Abstract

Bloch surface wave (BSW) can be considered as the dielectric analogue of surface plasmon polariton (SPP) with less loss since it is sustained at the surface of a truncated dielectric multilayer. As dielectric materials show nearly no ohmic loss, BSW can propagates much farther compared to SPP, and thus is beneficial for planar optical devices. In this paper, we study the spin-orbital interaction between incident beam and BSW. We demonstrate that due to the spin-orbital coupling, the near-field properties of generated BSW can be controlled with a meta-antenna structure. The meta-antenna is composed of two gold nano-antennas oriented at 45° and 135° as a near-field coupler. By careful design of the meta-antenna, the generated BSW can be guided and focused depending on the chirality of the incident beam. Three examples of meta-antennas are demonstrated for chiral sensitive focusing, directional switching and asymmetric focusing. The proposed method can be applied as a design method for low-loss on-chip photonic devices.

© 2019 Optical Society of America under the terms of the OSA Open Access Publishing Agreement

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2019 (1)

L. Sun, C.-Y. Wang, A. Krasnok, J. Choi, J. Shi, G.-D. Joseph, A. Zepeda, S. Gwo, C.-K. Shih, A. Alu, and X. Li, “Separation of valley excitons in MoS2 monolayer using a subwavelength asymmetric groove array,” Photonics 13(3), 180–184 (2019).
[Crossref]

2018 (5)

M. Wang, H. Zhang, T. Kovalevich, R. Salut, M.-S. Kim, M.-A. Suarez, M.-P. Bernal, H.-P. Herzig, H. Lu, and T. Grosjean, “Magnetic spin–orbit interaction of light,” Light: Sci. Appl. 7(1), 24 (2018).
[Crossref]

L. L. Doskolovich, E. A. Bezus, and D. A. Bykov, “Two-groove narrowband transmission filter integrated into a slab waveguide,” Photonics Res. 6(1), 61–65 (2018).
[Crossref]

E. A. Bezus, L. L. Doskolovich, D. A. Bykov, and V. A. Soifer, “Spatial integration and differentiation of optical beams in a slab waveguide by a dielectric ridge supporting high-Q resonances,” Opt. Express 26(19), 25156–25165 (2018).
[Crossref]

R. Wang, J. Chen, Y. Xiang, Y. Kuai, P. Wang, H. Ming, J. R. Lakowicz, and D.-G. Zhang, “Two-Dimensional Photonic Devices based on Bloch Surface Waves with One-Dimensional Grooves,” Phys. Rev. Appl. 10(2), 024032 (2018).
[Crossref]

X. Lei, Y. Ren, Y. Lu, and P. Wang, “Lens for Efficient Focusing of Bloch Surface Waves,” Phys. Rev. Appl. 10(4), 044032 (2018).
[Crossref]

2017 (4)

R. Wang, Y. Wang, D. Zhang, G. Si, L. Zhu, L. Du, S. Kou, R. Badugu, M. Rosenfeld, J. Lin, P. Wang, H. Ming, X. Yuan, and J. R. Lakowicz, “Diffraction free Bloch surface wave,” ACS Nano 11(6), 5383–5390 (2017).
[Crossref]

W. Choi, Y. Jo, J. Ahn, E. Seo, Q.-H. Park, Y. M. Jhon, and W. Choi, “Control of randomly scattered surface plasmon polaritons for multiple-input and multiple-output plasmonic switching devices,” Nat. Commun. 8(1), 14636 (2017).
[Crossref]

A. L. Lereu, M. Zerrad, A. Passian, and C. Amra, “Surface plasmons and Bloch surface waves: Towards optimized ultra-sensitive optical sensors,” Appl. Phys. Lett. 111(1), 011107 (2017).
[Crossref]

R. Wang, H. Xia, D. Zhang, J. Chen, L. Zhu, Y. Wang, E. Yang, T. Zang, X. Wen, G. Zou, P. Wang, H. Ming, R. Badugu, and J. R. Lakowicz, “Bloch surface waves confined in one dimension with a single polymeric nanofibre,” Nat. Commun. 8(1), 14330 (2017).
[Crossref]

2016 (1)

C. Caucheteur, T. Guo, F. Liu, B.-O. Guan, and J. Albert, “Ultrasensitive plasmonic sensing in air using optical fibre spectral combs,” Nat. Commun. 7(1), 13371 (2016).
[Crossref]

