Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge
- Autores
- Quinteiro, Guillermo Federico; Kuhn, Tilmann; Reiter, D. E.
- Año de publicación
- 2015
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- Twisted light is light carrying orbital angular momentum. The profile of such a beam is a ring-like structure with a node at the beam axis, where a phase singularity exists. Due to the strong spatial inhomogeneity the mathematical description of twisted-light–matter interaction is non-trivial, in particular close to the phase singularity, where the commonly used dipole-moment approximation cannot be applied. In this paper we show that, if the handedness of circular polarization and the orbital angular momentum of the twisted-light beam have the same sign, a Hamiltonian similar to the dipole-moment approximation can be derived. However, if the signs differ, in general the magnetic parts of the light beam become of significant importance and an interaction Hamiltonian which only accounts for electric fields is inappropriate. We discuss the consequences of these findings for twisted-light excitation of a semiconductor nanostructures, e.g., a quantum dot, placed at the phase singularity.
Fil: Quinteiro, Guillermo Federico. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Física de Buenos Aires. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Física de Buenos Aires; Argentina
Fil: Kuhn, Tilmann. Westfalische Wilhelms Universitat; Alemania
Fil: Reiter, D. E.. Westfalische Wilhelms Universitat; Alemania - Materia
-
OPTICAL VORTEX
TWISTED LIGHT - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
.jpg)
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/43505
Ver los metadatos del registro completo
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Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gaugeQuinteiro, Guillermo FedericoKuhn, TilmannReiter, D. E.OPTICAL VORTEXTWISTED LIGHThttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Twisted light is light carrying orbital angular momentum. The profile of such a beam is a ring-like structure with a node at the beam axis, where a phase singularity exists. Due to the strong spatial inhomogeneity the mathematical description of twisted-light–matter interaction is non-trivial, in particular close to the phase singularity, where the commonly used dipole-moment approximation cannot be applied. In this paper we show that, if the handedness of circular polarization and the orbital angular momentum of the twisted-light beam have the same sign, a Hamiltonian similar to the dipole-moment approximation can be derived. However, if the signs differ, in general the magnetic parts of the light beam become of significant importance and an interaction Hamiltonian which only accounts for electric fields is inappropriate. We discuss the consequences of these findings for twisted-light excitation of a semiconductor nanostructures, e.g., a quantum dot, placed at the phase singularity.Fil: Quinteiro, Guillermo Federico. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Física de Buenos Aires. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Física de Buenos Aires; ArgentinaFil: Kuhn, Tilmann. Westfalische Wilhelms Universitat; AlemaniaFil: Reiter, D. E.. Westfalische Wilhelms Universitat; AlemaniaAmerican Physical Society2015-03info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/43505Quinteiro, Guillermo Federico; Kuhn, Tilmann; Reiter, D. E.; Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge; American Physical Society; Physical Review A: Atomic, Molecular and Optical Physics; 91; 3; 3-2015; 1-121050-2947CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/https://journals.aps.org/pra/abstract/10.1103/PhysRevA.91.033808info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevA.91.033808info:eu-repo/semantics/altIdentifier/url/https://arxiv.org/abs/1401.8147info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-10-15T14:46:43Zoai:ri.conicet.gov.ar:11336/43505instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-10-15 14:46:43.643CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
| dc.title.none.fl_str_mv |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| title |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| spellingShingle |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge Quinteiro, Guillermo Federico OPTICAL VORTEX TWISTED LIGHT |
| title_short |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| title_full |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| title_fullStr |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| title_full_unstemmed |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| title_sort |
Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge |
| dc.creator.none.fl_str_mv |
Quinteiro, Guillermo Federico Kuhn, Tilmann Reiter, D. E. |
| author |
Quinteiro, Guillermo Federico |
| author_facet |
Quinteiro, Guillermo Federico Kuhn, Tilmann Reiter, D. E. |
| author_role |
author |
| author2 |
Kuhn, Tilmann Reiter, D. E. |
| author2_role |
author author |
| dc.subject.none.fl_str_mv |
OPTICAL VORTEX TWISTED LIGHT |
| topic |
OPTICAL VORTEX TWISTED LIGHT |
| purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
| dc.description.none.fl_txt_mv |
Twisted light is light carrying orbital angular momentum. The profile of such a beam is a ring-like structure with a node at the beam axis, where a phase singularity exists. Due to the strong spatial inhomogeneity the mathematical description of twisted-light–matter interaction is non-trivial, in particular close to the phase singularity, where the commonly used dipole-moment approximation cannot be applied. In this paper we show that, if the handedness of circular polarization and the orbital angular momentum of the twisted-light beam have the same sign, a Hamiltonian similar to the dipole-moment approximation can be derived. However, if the signs differ, in general the magnetic parts of the light beam become of significant importance and an interaction Hamiltonian which only accounts for electric fields is inappropriate. We discuss the consequences of these findings for twisted-light excitation of a semiconductor nanostructures, e.g., a quantum dot, placed at the phase singularity. Fil: Quinteiro, Guillermo Federico. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Física de Buenos Aires. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Física de Buenos Aires; Argentina Fil: Kuhn, Tilmann. Westfalische Wilhelms Universitat; Alemania Fil: Reiter, D. E.. Westfalische Wilhelms Universitat; Alemania |
| description |
Twisted light is light carrying orbital angular momentum. The profile of such a beam is a ring-like structure with a node at the beam axis, where a phase singularity exists. Due to the strong spatial inhomogeneity the mathematical description of twisted-light–matter interaction is non-trivial, in particular close to the phase singularity, where the commonly used dipole-moment approximation cannot be applied. In this paper we show that, if the handedness of circular polarization and the orbital angular momentum of the twisted-light beam have the same sign, a Hamiltonian similar to the dipole-moment approximation can be derived. However, if the signs differ, in general the magnetic parts of the light beam become of significant importance and an interaction Hamiltonian which only accounts for electric fields is inappropriate. We discuss the consequences of these findings for twisted-light excitation of a semiconductor nanostructures, e.g., a quantum dot, placed at the phase singularity. |
| publishDate |
2015 |
| dc.date.none.fl_str_mv |
2015-03 |
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info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
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article |
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publishedVersion |
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http://hdl.handle.net/11336/43505 Quinteiro, Guillermo Federico; Kuhn, Tilmann; Reiter, D. E.; Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge; American Physical Society; Physical Review A: Atomic, Molecular and Optical Physics; 91; 3; 3-2015; 1-12 1050-2947 CONICET Digital CONICET |
| url |
http://hdl.handle.net/11336/43505 |
| identifier_str_mv |
Quinteiro, Guillermo Federico; Kuhn, Tilmann; Reiter, D. E.; Formulation of the twisted-light–matter interaction at the phase singularity: The twisted-light gauge; American Physical Society; Physical Review A: Atomic, Molecular and Optical Physics; 91; 3; 3-2015; 1-12 1050-2947 CONICET Digital CONICET |
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eng |
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eng |
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