Plasmon polaritons in photonic superlattices containing a left-handed material
ABSTRACT: We analyze one-dimensional photonic superlattices which alternate layers of air and a left-handed material. We assume Drude-type dispersive responses for the dielectric permittivity and magnetic permeability of the left-handed material. Maxwell’s equations and the transfermatrix technique...
- Autores:
-
Reyes Gómez, Ernesto Amador
Mogilevtsev, D.
Cavalcanti, Solange Bessa
de Carvalho, C. A. A.
Oliveira, Luiz Eduardo
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2009
- Institución:
- Universidad de Antioquia
- Repositorio:
- Repositorio UdeA
- Idioma:
- eng
- OAI Identifier:
- oai:bibliotecadigital.udea.edu.co:10495/8401
- Acceso en línea:
- http://hdl.handle.net/10495/8401
- Palabra clave:
- Plasmón
Polaritón
Superláquidos fotónicos
- Rights
- openAccess
- License
- Atribución-NoComercial-SinDerivadas 2.5 Colombia
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| dc.title.spa.fl_str_mv |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| title |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| spellingShingle |
Plasmon polaritons in photonic superlattices containing a left-handed material Plasmón Polaritón Superláquidos fotónicos |
| title_short |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| title_full |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| title_fullStr |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| title_full_unstemmed |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| title_sort |
Plasmon polaritons in photonic superlattices containing a left-handed material |
| dc.creator.fl_str_mv |
Reyes Gómez, Ernesto Amador Mogilevtsev, D. Cavalcanti, Solange Bessa de Carvalho, C. A. A. Oliveira, Luiz Eduardo |
| dc.contributor.author.none.fl_str_mv |
Reyes Gómez, Ernesto Amador Mogilevtsev, D. Cavalcanti, Solange Bessa de Carvalho, C. A. A. Oliveira, Luiz Eduardo |
| dc.subject.none.fl_str_mv |
Plasmón Polaritón Superláquidos fotónicos |
| topic |
Plasmón Polaritón Superláquidos fotónicos |
| description |
ABSTRACT: We analyze one-dimensional photonic superlattices which alternate layers of air and a left-handed material. We assume Drude-type dispersive responses for the dielectric permittivity and magnetic permeability of the left-handed material. Maxwell’s equations and the transfermatrix technique are used to derive the dispersion relation and transmission spectra for the propagation of obliquely incident optical fields. The photonic dispersion indicates that the growth direction component of the electric (or magnetic) field leads to the propagation of electric (or magnetic) plasmon polaritons, for either TE or TM configurations. Furthermore, we show that if the plasma frequency is chosen within the photonic (n(ω)) =0 zeroth-order bandgap, the coupling of light with plasmons weakens considerably. As light propagation is forbidden in that particular frequency region, the plasmon-polariton mode reduces to a pure plasmon mode |
| publishDate |
2009 |
| dc.date.issued.none.fl_str_mv |
2009 |
| dc.date.accessioned.none.fl_str_mv |
2017-09-28T19:46:48Z |
| dc.date.available.none.fl_str_mv |
2017-09-28T19:46:48Z |
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info:eu-repo/semantics/article |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 |
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Artículo de investigación |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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publishedVersion |
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Reyes Gómez, E. A., Mogilevtsev, D., Cavalcanti, S. B., de Carvalho, C. A. A., & Oliveira, L. E. (2009). Plasmon polaritons in photonic superlattices containing a left-handed material. EPL, 88(24002), 1-6. DOI:10.1209/0295-5075/88/24002 |
| dc.identifier.issn.none.fl_str_mv |
0295-5075 |
| dc.identifier.uri.none.fl_str_mv |
http://hdl.handle.net/10495/8401 |
| dc.identifier.doi.none.fl_str_mv |
10.1209/0295-5075/88/24002 |
| dc.identifier.eissn.none.fl_str_mv |
1286-4854 |
| identifier_str_mv |
Reyes Gómez, E. A., Mogilevtsev, D., Cavalcanti, S. B., de Carvalho, C. A. A., & Oliveira, L. E. (2009). Plasmon polaritons in photonic superlattices containing a left-handed material. EPL, 88(24002), 1-6. DOI:10.1209/0295-5075/88/24002 0295-5075 10.1209/0295-5075/88/24002 1286-4854 |
| url |
http://hdl.handle.net/10495/8401 |
| dc.language.iso.spa.fl_str_mv |
eng |
| language |
eng |
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Atribución-NoComercial-SinDerivadas 2.5 Colombia |
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info:eu-repo/semantics/openAccess |
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http://creativecommons.org/licenses/by-nc-nd/2.5/co/ |
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http://purl.org/coar/access_right/c_abf2 |
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https://creativecommons.org/licenses/by-nc-nd/4.0/ |
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Atribución-NoComercial-SinDerivadas 2.5 Colombia http://creativecommons.org/licenses/by-nc-nd/2.5/co/ http://purl.org/coar/access_right/c_abf2 https://creativecommons.org/licenses/by-nc-nd/4.0/ |
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openAccess |
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application/pdf |
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Institute of Physics Publishing (IOP) |
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Universidad de Antioquia |
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andres.perez@udea.edu.co |
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Reyes Gómez, Ernesto AmadorMogilevtsev, D.Cavalcanti, Solange Bessade Carvalho, C. A. A.Oliveira, Luiz Eduardo2017-09-28T19:46:48Z2017-09-28T19:46:48Z2009Reyes Gómez, E. A., Mogilevtsev, D., Cavalcanti, S. B., de Carvalho, C. A. A., & Oliveira, L. E. (2009). Plasmon polaritons in photonic superlattices containing a left-handed material. EPL, 88(24002), 1-6. DOI:10.1209/0295-5075/88/240020295-5075http://hdl.handle.net/10495/840110.1209/0295-5075/88/240021286-4854ABSTRACT: We analyze one-dimensional photonic superlattices which alternate layers of air and a left-handed material. We assume Drude-type dispersive responses for the dielectric permittivity and magnetic permeability of the left-handed material. Maxwell’s equations and the transfermatrix technique are used to derive the dispersion relation and transmission spectra for the propagation of obliquely incident optical fields. The photonic dispersion indicates that the growth direction component of the electric (or magnetic) field leads to the propagation of electric (or magnetic) plasmon polaritons, for either TE or TM configurations. Furthermore, we show that if the plasma frequency is chosen within the photonic (n(ω)) =0 zeroth-order bandgap, the coupling of light with plasmons weakens considerably. As light propagation is forbidden in that particular frequency region, the plasmon-polariton mode reduces to a pure plasmon modeapplication/pdfengInstitute of Physics Publishing (IOP)info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/PlasmónPolaritónSuperláquidos fotónicosPlasmon polaritons in photonic superlattices containing a left-handed materialEPL168824002ORIGINALReyesErnesto_2009_PlasmonPolaritonsPhotonic.pdfReyesErnesto_2009_PlasmonPolaritonsPhotonic.pdfArtículo de investigaciónapplication/pdf406820http://bibliotecadigital.udea.edu.co/bitstream/10495/8401/1/ReyesErnesto_2009_PlasmonPolaritonsPhotonic.pdfd7ea1676657b2c512e59c5e7f85d92a5MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/8401/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD55CC-LICENSElicense_urllicense_urltext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/8401/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8401/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8401/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD5410495/8401oai:bibliotecadigital.udea.edu.co:10495/84012021-05-16 11:46:05.719Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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 |