2015 (2)

K. Y. Bliokh, F. J. Rodriguez-Fortuno, F. Noril, and A. V. Zayats, “Spin–orbit interactions of light,” Nat,” Photonics 9(12), 796–808 (2015).
[Crossref]

S.-Y. Lee, K. Kim, S.-J. Kim, H. Park, K.-Y. Kim, and B. Lee, “Plasmonic meta-slit: shaping and controlling near-field focus,” Optica 2(1), 6–13 (2015).
[Crossref]

2014 (1)

G. Calafiore, A. Koshelev, S. Dhuey, A. Goltsov, P. Sasorov, S. Babin, V. Yankov, S. Cabrini, and C. Peroz, “Holographic planar lightwave circuit for on-chip spectroscopy,” Light: Sci. Appl. 3(9), e203 (2014).
[Crossref]

2013 (4)

J. Lin, J. P. Mueller, Q. Wang, G. Yuan, N. Antoniou, X.-C. Yuan, and F. Capasso, “Polarization-controlled tunable directional coupling of surface plasmon polaritons,” Science 340(6130), 331–334 (2013).
[Crossref]

N. Rotenberg, T. L. Krijger, B. le Feber, M. Spasenovic, F. J. Garcia de Abajo, and L. Kuipers, “Magnetic and electric response of single subwavelength holes,” Phys. Rev. B 88(24), 241408 (2013).
[Crossref]

C. Min, Z. Shen, J. Shen, Y. Zhang, H. Fang, G. Yuan, L. Du, S. Zhu, T. Lei, and X. Yuan, “Focused plasmonic trapping of metallic particles,” Nat. Commun. 4(1), 2891 (2013).
[Crossref]

J. Leuthold, C. Hoessbacher, S. Muehlbrandt, A. Melikyan, M. Kohl, C. Koos, W. Freude, V. Dolores-Calzadilla, M. Smit, I. Suarez, J. Martínez-Pastor, E. P. Fitrakis, and I. Tomkos, “Plasmonic communications: Light on a wire,” Opt. Photonics News 24(5), 28–35 (2013).
[Crossref]

2012 (4)

D. Lu and Z. Liu, “Hyperlenses and metalenses for far-field super-resolution imaging,” Nat. Commun. 3(1), 1205 (2012).
[Crossref]

M. Kang, T. Feng, H.-T. Wang, and J. Li, “Wave front engineering from an array of thin aperture antennas,” Opt. Express 20(14), 15882–15890 (2012).
[Crossref]

L. Huang, X. Chen, H. Muhlenbernd, G. Li, B. Bai, Q. Tan, G. Jin, T. Zentgraf, and S. Zhang, “Dispersionless phase discontinuities for controlling light propagation,” Nano Lett. 12(11), 5750–5755 (2012).
[Crossref]

C. Peroz, C. Calo, A. Goltsov, S. Dhuey, A. Koshelev, P. Sasorov, I. Ivonin, S. Babin, S. Cabrini, and V. Yankov, “Multiband wavelength demultiplexer based on digital planar holography for on-chip spectroscopy applications,” Opt. Lett. 37(4), 695–697 (2012).
[Crossref]

2011 (2)

K. Wang, E. Schonbrun, P. Steinvurzel, and K. B. Crozier, “Trapping and rotating nanoparticles using a plasmonic nano-tweezer with an integrated heat sink,” Nat. Commun. 2(1), 469 (2011).
[Crossref]

G. W. Webb, I. V. Minin, and O. V. Minin, “Variable Reference Phase in Diffractive Antennas,” IEEE Antennas Propag. Mag. 53(2), 77–94 (2011).
[Crossref]

2010 (2)

B. C. Stipe, T. C. Strand, C. C. Poon, H. Balamane, T. D. Boone, J. A. Katine, J.-L. Li, V. Rawat, H. Nemoto, A. Hirotsune, O. Hellwig, R. Ruiz, E. Dobisz, D. S. Kercher, N. Robertson, T. R. Albrecht, and B. D. Terris, “Magnetic recording at 1.5 Pb m−2 using an integrated plasmonic antenna,” Nat. Photonics 4(7), 484–488 (2010).
[Crossref]

