Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides
| Ano de defesa: | 2022 |
|---|---|
| Autor(a) principal: | |
| Orientador(a): | |
| Banca de defesa: | |
| Tipo de documento: | Tese |
| Tipo de acesso: | Acesso aberto |
| Idioma: | por eng |
| Instituição de defesa: |
Universidade Presbiteriana Mackenzie
|
| Programa de Pós-Graduação: |
Não Informado pela instituição
|
| Departamento: |
Não Informado pela instituição
|
| País: |
Não Informado pela instituição
|
| Palavras-chave em Português: | |
| Link de acesso: | https://dspace.mackenzie.br/handle/10899/28924 |
Resumo: | Since the isolation of graphene, an increasing number of 2D materials have been produced, attracting attention of researchers. Graphene, however, behaves as a zero-gap semiconductor, which limits its applicability in photonic and optoelectronic devices. 2D transition metal dichalcogenides (TMDs), on the other hand, can exhibit different phases, with tunable bandgap energy, enabling photonic applications including modulators, photodetectors, and lightemitting diodes. Furthermore, TMD monolayers present large nonlinear optical susceptibilities, which are responsible for effects such as second- and third-harmonic generation (SHG/THG), important for all-optical wavelength conversion. However, and despite the enormous number of benefits, direct TMD utilization for practical nonlinear optical applications is still an ongoing challenge. The atomic thickness of these materials results in reduced light–matter interaction, which naturally leads to low net frequency converted intensities (even if the conversion efficiency per unit thickness is higher than that in conventional materials). Therefore, ways to enhance the process and maximize the nonlinear interaction are crucial for making practical applications viable. In this work, we propose two different approaches for enhancing the nonlinear conversion efficiency in 2D TMDs. In our first strategy, we propose optimizing the overall system through the influence of the substrate. We demonstrate the use of fluorinedoped-thin-oxide (FTO) with an epsilon-near-zero point close to the pump wavelength to increase the nonlinear conversion efficiency in monolayer TMDs. Polarized SHG measurements reveal an intensity one order of magnitude higher on TMDs deposited on FTO than that on a bare glass substrate. Secondly, a promising alternative is to increase the lightmatter interaction length by integration of 2D materials in on-chip waveguides. We exploit an exfoliation method to obtain macroscopic single-crystal monolayers, comparable in quality to microscopic flakes, which can in principle be transferred to waveguide structures, opening a path to real photonic devices. Thus, we present the use of different techniques to manipulate 2D TMDs and propose the use of different substrates and platforms to obtain optimized and more efficient nonlinear optical responses. |
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Vianna, Pilar GregoryMatos, Christiano José Santiago de2022-04-06T14:45:01Z2022-04-06T14:45:01Z2022-02-11Since the isolation of graphene, an increasing number of 2D materials have been produced, attracting attention of researchers. Graphene, however, behaves as a zero-gap semiconductor, which limits its applicability in photonic and optoelectronic devices. 2D transition metal dichalcogenides (TMDs), on the other hand, can exhibit different phases, with tunable bandgap energy, enabling photonic applications including modulators, photodetectors, and lightemitting diodes. Furthermore, TMD monolayers present large nonlinear optical susceptibilities, which are responsible for effects such as second- and third-harmonic generation (SHG/THG), important for all-optical wavelength conversion. However, and despite the enormous number of benefits, direct TMD utilization for practical nonlinear optical applications is still an ongoing challenge. The atomic thickness of these materials results in reduced light–matter interaction, which naturally leads to low net frequency converted intensities (even if the conversion efficiency per unit thickness is higher than that in conventional materials). Therefore, ways to enhance the process and maximize the nonlinear interaction are crucial for making practical applications viable. In this work, we propose two different approaches for enhancing the nonlinear conversion efficiency in 2D TMDs. In our first strategy, we propose optimizing the overall system through the influence of the substrate. We demonstrate the use of fluorinedoped-thin-oxide (FTO) with an epsilon-near-zero point close to the pump wavelength to increase the nonlinear conversion efficiency in monolayer TMDs. Polarized SHG measurements reveal an intensity one order of magnitude higher on TMDs deposited on FTO than that on a bare glass substrate. Secondly, a promising alternative is to increase the lightmatter interaction length by integration of 2D materials in on-chip waveguides. We exploit an exfoliation method to obtain macroscopic single-crystal monolayers, comparable in quality to microscopic flakes, which can in principle be transferred to waveguide structures, opening a path to real photonic devices. Thus, we