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Spoof surface plasmon

Spoof surface plasmons, also known as spoof surface plasmon polaritons and designer surface plasmons,[1] are surface electromagnetic waves in microwave and terahertz regimes that propagate along planar interfaces with sign-changing permittivities. Spoof surface plasmons are a type of surface plasmon polariton, which ordinarily propagate along metal and dielectric interfaces in infrared and visible frequencies. Since surface plasmon polaritons cannot exist naturally in microwave and terahertz frequencies due to dispersion properties of metals, spoof surface plasmons necessitate the use of artificially-engineered metamaterials.

Spoof surface plasmons share the natural properties of surface plasmon polaritons, such as dispersion characteristics and subwavelength field confinement. They were first theorized by John Pendry et al.[2]

Theory edit

 
SPP oscillation in between a metal-dielectric interface

Surface plasmon polaritons (SPP) result from the coupling of delocalized electron oscillations ("surface plasmon") to electromagnetic waves ("polariton"). SPPs propagate along the interface between a positive- and a negative-permittivity material. These waves decay perpendicularly from the interface ("evanescent field"). For a plasmonic medium that is stratified along the z-direction in Cartesian coordinates, dispersion relation for SPPs can be obtained from solving Maxwell's equations:[3]

 

where

  •   is the wave vector that is parallel to the interface. It is in the direction of propagation.
  •   is the angular frequency.
  •   is the speed of light.
  •   and   are the relative permittivies for metal and the dielectric.

Per this relation, SPPs have shorter wavelengths than light in free space for a frequency band below surface plasmon frequency; this property, as well as subwavelength confinement, enables new applications in subwavelength optics and systems beyond the diffraction-limit.[3] Nevertheless, for lower frequency bands such as microwave and terahertz, surface plasmon polariton modes are not supported; metals function approximately as perfect electrical conductors with imaginary dielectric functions in this regime.[4] Per the effective medium approach, metal surfaces with subwavelength structural elements can mimic the plasma behaviour, resulting in artificial surface plasmon polariton excitations with similar dispersion behaviour.[4][5][6]

For the canonical case of a metamaterial medium that is formed by thin metallic wires on a periodic square lattice, the effective relative permittivity can be represented by the Drude model formula:[4]

 
 

where

  •   is the effective plasma frequency of the medium.
  •   is the vacuum permittivity.
  •   is the lattice period.
  •   is the radius of the constitutive wires.
  •   is the electrical conductivity of the metal.

Methods and applications edit

Simulation of spoof surface plasmon propagation through a backward-wave metamaterial in the microwave regime[7]

The use of subwavelength structures to induce low-frequency plasmonic excitations was first theorized by John Pendry et al. in 1996; Pendry proposed that a periodic lattice of thin metallic wires with a radius of 1 μm could be used to support surface-bound modes, with a plasma cut-off frequency of 8.2 GHz.[4] In 2004, Pendry et al. extended the approach to metal surfaces that are perforated by holes, terming the artificial SPP excitations as "spoof surface plasmons."[5][6]

In 2006, terahertz pulse propagation in planar metallic structures with holes were shown via FDTD simulations.[8] Martin-Cano et al. has realized the spatial and temporal modulation of guided terahertz modes via metallic parallelepiped structures, which they termed as "domino plasmons."[9] Designer spoof plasmonic structures were also tailored to improve the performance of terahertz quantum cascade lasers in 2010.[10]

Spoof surface plasmons were proposed as a possible solution for decreasing the crosstalk in microwave integrated circuits, transmission lines and waveguides.[2] In 2013, Ma et al. demonstrated a matched conversion from coplanar waveguide with a characteristic impedance of 50Ω to a spoof-plasmonic structure.[11] In 2014, integration of commercial low-noise amplifier with spoof plasmonic structures was realized; the system reportedly worked from 6 to 20 GHz with a gain around 20 dB.[12] Kianinejad et al. also reported the design of a slow-wave spoof-plasmonic transmission line; conversion from quasi-TEM microstrip modes to TM spoof plasmon modes were also demonstrated.[13]

Khanikaev et al. reported nonreciprocal spoof surface plasmon modes in structured conductor embedded in an asymmetric magneto-optical medium, which results in one-way transmission.[14] Pan et al. observed the rejection of certain spoof plasmon modes with an introduction of electrically resonant metamaterial particles to the spoof plasmonic strip.[15] Localized spoof surface plasmons were also demonstrated for metallic disks in microwave frequencies.[16][17]