D. O’Connor and A. V. Zayats, “Data storage: The third plasmonic revolution,” Nat. Nanotechnol. 5(7), 482–483 (2010).
[Crossref]

2009 (2)

I. Soboleva, E. Descrovi, C. Summonte, A. Fedyanin, and F. Giorgis, “Fluorescence emission enhanced by surface electromagnetic waves on one-dimensional photonic crystals,” Appl. Phys. Lett. 94(23), 231122 (2009).
[Crossref]

S. Babin, A. Bugrov, S. Cabrini, S. Dhuey, A. Goltsov, I. Ivonin, E.-B. Kley, C. Peroz, H. Schmidt, and V. Yankov, “Digital optical spectrometer-on-chip,” Appl. Phys. Lett. 95(4), 041105 (2009).
[Crossref]

2007 (2)

G. Lévêque, O. J. F. Martin, and J. Weiner, “Transient behavior of surface plasmon polaritons scattered at a subwavelength groove,” Phys. Rev. B 76(15), 155418 (2007).
[Crossref]

E. Descrovi, F. Frascella, B. Sciacca, F. Geobaldo, L. Dominici, and F. Michelotti, “Coupling of surface waves in highly defined one-dimensional porous silicon photonic crystals for gas sensing applications,” Appl. Phys. Lett. 91(24), 241109 (2007).
[Crossref]

2006 (2)

S. I. Bozhevolnyi, V. S. Volkov, E. Devaux, J.-Y. Laluet, and T. W. Ebbesen, “Channel plasmon subwavelength waveguide components including interferometers and ring resonators,” Nature 440(7083), 508–511 (2006).
[Crossref]

E. Ozbay, “Plasmonics: Merging photonics and electronics at nanoscale dimensions,” Science 311(5758), 189–193 (2006).
[Crossref]

2005 (1)

N. Fang, H. Lee, C. Sun, and X. Zhang, “Sub–diffraction-limited optical imaging with a silver superlens,” Science 308(5721), 534–537 (2005).
[Crossref]

2001 (1)

1977 (1)

Ahn, J.

W. Choi, Y. Jo, J. Ahn, E. Seo, Q.-H. Park, Y. M. Jhon, and W. Choi, “Control of randomly scattered surface plasmon polaritons for multiple-input and multiple-output plasmonic switching devices,” Nat. Commun. 8(1), 14636 (2017).
[Crossref]

Albert, J.

C. Caucheteur, T. Guo, F. Liu, B.-O. Guan, and J. Albert, “Ultrasensitive plasmonic sensing in air using optical fibre spectral combs,” Nat. Commun. 7(1), 13371 (2016).
[Crossref]

Albrecht, T. R.

B. C. Stipe, T. C. Strand, C. C. Poon, H. Balamane, T. D. Boone, J. A. Katine, J.-L. Li, V. Rawat, H. Nemoto, A. Hirotsune, O. Hellwig, R. Ruiz, E. Dobisz, D. S. Kercher, N. Robertson, T. R. Albrecht, and B. D. Terris, “Magnetic recording at 1.5 Pb m−2 using an integrated plasmonic antenna,” Nat. Photonics 4(7), 484–488 (2010).
[Crossref]

Alu, A.

L. Sun, C.-Y. Wang, A. Krasnok, J. Choi, J. Shi, G.-D. Joseph, A. Zepeda, S. Gwo, C.-K. Shih, A. Alu, and X. Li, “Separation of valley excitons in MoS2 monolayer using a subwavelength asymmetric groove array,” Photonics 13(3), 180–184 (2019).
[Crossref]

Amra, C.

A. L. Lereu, M. Zerrad, A. Passian, and C. Amra, “Surface plasmons and Bloch surface waves: Towards optimized ultra-sensitive optical sensors,” Appl. Phys. Lett. 111(1), 011107 (2017).
[Crossref]

Antoniou, N.

J. Lin, J. P. Mueller, Q. Wang, G. Yuan, N. Antoniou, X.-C. Yuan, and F. Capasso, “Polarization-controlled tunable directional coupling of surface plasmon polaritons,” Science 340(6130), 331–334 (2013).
[Crossref]

Babin, S.