present the use of different techniques to manipulate 2D TMDs and propose the use of different substrates and platforms to obtain optimized and more efficient nonlinear optical responses.CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nívelhttps://dspace.mackenzie.br/handle/10899/28924porengUniversidade Presbiteriana MackenzieAttribution-NonCommercial-NoDerivs 3.0 Brazilhttp://creativecommons.org/licenses/by-nc-nd/3.0/br/info:eu-repo/semantics/openAccess2D materialstransition metal dichalcogenides (TMDs)second-harmonic generation (SHG)nonlinear opticsepsilon-near-zero (ENZ)Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenidesinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/doctoralThesisreponame:Repositório Digital do Mackenzieinstname:Universidade Presbiteriana Mackenzie (MACKENZIE)instacron:MACKENZIEhttp://lattes.cnpq.br/6843256597783676http://lattes.cnpq.br/5168675150642820https://orcid.org/0000-0001-9767-5538Saito, Lúcia Akemi Miyazatohttp://lattes.cnpq.br/0915583034741895https://orcid.org/0000-0001-7157-1191Rosa, Henrique Guimarãeshttp://lattes.cnpq.br/7713098655067147Murray, Roberthttps://orcid.org/0000-0002-4036-1797Gomes, Anderson Stevens Leonidashttp://lattes.cnpq.br/8841334894205599Desde o isolamento do grafeno, um número crescente de materiais 2D tem sido produzido, atraindo a atenção de pesquisadores das mais diversas áreas. O grafeno comporta-se como um semicondutor de gap zero, o que limita sua aplicabilidade em dispositivos fotônicos e optoeletrônicos. Já os dicalcogenetos de metais de transição (TMDs, do inglês, transition metal dichalcogenides), podem exibir diferentes fases, com energia de bandgap variável, importante para aplicações fotônicas como moduladores, fotodetectores e diodos emissores de luz. Além disso, os TMDs monocamada apresentam altas suscetibilidades ópticas não lineares, responsáveis por efeitos como a geração de segundo e terceiro harmônico (SHG / THG), importante para conversão de frequência totalmente óptica. No entanto, e apesar do enorme número de benefícios, a utilização dos TMDs para aplicações práticas ainda é um desafio. A espessura atômica desses materiais resulta em baixa interação luz-matéria, o que naturalmente leva a baixas eficiências de conversão de frequência (mesmo considerando a eficiência de conversão por unidade de espessura maior do que em materiais convencionais). Portanto, formas de aprimorar os processos e maximizar a interação não linear são cruciais para viabilizar aplicações práticas. Neste trabalho, propomos duas abordagens diferentes para aumentar a eficiência de conversão não linear em TMDs. A primeira estratégia foca na otimização do sistema por meio da influência do substrato. Demonstramos o uso de óxido de estanho dopado com flúor (FTO, do inglês fluorine-doped thin oxide), com a constante dielétrica próxima a zero (ENZ, do inglês epsilon-near-zero) próximo ao comprimento de onda de bombeio, para maximizar a eficiência de conversão não linear em TMDs monocamada. Medidas de SHG polarizado revelam uma intensidade uma ordem de magnitude maior em TMDs depositados em FTO do que em vidro. A segunda estratégia, apresentada como uma alternativa promissora é aumentar o comprimento da interação luz-matéria pela integração de materiais 2D em guias de onda. Exploramos a exfoliação assistida por ouro desses materiais a fim de obter monocristais macroscópicos de uma única camada, comparáveis em qualidade aos flakes microscópicos, que podem, em princípio, ser transferidos para estruturas de guias de ondas abrindo caminho para dispositivos fotônicos reais. Dessa forma, apresentamos o uso de diferentes técnicas de manipulação de TMDs e propomos o uso de diferentes substratos e plataformas para a obtenção de respostas ópticas não lineares otimizadas e mais eficientes.materiais 2Ddicalcogenetos de metais de transiçãogeração de segundo harmônicoóptica não-linearepsilon-near-zero (ENZ)BrasilEscola de Engenharia Mackenzie (EE)UPMEngenharia de Materiais e NanotecnologiaTecnologia e desenvolvimento de materiaisORIGINALPilar Gregory ViannaPROTEGIDO.pdfPilar Gregory ViannaPROTEGIDO.pdfPilar Gregory Viannaapplication/pdf3806906https://dspace.mackenzie.br/bitstreams/f4cc9860-8874-4018-bf41-3101965a6601/downloade9c7609654c2ebd489edb19763134966MD51CC-LICENSElicense_rdflicense_rdfapplication/rdf+xml; charset=utf-8811https://dspace.mackenzie.br/bitstreams/9fce38d1-21ac-4866-9b52-8bcd241069f6/downloade39d27027a6cc9cb039ad269a5db8e34MD52LICENSElicense.txtlicense.txttext/plain; charset=utf-81997https://dspace.mackenzie.br/bitstreams/fba666c0-9c4c-465a-bdcc-c12f9815571a/downloadfb735e1a8fa1feda568f1b61905f8d57MD53TEXTPilar Gregory ViannaPROTEGIDO.pdf.txtPilar Gregory ViannaPROTEGIDO.pdf.txtExtracted texttext/plain174114https://dspace.mackenzie.br/bitstreams/43e23016-fa05-4d26-8d85-75af476de489/download52137c085b715699396a599fb30c5a25MD54THUMBNAILPilar Gregory ViannaPROTEGIDO.pdf.jpgPilar Gregory ViannaPROTEGIDO.pdf.jpgGenerated Thumbnailimage/jpeg1149https://dspace.mackenzie.br/bitstreams/370177fb-2428-4493-a578-2feeeddb7b50/downloade2e185c48ec12cffbda305713bbf4e73MD5510899/289242022-04-07 02:01:48.417http://creativecommons.org/licenses/by-nc-nd/3.0/br/Attribution-NonCommercial-NoDerivs 3.0 Braziloai:dspace.mackenzie.br:10899/28924https://dspace.mackenzie.brBiblioteca Digital de Teses e Dissertaçõeshttp://tede.mackenzie.br/jspui/PRIhttps://adelpha-api.mackenzie.br/server/oai/repositorio@mackenzie.br||paola.damato@mackenzie.bropendoar:102772022-04-07T02:01:48Repositório Digital do Mackenzie - Universidade Presbiteriana Mackenzie (MACKENZIE)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 |