See also edit

References edit

  1. ^ Garcia-Vidal, Francisco J.; Fernández-Domínguez, Antonio I.; Martin-Moreno, Luis; Zhang, Hao Chi; Tang, Wenxuan; Peng, Ruwen; Cui, Tie Jun (2022). "Spoof surface plasmon photonics". Reviews of Modern Physics. 04 (2): 025004. Bibcode:2022RvMP...94b5004G. doi:10.1103/RevModPhys.94.025004. hdl:10261/280707. S2CID 248954068.
  2. ^ a b Tang, Wen Xuan; Zhang, Hao Chi; Ma, Hui Feng; Jiang, Wei Xiang; et al. (4 January 2019). "Concept, Theory, Design, and Applications of Spoof Surface Plasmon Polaritons at Microwave Frequencies". Advanced Optical Materials. 7 (1): 1800421. doi:10.1002/adom.201800421.
  3. ^ a b Maier, Stefan A. (2007). Plasmonics: Fundamentals and Applications. New York: Springer Publishing. ISBN 978-0-387-33150-8.
  4. ^ a b c d Pendry, J. B.; Holden, A. J.; Stewart, W. J.; Youngs, I. (June 1996). "Extremely Low Frequency Plasmons in Metallic Mesostructures". Physical Review Letters. 46 (25): 4773–4776. Bibcode:1996PhRvL..76.4773P. doi:10.1103/PhysRevLett.76.4773. PMID 10061377.
  5. ^ a b Pendry, J. B.; Martín-Moreno, L.; Garcia-Vidal, F. J. (6 August 2004). "Mimicking Surface Plasmons with Structured Surfaces". Science. 305 (5685): 847–848. Bibcode:2004Sci...305..847P. doi:10.1126/science.1098999. PMID 15247438. S2CID 44412157.
  6. ^ a b Garcia-Vidal, F. J.; Martín-Moreno, L.; Pendry, J. B. (January 2005). "Surfaces with holes in them: new plasmonic metamaterials". Journal of Optics A. 7 (2): S97–S101. Bibcode:2005JOptA...7S..97G. doi:10.1088/1464-4258/7/2/013.
  7. ^ Liu, Xiaoyong; Feng, Yijun; Zhu, Bo; Zhao, Junming; Jiang, Tian (February 2016). "Backward spoof surface wave in plasmonic metamaterial of ultrathin metallic structure". Scientific Reports. 6 (6): 20448. Bibcode:2016NatSR...620448L. doi:10.1038/srep20448. PMC 4740866. PMID 26842340.
  8. ^ Maier, Stefan A.; Andrews, Steve R. (June 2006). "Terahertz pulse propagation using plasmon-polariton-like surface modes on structured conductive surfaces". Applied Physics Letters. 88 (25): 251120. Bibcode:2006ApPhL..88y1120M. doi:10.1063/1.2216105.
  9. ^ Martin-Cano, D.; Nesterov, M. L.; Fernandez-Dominguez, A. I.; Garcia-Vidal, F. J.; Martin-Moreno, L.; Moreno, Esteban (2010). "Domino plasmons for subwavelength terahertz circuitry". Optics Express. 18 (2): 754–764. arXiv:0911.4525. Bibcode:2010OExpr..18..754M. doi:10.1364/OE.18.000754. hdl:10261/47867. PMID 20173896. S2CID 2299072.
  10. ^ Yu, Nanfang; Wang, Qi Jie; Kats, Mikhail A.; Capasso, Federico; et al. (August 2010). "Designer spoof surface plasmon structures collimate terahertz laser beams". Nature Materials. 9 (9): 730–735. Bibcode:2010NatMa...9..730Y. doi:10.1038/nmat2822. PMID 20693995.
  11. ^ Ma, Hui Feng; Shen, Xiaopeng; Cheng, Qiang; Jiang, Wei Xiang; et al. (November 2013). "Broadband and high‐efficiency conversion from guided waves to spoof surface plasmon polaritons". Laser & Photonics Reviews. 8 (1): 146–151. doi:10.1002/lpor.201300118. S2CID 120708454.
  12. ^ Zhang, Hao Chi; Liu, Shuo; Shen, Xiaopeng; Chen, Lin Hui; et al. (November 2014). "Broadband amplification of spoof surface plasmon polaritons at microwave frequencies". Laser & Photonics Reviews. 9 (1): 83–90. doi:10.1002/lpor.201400131. S2CID 118667968.
  13. ^ Kianinejad, Amin; Chen, Zhi Ning; Qiu, Cheng-Wei (June 2015). "Design and Modeling of Spoof Surface Plasmon Modes-Based Microwave Slow-Wave Transmission Line". IEEE Transactions on Microwave Theory and Techniques. 63 (6): 1817–1825. Bibcode:2015ITMTT..63.1817K. doi:10.1109/TMTT.2015.2422694. S2CID 16388137.
  14. ^ Khanikaev, Alexander B.; Mousavi, S. Hossein; Shvets, Gennady; Kivshar, Yuri S. (September 2010). "One-Way Extraordinary Optical Transmission and Nonreciprocal Spoof Plasmons". Physical Review Letters. 105 (12–17): 126804. Bibcode:2010PhRvL.105l6804K. doi:10.1103/PhysRevLett.105.126804. PMID 20867667.
  15. ^ Pan, Bai Cao; Liao, Zhen; Zhao, Jie; Cui, Tie Jun (2014). "Controlling rejections of spoof surface plasmon polaritons using metamaterial particles". Optics Express. 22 (11): 13940–13950. Bibcode:2014OExpr..2213940P. doi:10.1364/OE.22.013940. PMID 24921585.
  16. ^ Shen, Xiaopeng; Cui, Tie Jun (January 2014). "Ultrathin plasmonic metamaterial for spoof localized surface plasmons". Laser & Photonics Reviews. 8 (1): 137–145. Bibcode:2014LPRv....8..137S. doi:10.1002/lpor.201300144. S2CID 118085394.
  17. ^ Huidobro, Paloma A.; Shen, Xiaopeng; Cuerda, J.; Moreno, Esteban; et al. (April 2014). "Magnetic Localized Surface Plasmons". Physical Review X. 4 (2): 021003. Bibcode:2014PhRvX...4b1003H. doi:10.1103/PhysRevX.4.021003.