G. Calafiore, A. Koshelev, S. Dhuey, A. Goltsov, P. Sasorov, S. Babin, V. Yankov, S. Cabrini, and C. Peroz, “Holographic planar lightwave circuit for on-chip spectroscopy,” Light: Sci. Appl. 3(9), e203 (2014).
[Crossref]

C. Peroz, C. Calo, A. Goltsov, S. Dhuey, A. Koshelev, P. Sasorov, I. Ivonin, S. Babin, S. Cabrini, and V. Yankov, “Multiband wavelength demultiplexer based on digital planar holography for on-chip spectroscopy applications,” Opt. Lett. 37(4), 695–697 (2012).
[Crossref]

S. Babin, A. Bugrov, S. Cabrini, S. Dhuey, A. Goltsov, I. Ivonin, E.-B. Kley, C. Peroz, H. Schmidt, and V. Yankov, “Digital optical spectrometer-on-chip,” Appl. Phys. Lett. 95(4), 041105 (2009).
[Crossref]

Badugu, R.

R. Wang, H. Xia, D. Zhang, J. Chen, L. Zhu, Y. Wang, E. Yang, T. Zang, X. Wen, G. Zou, P. Wang, H. Ming, R. Badugu, and J. R. Lakowicz, “Bloch surface waves confined in one dimension with a single polymeric nanofibre,” Nat. Commun. 8(1), 14330 (2017).
[Crossref]

R. Wang, Y. Wang, D. Zhang, G. Si, L. Zhu, L. Du, S. Kou, R. Badugu, M. Rosenfeld, J. Lin, P. Wang, H. Ming, X. Yuan, and J. R. Lakowicz, “Diffraction free Bloch surface wave,” ACS Nano 11(6), 5383–5390 (2017).
[Crossref]

Bai, B.

L. Huang, X. Chen, H. Muhlenbernd, G. Li, B. Bai, Q. Tan, G. Jin, T. Zentgraf, and S. Zhang, “Dispersionless phase discontinuities for controlling light propagation,” Nano Lett. 12(11), 5750–5755 (2012).
[Crossref]

Balamane, H.

B. C. Stipe, T. C. Strand, C. C. Poon, H. Balamane, T. D. Boone, J. A. Katine, J.-L. Li, V. Rawat, H. Nemoto, A. Hirotsune, O. Hellwig, R. Ruiz, E. Dobisz, D. S. Kercher, N. Robertson, T. R. Albrecht, and B. D. Terris, “Magnetic recording at 1.5 Pb m−2 using an integrated plasmonic antenna,” Nat. Photonics 4(7), 484–488 (2010).
[Crossref]

Bernal, M.-P.

M. Wang, H. Zhang, T. Kovalevich, R. Salut, M.-S. Kim, M.-A. Suarez, M.-P. Bernal, H.-P. Herzig, H. Lu, and T. Grosjean, “Magnetic spin–orbit interaction of light,” Light: Sci. Appl. 7(1), 24 (2018).
[Crossref]

Bezus, E. A.

Bliokh, K. Y.

K. Y. Bliokh, F. J. Rodriguez-Fortuno, F. Noril, and A. V. Zayats, “Spin–orbit interactions of light,” Nat,” Photonics 9(12), 796–808 (2015).
[Crossref]

Boone, T. D.

B. C. Stipe, T. C. Strand, C. C. Poon, H. Balamane, T. D. Boone, J. A. Katine, J.-L. Li, V. Rawat, H. Nemoto, A. Hirotsune, O. Hellwig, R. Ruiz, E. Dobisz, D. S. Kercher, N. Robertson, T. R. Albrecht, and B. D. Terris, “Magnetic recording at 1.5 Pb m−2 using an integrated plasmonic antenna,” Nat. Photonics 4(7), 484–488 (2010).
[Crossref]

Bozhevolnyi, S. I.

S. I. Bozhevolnyi, V. S. Volkov, E. Devaux, J.-Y. Laluet, and T. W. Ebbesen, “Channel plasmon subwavelength waveguide components including interferometers and ring resonators,” Nature 440(7083), 508–511 (2006).
[Crossref]

Bugrov, A.

S. Babin, A. Bugrov, S. Cabrini, S. Dhuey, A. Goltsov, I. Ivonin, E.-B. Kley, C. Peroz, H. Schmidt, and V. Yankov, “Digital optical spectrometer-on-chip,” Appl. Phys. Lett. 95(4), 041105 (2009).
[Crossref]

Bykov, D. A.

