Cristais anidros das bases do ADN sÃo semicondutores de Gap largo

Bibliographic Details
Main Author: Francisco Francinà Maia JÃnior
Publication Date: 2011
Format: Doctoral thesis
Language: por
Source: Biblioteca Digital de Teses e Dissertações da UFC
Download full: http://www.teses.ufc.br/tde_busca/arquivo.php?codArquivo=9592
Summary: Guanine (G), adenine (A), cytosine (C), and thymine (T) nucleotide bases are the essential building blocks of DNA (deoxyribonucleic acid), which contains the genetic information used to build living cells. DNA strands are also promising candidates to fabricate molecular nanodevices, since they are stable polymers easy to replicate. Despite the early suggestion of the possibility of using DNA as a nanoscale conductor almost ten years after the elucidation of its helical structure, charge carrier transport through DNA-based structures is still a matter of debate. Here, we present the structural, electronic and optical properties of anhydrous crystals of DNA nucleobases found after DFT (Density Functional Theory) calculations, as well as experimental measurements of optical absorption for powders of these crystals. Experimental measurements of the UV absorption spectra for the anhydrous crystals were carried out on these pellets using a Varian Cary 5000 UV-visible NIR spectrophotometer. The absorption spectrum of the samples was recorded in the wavelength range between 200 and 800 nm (50000-12500 cm-1). The computational simulations of the present work were performed using the CASTEP code, which is based in the DFT approach. The Local Density Approximation (LDA) exchange-correlation potential developed by Ceperley and Alder and parametrized by Perdew and Zunger was adopted as well. With respect to our choice of functional, a note of caution must be made: in anhydrous DNA bases crystals, van der Waals interactions along the molecular stacking axis and hydrogen bonding between molecules in the same stacking plane are relevant to explain their structural features, and it is well known that pure DFT methods are unable to give a good description of dispersive forces. Besides, the LDA approximation is not the best option to provide an accurate account of hydrogen bonds. However, some DFT studies of layered crystals such as graphite as well as guanine hydrated crystals have shown that the LDA gives reasonable values for atomic distances, notwithstanding the limitations of this functional. This and the relatively low cost of LDA computations have motivated us to its adoption instead of more sophisticated (and computationally expensive) means. Guanine and cytosine (adenine and thymine) anhydrous crystals are predicted from the DFT simulations to be direct (indirect) band gap semiconductors, with values 2.68 eV and 3.30 eV (2.83 eV and 3.32 eV), respectively, while the experimentally estimated band gaps we have measured are 3.7 eV and 3.8 eV (3.5 eV and 4.0 eV), in the same order. Our LDA figures for the energy gaps are smaller than experimental values, as expected, and the gaps estimated from the optical absorption measurements presented in this work are in general smaller than experimental data available in the literature (except for guanine). The LDA ordering of increasing band gaps is G < A < C < T, while the ordering of gaps obtained experimentally is not settled: our work finds (from optical absorption measurements) A < G < C < T in contrast with the X-ray measurements, that indicate the energy gap sequence G < C < A < T. For electrons and holes moving along selected hydrogen bonds (parallel to the molecular plane of a given nucleobase), effective masses are in general large, exception made to thymine. When the same electrons move along the pi-stacking axis, however, effective masses stay between 4.0 and 6.3 free electron masses (m0), which suggests that stackings of nucleobases behave like wide gap semiconductors for electrons. The perpendicular transport of holes is also favored for nucleobase stackings without thymine. Finally, the complex dielectric function was calculated for each anydrous DNA base crystal, and a very pronounced anisotropy was observed for polarized incident light in the cases of guanine, adenine, and thymine, but not for cytosine.