Further reading edit

spoof, surface, plasmon, also, known, spoof, surface, plasmon, polaritons, designer, surface, plasmons, surface, electromagnetic, waves, microwave, terahertz, regimes, that, propagate, along, planar, interfaces, with, sign, changing, permittivities, type, surf. Spoof surface plasmons also known as spoof surface plasmon polaritons and designer surface plasmons 1 are surface electromagnetic waves in microwave and terahertz regimes that propagate along planar interfaces with sign changing permittivities Spoof surface plasmons are a type of surface plasmon polariton which ordinarily propagate along metal and dielectric interfaces in infrared and visible frequencies Since surface plasmon polaritons cannot exist naturally in microwave and terahertz frequencies due to dispersion properties of metals spoof surface plasmons necessitate the use of artificially engineered metamaterials Spoof surface plasmons share the natural properties of surface plasmon polaritons such as dispersion characteristics and subwavelength field confinement They were first theorized by John Pendry et al 2 Contents 1 Theory 2 Methods and applications 3 See also 4 References 5 Further readingTheory editMain article Surface plasmon polariton nbsp SPP oscillation in between a metal dielectric interfaceSurface plasmon polaritons SPP result from the coupling of delocalized electron oscillations surface plasmon to electromagnetic waves polariton SPPs propagate along the interface between a positive and a negative permittivity material These waves decay perpendicularly from the interface evanescent field For a plasmonic medium that is stratified along the z direction in Cartesian coordinates dispersion relation for SPPs can be obtained from solving Maxwell s equations 3 k x w c e 1 e 2 e 1 e 2 1 2 displaystyle k x frac omega c left frac varepsilon 1 varepsilon 2 varepsilon 1 varepsilon 2 right frac 1 2 nbsp where k x displaystyle k x nbsp is the wave vector that is parallel to the interface It is in the direction of propagation w displaystyle omega nbsp is the angular frequency c displaystyle c nbsp is the speed of light e 1 displaystyle varepsilon 1 nbsp and e 2 displaystyle varepsilon 2 nbsp are the relative permittivies for metal and the dielectric Per this relation SPPs have shorter wavelengths than light in free space for a frequency band below surface plasmon frequency this property as well as subwavelength confinement enables new applications in subwavelength optics and systems beyond the diffraction limit 3 Nevertheless for lower frequency bands such as microwave and terahertz surface plasmon polariton modes are not supported metals function approximately as perfect electrical conductors with imaginary dielectric functions in this regime 4 Per the effective medium approach metal surfaces with subwavelength structural elements can mimic the plasma behaviour resulting in artificial surface plasmon polariton excitations with similar dispersion behaviour 4 5 6 For the canonical case of a metamaterial medium that is formed by thin metallic wires on a periodic square lattice the effective relative permittivity can be represented by the Drude model formula 4 e e f f 1 w p 2 w w i e 0 a 2 w p 2 p r 2 s displaystyle varepsilon eff 1 frac omega p 2 omega left omega i frac varepsilon 0 a 2 omega p 2 pi r 2 sigma right nbsp w p 2 2 p c 2 a 2 l n a r displaystyle omega p 2 frac 2 pi c 2 a 2 ln a r nbsp where w p displaystyle omega p nbsp is the effective plasma frequency of the