Cabrini, S.

G. Calafiore, A. Koshelev, S. Dhuey, A. Goltsov, P. Sasorov, S. Babin, V. Yankov, S. Cabrini, and C. Peroz, “Holographic planar lightwave circuit for on-chip spectroscopy,” Light: Sci. Appl. 3(9), e203 (2014).
[Crossref]

C. Peroz, C. Calo, A. Goltsov, S. Dhuey, A. Koshelev, P. Sasorov, I. Ivonin, S. Babin, S. Cabrini, and V. Yankov, “Multiband wavelength demultiplexer based on digital planar holography for on-chip spectroscopy applications,” Opt. Lett. 37(4), 695–697 (2012).
[Crossref]

S. Babin, A. Bugrov, S. Cabrini, S. Dhuey, A. Goltsov, I. Ivonin, E.-B. Kley, C. Peroz, H. Schmidt, and V. Yankov, “Digital optical spectrometer-on-chip,” Appl. Phys. Lett. 95(4), 041105 (2009).
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C. Min, Z. Shen, J. Shen, Y. Zhang, H. Fang, G. Yuan, L. Du, S. Zhu, T. Lei, and X. Yuan, “Focused plasmonic trapping of metallic particles,” Nat. Commun. 4(1), 2891 (2013).
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J. Lin, J. P. Mueller, Q. Wang, G. Yuan, N. Antoniou, X.-C. Yuan, and F. Capasso, “Polarization-controlled tunable directional coupling of surface plasmon polaritons,” Science 340(6130), 331–334 (2013).
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K. Y. Bliokh, F. J. Rodriguez-Fortuno, F. Noril, and A. V. Zayats, “Spin–orbit interactions of light,” Nat,” Photonics 9(12), 796–808 (2015).
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D. O’Connor and A. V. Zayats, “Data storage: The third plasmonic revolution,” Nat. Nanotechnol. 5(7), 482–483 (2010).
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L. Huang, X. Chen, H. Muhlenbernd, G. Li, B. Bai, Q. Tan, G. Jin, T. Zentgraf, and S. Zhang, “Dispersionless phase discontinuities for controlling light propagation,” Nano Lett. 12(11), 5750–5755 (2012).
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L. Sun, C.-Y. Wang, A. Krasnok, J. Choi, J. Shi, G.-D. Joseph, A. Zepeda, S. Gwo, C.-K. Shih, A. Alu, and X. Li, “Separation of valley excitons in MoS2 monolayer using a subwavelength asymmetric groove array,” Photonics 13(3), 180–184 (2019).
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R. Wang, Y. Wang, D. Zhang, G. Si, L. Zhu, L. Du, S. Kou, R. Badugu, M. Rosenfeld, J. Lin, P. Wang, H. Ming, X. Yuan, and J. R. Lakowicz, “Diffraction free Bloch surface wave,” ACS Nano 11(6), 5383–5390 (2017).
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R. Wang, J. Chen, Y. Xiang, Y. Kuai, P. Wang, H. Ming, J. R. Lakowicz, and D.-G. Zhang, “Two-Dimensional Photonic Devices based on Bloch Surface Waves with One-Dimensional Grooves,” Phys. Rev. Appl. 10(2), 024032 (2018).
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L. Huang, X. Chen, H. Muhlenbernd, G. Li, B. Bai, Q. Tan, G. Jin, T. Zentgraf, and S. Zhang, “Dispersionless phase discontinuities for controlling light propagation,” Nano Lett. 12(11), 5750–5755 (2012).
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Zhang, X.

N. Fang, H. Lee, C. Sun, and X. Zhang, “Sub–diffraction-limited optical imaging with a silver superlens,” Science 308(5721), 534–537 (2005).
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Zhang, Y.

C. Min, Z. Shen, J. Shen, Y. Zhang, H. Fang, G. Yuan, L. Du, S. Zhu, T. Lei, and X. Yuan, “Focused plasmonic trapping of metallic particles,” Nat. Commun. 4(1), 2891 (2013).
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Zhu, L.