| dc.title.pt_BR.fl_str_mv |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| title |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| spellingShingle |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides Vianna, Pilar Gregory 2D materials transition metal dichalcogenides (TMDs) second-harmonic generation (SHG) nonlinear optics epsilon-near-zero (ENZ) |
| title_short |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| title_full |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| title_fullStr |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| title_full_unstemmed |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| title_sort |
Methods to enhance the nonlinear optical frequency conversion in transition metal dichalcogenides |
| author |
Vianna, Pilar Gregory |
| author_facet |
Vianna, Pilar Gregory |
| author_role |
author |
| dc.contributor.author.fl_str_mv |
Vianna, Pilar Gregory |
| dc.contributor.advisor1.fl_str_mv |
Matos, Christiano José Santiago de |
| contributor_str_mv |
Matos, Christiano José Santiago de |
| dc.subject.por.fl_str_mv |
2D materials transition metal dichalcogenides (TMDs) second-harmonic generation (SHG) nonlinear optics epsilon-near-zero (ENZ) |
| topic |
2D materials transition metal dichalcogenides (TMDs) second-harmonic generation (SHG) nonlinear optics epsilon-near-zero (ENZ) |
| description |
Since the isolation of graphene, an increasing number of 2D materials have been produced, attracting attention of researchers. Graphene, however, behaves as a zero-gap semiconductor, which limits its applicability in photonic and optoelectronic devices. 2D transition metal dichalcogenides (TMDs), on the other hand, can exhibit different phases, with tunable bandgap energy, enabling photonic applications including modulators, photodetectors, and lightemitting diodes. Furthermore, TMD monolayers present large nonlinear optical susceptibilities, which are responsible for effects such as second- and third-harmonic generation (SHG/THG), important for all-optical wavelength conversion. However, and despite the enormous number of benefits, direct TMD utilization for practical nonlinear optical applications is still an ongoing challenge. The atomic thickness of these materials results in reduced light–matter interaction, which naturally leads to low net frequency converted intensities (even if the conversion efficiency per unit thickness is higher than that in conventional materials). Therefore, ways to enhance the process and maximize the nonlinear interaction are crucial for making practical applications viable. In this work, we propose two different approaches for enhancing the nonlinear conversion efficiency in 2D TMDs. In our first strategy, we propose optimizing the overall system through the influence of the substrate. We demonstrate the use of fluorinedoped-thin-oxide (FTO) with an epsilon-near-zero point close to the pump wavelength to increase the nonlinear conversion efficiency in monolayer TMDs. Polarized SHG measurements reveal an intensity one order of magnitude higher on TMDs deposited on FTO than that on a bare glass substrate. Secondly, a promising alternative is to increase the lightmatter interaction length by integration of 2D materials in on-chip waveguides. We exploit an exfoliation method to obtain macroscopic single-crystal monolayers, comparable in quality to microscopic flakes, which can in principle be transferred to waveguide structures, opening a path to real photonic devices. Thus, we present the use of different techniques to manipulate 2D TMDs and propose the use of different substrates and platforms to obtain optimized and more efficient nonlinear optical responses. |
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2022 |
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2022-04-06T14:45:01Z |
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2022-04-06T14:45:01Z |
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2022-02-11 |
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info:eu-repo/semantics/publishedVersion |
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info:eu-repo/semantics/doctoralThesis |
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https://dspace.mackenzie.br/handle/10899/28924 |
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por eng |
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por eng |
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Attribution-NonCommercial-NoDerivs 3.0 Brazil http://creativecommons.org/licenses/by-nc-nd/3.0/br/ |
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Universidade Presbiteriana Mackenzie |
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Universidade Presbiteriana Mackenzie |
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