medium e 0 displaystyle varepsilon 0 nbsp is the vacuum permittivity a displaystyle a nbsp is the lattice period r displaystyle r nbsp is the radius of the constitutive wires s displaystyle sigma nbsp is the electrical conductivity of the metal Methods and applications edit source source source source source source Simulation of spoof surface plasmon propagation through a backward wave metamaterial in the microwave regime 7 The use of subwavelength structures to induce low frequency plasmonic excitations was first theorized by John Pendry et al in 1996 Pendry proposed that a periodic lattice of thin metallic wires with a radius of 1 mm could be used to support surface bound modes with a plasma cut off frequency of 8 2 GHz 4 In 2004 Pendry et al extended the approach to metal surfaces that are perforated by holes terming the artificial SPP excitations as spoof surface plasmons 5 6 In 2006 terahertz pulse propagation in planar metallic structures with holes were shown via FDTD simulations 8 Martin Cano et al has realized the spatial and temporal modulation of guided terahertz modes via metallic parallelepiped structures which they termed as domino plasmons 9 Designer spoof plasmonic structures were also tailored to improve the performance of terahertz quantum cascade lasers in 2010 10 Spoof surface plasmons were proposed as a possible solution for decreasing the crosstalk in microwave integrated circuits transmission lines and waveguides 2 In 2013 Ma et al demonstrated a matched conversion from coplanar waveguide with a characteristic impedance of 50W to a spoof plasmonic structure 11 In 2014 integration of commercial low noise amplifier with spoof plasmonic structures was realized the system reportedly worked from 6 to 20 GHz with a gain around 20 dB 12 Kianinejad et al also reported the design of a slow wave spoof plasmonic transmission line conversion from quasi TEM microstrip modes to TM spoof plasmon modes were also demonstrated 13 Khanikaev et al reported nonreciprocal spoof surface plasmon modes in structured conductor embedded in an asymmetric magneto optical medium which results in one way transmission 14 Pan et al observed the rejection of certain spoof plasmon modes with an introduction of electrically resonant metamaterial particles to the spoof plasmonic strip 15 Localized spoof surface plasmons were also demonstrated for metallic disks in microwave frequencies 16 17 See also editPhotonic crystal Plasmonic metamaterial Split ring resonator Superlens Terahertz metamaterialReferences edit Garcia Vidal Francisco J Fernandez Dominguez Antonio I Martin Moreno Luis Zhang Hao Chi Tang Wenxuan Peng Ruwen Cui Tie Jun 2022 Spoof surface plasmon photonics Reviews of Modern Physics 04 2 025004 Bibcode 2022RvMP 94b5004G doi 10 1103 RevModPhys 94 025004 hdl 10261 280707 S2CID 248954068 a b Tang Wen Xuan Zhang Hao Chi Ma Hui Feng Jiang Wei Xiang et al 4 January 2019 Concept Theory Design and Applications of Spoof Surface Plasmon Polaritons at Microwave Frequencies Advanced Optical Materials 7 1 1800421 doi 10 1002 adom 201800421 a b Maier Stefan A 2007 Plasmonics Fundamentals and Applications New York Springer Publishing ISBN 978 0 387 33150 8 a b c d Pendry J B Holden A J Stewart W J Youngs I June 1996 Extremely Low Frequency Plasmons in Metallic Mesostructures Physical Review Letters 46 25 4773 4776 Bibcode 1996PhRvL 76 4773P doi 10 1103 PhysRevLett 76 4773 PMID 10061377 a b Pendry J B Martin Moreno L Garcia Vidal F J 6 August 2004 Mimicking Surface Plasmons