R. Wang, Y. Wang, D. Zhang, G. Si, L. Zhu, L. Du, S. Kou, R. Badugu, M. Rosenfeld, J. Lin, P. Wang, H. Ming, X. Yuan, and J. R. Lakowicz, “Diffraction free Bloch surface wave,” ACS Nano 11(6), 5383–5390 (2017).
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Zhu, S.

C. Min, Z. Shen, J. Shen, Y. Zhang, H. Fang, G. Yuan, L. Du, S. Zhu, T. Lei, and X. Yuan, “Focused plasmonic trapping of metallic particles,” Nat. Commun. 4(1), 2891 (2013).
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R. Wang, H. Xia, D. Zhang, J. Chen, L. Zhu, Y. Wang, E. Yang, T. Zang, X. Wen, G. Zou, P. Wang, H. Ming, R. Badugu, and J. R. Lakowicz, “Bloch surface waves confined in one dimension with a single polymeric nanofibre,” Nat. Commun. 8(1), 14330 (2017).
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ACS Nano (1)

R. Wang, Y. Wang, D. Zhang, G. Si, L. Zhu, L. Du, S. Kou, R. Badugu, M. Rosenfeld, J. Lin, P. Wang, H. Ming, X. Yuan, and J. R. Lakowicz, “Diffraction free Bloch surface wave,” ACS Nano 11(6), 5383–5390 (2017).
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G. Calafiore, A. Koshelev, S. Dhuey, A. Goltsov, P. Sasorov, S. Babin, V. Yankov, S. Cabrini, and C. Peroz, “Holographic planar lightwave circuit for on-chip spectroscopy,” Light: Sci. Appl. 3(9), e203 (2014).
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M. Wang, H. Zhang, T. Kovalevich, R. Salut, M.-S. Kim, M.-A. Suarez, M.-P. Bernal, H.-P. Herzig, H. Lu, and T. Grosjean, “Magnetic spin–orbit interaction of light,” Light: Sci. Appl. 7(1), 24 (2018).
[Crossref]

Nano Lett. (1)

L. Huang, X. Chen, H. Muhlenbernd, G. Li, B. Bai, Q. Tan, G. Jin, T. Zentgraf, and S. Zhang, “Dispersionless phase discontinuities for controlling light propagation,” Nano Lett. 12(11), 5750–5755 (2012).
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R. Wang, H. Xia, D. Zhang, J. Chen, L. Zhu, Y. Wang, E. Yang, T. Zang, X. Wen, G. Zou, P. Wang, H. Ming, R. Badugu, and J. R. Lakowicz, “Bloch surface waves confined in one dimension with a single polymeric nanofibre,” Nat. Commun. 8(1), 14330 (2017).
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W. Choi, Y. Jo, J. Ahn, E. Seo, Q.-H. Park, Y. M. Jhon, and W. Choi, “Control of randomly scattered surface plasmon polaritons for multiple-input and multiple-output plasmonic switching devices,” Nat. Commun. 8(1), 14636 (2017).
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C. Caucheteur, T. Guo, F. Liu, B.-O. Guan, and J. Albert, “Ultrasensitive plasmonic sensing in air using optical fibre spectral combs,” Nat. Commun. 7(1), 13371 (2016).
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D. Lu and Z. Liu, “Hyperlenses and metalenses for far-field super-resolution imaging,” Nat. Commun. 3(1), 1205 (2012).
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C. Min, Z. Shen, J. Shen, Y. Zhang, H. Fang, G. Yuan, L. Du, S. Zhu, T. Lei, and X. Yuan, “Focused plasmonic trapping of metallic particles,” Nat. Commun. 4(1), 2891 (2013).
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K. Wang, E. Schonbrun, P. Steinvurzel, and K. B. Crozier, “Trapping and rotating nanoparticles using a plasmonic nano-tweezer with an integrated heat sink,” Nat. Commun. 2(1), 469 (2011).
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Nat. Nanotechnol. (1)

D. O’Connor and A. V. Zayats, “Data storage: The third plasmonic revolution,” Nat. Nanotechnol. 5(7), 482–483 (2010).
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B. C. Stipe, T. C. Strand, C. C. Poon, H. Balamane, T. D. Boone, J. A. Katine, J.-L. Li, V. Rawat, H. Nemoto, A. Hirotsune, O. Hellwig, R. Ruiz, E. Dobisz, D. S. Kercher, N. Robertson, T. R. Albrecht, and B. D. Terris, “Magnetic recording at 1.5 Pb m−2 using an integrated plasmonic antenna,” Nat. Photonics 4(7), 484–488 (2010).
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Optica (1)

