: 6633: 6629: 6625: 6620: 6615: 6611: 6607: 6603: 6599: 6598: 6593: 6589: 6588:Pendry, J. B. 6583: 6580: 6575: 6569: 6565: 6564: 6555: 6553: 6549: 6544: 6538: 6534: 6533: 6528: 6522: 6519: 6513: 6508: 6504: 6500: 6493: 6491: 6487: 6482: 6476: 6472: 6465: 6462: 6457: 6451: 6447: 6443: 6439: 6433: 6431: 6427: 6422: 6418: 6415:: 1128–1133. 6414: 6410: 6406: 6399: 6396: 6391: 6387: 6383: 6379: 6375: 6371: 6367: 6363: 6358: 6353: 6350:(6): 1113–5. 6349: 6345: 6338: 6335: 6328: 6324: 6323: 6317: 6308: 6307: 6294: 6287: 6285: 6281: 6275: 6271: 6266: 6262: 6258: 6254: 6250: 6249:10044/1/42407 6246: 6242: 6238: 6234: 6230: 6225: 6220: 6216: 6212: 6205: 6200: 6199: 6196: 6192: 6188: 6184: 6180: 6176: 6172: 6168: 6164: 6160: 6153: 6150: 6135: 6128: 6125: 6118: 6114: 6113: 6107: 6098: 6087: 6082: 6081: 6071: 6064: 6062: 6060: 6056: 6051: 6047: 6043: 6039: 6035: 6031: 6027: 6023: 6016: 6009: 6006: 6000: 5992: 5988: 5984: 5978: 5976: 5972: 5965: 5961: 5958: 5956: 5953: 5951: 5948: 5946: 5943: 5941: 5938: 5936: 5933: 5931: 5928: 5926: 5923: 5922: 5918: 5916: 5902: 5899: 5891: 5887: 5877: 5872: 5869: 5846: 5843: 5838: 5828: 5803: 5800: 5797: 5789: 5786:-axis in the 5785: 5769: 5749: 5716: 5712: 5702: 5697: 5693: 5690: 5687: 5684: 5680: 5672: 5669: 5659: 5655: 5644: 5641: 5631: 5627: 5615: 5602: 5598: 5589: 5586: 5580: 5573: 5572: 5571: 5552: 5543: 5539: 5536: 5533: 5528: 5524: 5520: 5505: 5501: 5491: 5487: 5484: 5479: 5475: 5471: 5468: 5455: 5451: 5446: 5442: 5425: 5421: 5412: 5409: 5403: 5400: 5395: 5385: 5373: 5372: 5371: 5368: 5350: 5340: 5310: 5291: 5284: 5274: 5264: 5251: 5239: 5234: 5230: 5217: 5213: 5207: 5203: 5191: 5187: 5182: 5179: 5170: 5166: 5160: 5154: 5146: 5142: 5132: 5127: 5124: 5114: 5113: 5112: 5096: 5092: 5068: 5061: 5045: 5042: 5032: 5018: 4996: 4992: 4989: 4983: 4980: 4960: 4951: 4931: 4923: 4907: 4883: 4877: 4871: 4862: 4856: 4852: 4845: 4841: 4837: 4834: 4829: 4825: 4819: 4815: 4808: 4805: 4801: 4796: 4791: 4772: 4765: 4753: 4752: 4751: 4749: 4733: 4710: 4707: 4704: 4681: 4673: 4657: 4633: 4625: 4621: 4615: 4611: 4605: 4601: 4597: 4594: 4589: 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704:( 690:e 683:t 676:v

Index

Condensed matter physics

Phases
Phase transition
QCP
States of matter
Solid
Liquid
Gas
Plasma
Bose–Einstein condensate
Bose gas
Fermionic condensate
Fermi gas
Fermi liquid
Supersolid
Superfluidity
Luttinger liquid
Time crystal
Order parameter
Phase transition
QCP
Electronic band structure
Plasma
Insulator
Mott insulator
Semiconductor
Semimetal
Conductor
Superconductor

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