with Structured Surfaces Science 305 5685 847 848 Bibcode 2004Sci 305 847P doi 10 1126 science 1098999 PMID 15247438 S2CID 44412157 a b Garcia Vidal F J Martin Moreno L Pendry J B January 2005 Surfaces with holes in them new plasmonic metamaterials Journal of Optics A 7 2 S97 S101 Bibcode 2005JOptA 7S 97G doi 10 1088 1464 4258 7 2 013 Liu Xiaoyong Feng Yijun Zhu Bo Zhao Junming Jiang Tian February 2016 Backward spoof surface wave in plasmonic metamaterial of ultrathin metallic structure Scientific Reports 6 6 20448 Bibcode 2016NatSR 620448L doi 10 1038 srep20448 PMC 4740866 PMID 26842340 Maier Stefan A Andrews Steve R June 2006 Terahertz pulse propagation using plasmon polariton like surface modes on structured conductive surfaces Applied Physics Letters 88 25 251120 Bibcode 2006ApPhL 88y1120M doi 10 1063 1 2216105 Martin Cano D Nesterov M L Fernandez Dominguez A I Garcia Vidal F J Martin Moreno L Moreno Esteban 2010 Domino plasmons for subwavelength terahertz circuitry Optics Express 18 2 754 764 arXiv 0911 4525 Bibcode 2010OExpr 18 754M doi 10 1364 OE 18 000754 hdl 10261 47867 PMID 20173896 S2CID 2299072 Yu Nanfang Wang Qi Jie Kats Mikhail A Capasso Federico et al August 2010 Designer spoof surface plasmon structures collimate terahertz laser beams Nature Materials 9 9 730 735 Bibcode 2010NatMa 9 730Y doi 10 1038 nmat2822 PMID 20693995 Ma Hui Feng Shen Xiaopeng Cheng Qiang Jiang Wei Xiang et al November 2013 Broadband and high efficiency conversion from guided waves to spoof surface plasmon polaritons Laser amp Photonics Reviews 8 1 146 151 doi 10 1002 lpor 201300118 S2CID 120708454 Zhang Hao Chi Liu Shuo Shen Xiaopeng Chen Lin Hui et al November 2014 Broadband amplification of spoof surface plasmon polaritons at microwave frequencies Laser amp Photonics Reviews 9 1 83 90 doi 10 1002 lpor 201400131 S2CID 118667968 Kianinejad Amin Chen Zhi Ning Qiu Cheng Wei June 2015 Design and Modeling of Spoof Surface Plasmon Modes Based Microwave Slow Wave Transmission Line IEEE Transactions on Microwave Theory and Techniques 63 6 1817 1825 Bibcode 2015ITMTT 63 1817K doi 10 1109 TMTT 2015 2422694 S2CID 16388137 Khanikaev Alexander B Mousavi S Hossein Shvets Gennady Kivshar Yuri S September 2010 One Way Extraordinary Optical Transmission and Nonreciprocal Spoof Plasmons Physical Review Letters 105 12 17 126804 Bibcode 2010PhRvL 105l6804K doi 10 1103 PhysRevLett 105 126804 PMID 20867667 Pan Bai Cao Liao Zhen Zhao Jie Cui Tie Jun 2014 Controlling rejections of spoof surface plasmon polaritons using metamaterial particles Optics Express 22 11 13940 13950 Bibcode 2014OExpr 2213940P doi 10 1364 OE 22 013940 PMID 24921585 Shen Xiaopeng Cui Tie Jun January 2014 Ultrathin plasmonic metamaterial for spoof localized surface plasmons Laser amp Photonics Reviews 8 1 137 145 Bibcode 2014LPRv 8 137S doi 10 1002 lpor 201300144 S2CID 118085394 Huidobro Paloma A Shen Xiaopeng Cuerda J Moreno Esteban et al April 2014 Magnetic Localized Surface Plasmons Physical Review X 4 2 021003 Bibcode 2014PhRvX 4b1003H doi 10 1103 PhysRevX 4 021003 Further reading editHuidobro Paloma Arroyo Fernandez Dominguez Antonio I Pendry John B Martin Moreno Luis Garcia Vidal Francisco J January 2018 Spoof Surface Plasmon Metamaterials Cambridge University Press doi 10 1017 9781108553445 ISBN 9781108553445 S2CID 139524223 Retrieved from https en wikipedia org w index php title Spoof surface plasmon amp oldid 1189346640, wikipedia, wiki, book, books, library,

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