Photonics (2)

L. Sun, C.-Y. Wang, A. Krasnok, J. Choi, J. Shi, G.-D. Joseph, A. Zepeda, S. Gwo, C.-K. Shih, A. Alu, and X. Li, “Separation of valley excitons in MoS2 monolayer using a subwavelength asymmetric groove array,” Photonics 13(3), 180–184 (2019).
[Crossref]

K. Y. Bliokh, F. J. Rodriguez-Fortuno, F. Noril, and A. V. Zayats, “Spin–orbit interactions of light,” Nat,” Photonics 9(12), 796–808 (2015).
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Figures (5)

Fig. 1.
Fig. 1. (a) Schematic presentation of BSW substrate with a gold nano-antenna laid on top along X axis under light excitation, the generated BSW propagates along Y axis and thus can be described by Hy, Hz and Ex components; (b) Dispersion relation of BSW structure described by reflectivity as a function of incident angle of a plane wave illuminating from the bottom, whose two modes located at 62.8° and 66.1° are corresponding to BSW mode and guided mode, respectively. The dashed line indicates the 633nm wavelength.
Fig. 2.
Fig. 2. (a) Up: Schematic presentation of a single 250nm×50nm×50nm nano-antenna following Y axis laying on the BSW substrate under excitation; Down: |Hz| field distribution of BSW excited when the linear polarization of incident beam is set to X(left) and Y(right), respectively; (b) Angular distribution of BSW as (a), blue and red curve represent BSW generated by incident beam with X and Y polarization respectively. The BSW intensity generated by X polarized light is amplified for 20 times for clarity.
Fig. 3.
Fig. 3. (a) Distribution of real part of Hz of an individual nano-antenna oriented at 45° and 135° under LCP excitation; (b) Schematic presentation of a double-line meta-antenna composed of a 135° nano-antenna on the left (line A) and a 45° nano-antenna on the right (line B). Horizontally the distance between the two nano-antennas is D, and vertically the nano-antenna pairs are repeated by a period of d, the number of meta-antenna pairs can be chosen according to different applications; (c)–(d) Intensity field distribution of 9 double line meta-antenna under LCP and RCP excitation, respectively. The beam is incident normally from the top. D and d are set to be 1/4 λbsw and 300nm, respectively. The distance between adjacent meta-antenna pairs is set to be 2λbsw. The positions and orientations of the nano-antennas are schematically presented by golden sticks on white background in the center of the figures. The background is white because the electric field saturate in the center.
Fig. 4.
Fig. 4. (a) Schematic presentation of meta-antenna integrated with FZP under circular polarized light incident beam excitation, the integration of FZP is simply by removing the nano-antennas fall into R1 < R < R2 (named “dark zone”, same operations should be applied for higher orders); (b) - (c) Intensity profile of meta-antenna integrated with FZP under LCP/RCP incident excitation respectively.
Fig. 5.
Fig. 5. (a) Schematic presentation of Type I, II, III (brown, blue, green) meta-antenna; (b) Schematic presentation of design protocol of asymmetric focusing hybrid FZP lens; (c) - (d) Intensity field distribution of designed hybrid FZP under LCP and RCP excitation, respectively.

Equations (7)

Equations on this page are rendered with MathJax. Learn more.

E l c p = E x + i E y ,
p = | E x | cos ( α ) + i | E y | sin ( α ) = E 0 exp ( i α ) ,
E ( r ) = i ω μ 0 m = 1 N ( G 0 ( r , r m ) + G σ ( r , r m ) ) P ( r r m ) e i φ m ,
E ( x , y ) = A ( α ) e i φ α e i k | x | ,
E T a r g e t = E A exp ( i k x ) + E B exp ( i k ( x + D ) ) ,
E T a r g e t = E A exp ( i k x ) + E A exp [ i k ( x + D ) π 2 ] = A ( α ) e i α e i k x [ 1 + e i ( k D π 2 ) ] .
R m = m f λ B S W + λ B S W 2 m 2 4 ,

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