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spelling info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/doctoralThesisCristais anidros das bases do ADN sÃo semicondutores de Gap largoAnhydrous cristals of DNA bases are wide gap semiconductors2011-01-20Valder Nogueira Freire12105473334http://lattes.cnpq.br/864792232710095389107594372Francisco Francinà Maia JÃniorUniversidade Federal do CearÃPrograma de PÃs-GraduaÃÃo em FÃsicaUFCBRElectronic properties DNA ab initio nucleotide basesPropriedades eletrÃnicas DNA ab initio bases nucleotÃdicasFISICA DA MATERIA CONDENSADAGuanine (G), adenine (A), cytosine (C), and thymine (T) nucleotide bases are the essential building blocks of DNA (deoxyribonucleic acid), which contains the genetic information used to build living cells. DNA strands are also promising candidates to fabricate molecular nanodevices, since they are stable polymers easy to replicate. Despite the early suggestion of the possibility of using DNA as a nanoscale conductor almost ten years after the elucidation of its helical structure, charge carrier transport through DNA-based structures is still a matter of debate. Here, we present the structural, electronic and optical properties of anhydrous crystals of DNA nucleobases found after DFT (Density Functional Theory) calculations, as well as experimental measurements of optical absorption for powders of these crystals. Experimental measurements of the UV absorption spectra for the anhydrous crystals were carried out on these pellets using a Varian Cary 5000 UV-visible NIR spectrophotometer. The absorption spectrum of the samples was recorded in the wavelength range between 200 and 800 nm (50000-12500 cm-1). The computational simulations of the present work were performed using the CASTEP code, which is based in the DFT approach. The Local Density Approximation (LDA) exchange-correlation potential developed by Ceperley and Alder and parametrized by Perdew and Zunger was adopted as well. With respect to our choice of functional, a note of caution must be made: in anhydrous DNA bases crystals, van der Waals interactions along the molecular stacking axis and hydrogen bonding between molecules in the same stacking plane are relevant to explain their structural features, and it is well known that pure DFT methods are unable to give a good description of dispersive forces. Besides, the LDA approximation is not the best option to provide an accurate account of hydrogen bonds. However, some DFT studies of layered crystals such as graphite as well as guanine hydrated crystals have shown that the LDA gives reasonable values for atomic distances, notwithstanding the limitations of this functional. This and the relatively low cost of LDA computations have motivated us to its adoption instead of more sophisticated (and computationally expensive) means. Guanine and cytosine (adenine and thymine) anhydrous crystals are predicted from the DFT simulations to be direct (indirect) band gap semiconductors, with values 2.68 eV and 3.30 eV (2.83 eV and 3.32 eV), respectively, while the experimentally estimated band gaps we have measured are 3.7 eV and 3.8 eV (3.5 eV and 4.0 eV), in the same order. Our LDA figures for the energy gaps are smaller than experimental values, as expected, and the gaps estimated from the optical absorption measurements presented in this work are in general smaller than experimental data available in the literature (except for guanine). The LDA ordering of increasing band gaps is G < A < C < T, while the ordering of gaps obtained experimentally is not settled: our work finds (from optical absorption measurements) A < G < C < T in contrast with the X-ray measurements, that indicate the energy gap sequence G < C < A < T. For electrons and holes moving along selected hydrogen bonds (parallel to the molecular plane of a given nucleobase), effective masses are in general large, exception made to thymine. When the same electrons move along the pi-stacking axis, however, effective masses stay between 4.0 and 6.3 free electron masses (m0), which suggests that stackings of nucleobases behave like wide gap semiconductors for electrons. The perpendicular transport of holes is also favored for nucleobase stackings without thymine. Finally, the complex dielectric function was calculated for each anydrous DNA base crystal, and a very pronounced anisotropy was observed for polarized incident light in the cases of guanine, adenine, and thymine, but not for cytosine.As bases nucleotÃdicas guanina (G), adenina (A), citosina (C) e timina (T) sÃo bases nucleotÃdicasos blocos essenciais da molÃcula do Ãcido desoxiribonucleico (ADN), que contÃm a as informaÃÃes genÃticas usadas pelas cÃlulas vivas. Filamentos de ADN sÃo tambÃm candidatos promissores para fabricaÃÃo nanodispositivos moleculares, visto que polÃmeros estÃveis e de fÃcil replicaÃÃo. Apesar desta sugestÃo inicial da possibilidade de usar o ADN como condutor em nanoescala apenas dez anos apÃs a elucidaÃÃo da estrutura helicoidal do ADN, o transporte de portadores de cargas atravÃs de estruturas baseadas no ADN ainda sÃo matÃria de debate. Aqui, sÃo apresentadas as propriedades estruturais, eletrÃnicas e Ãpticas dos cristais anidros das bases do ADN obtidas apÃs cÃlculos baseados na teoria do funcional da densidade (DFT, do inglÃs Density Functional Theory), assim como medidas de absorÃÃo Ãtica para o pà desses cristais. Os experimentos do espectro absorÃÃo UV para os cristais foram realizadas sobre pastilhas usando o espectrometro Varian Cary 5000 UV-visible NIR, considerando o intervalo de 200 and 800 nm (50000-12500 cm-1). Os cÃlculos teÃricos da presente tese foram desenvolvidos usando o pacote CASTEP, baseado na teoria DFT. Na descriÃÃo do potencial de troca e correlaÃÃo, foi utilizada aproximaÃÃo local da densidade (LDA, do inglÃs Local Density Approximation) desenvolvida por Cerpeley e Alder e parametrizado por Perdew e Zunger (CA-PZ). Sobre a escolha do funcional, uma observaÃÃo deve ser feita: nos cristais anidros das bases do ADN, interaÃÃes de van der Waals ao longo do eixo de empilhamento molecular e as ligaÃÃes de hidrogÃnio entre as molÃculas do mesmo plano sÃo relevantes na explicaÃÃo das suas caracterÃsticas, e à bem conhecido que os mÃtodos de DFT puro sÃo incapazes de uma boa descriÃÃo das forÃas dispersivas. AlÃm disso, a aproximaÃÃo LDA nÃo à a melhor opÃÃo para cÃlculos precisos das ligaÃÃes de hidrogÃnio. Entretanto, alguns trabalhos DFT de cristais formados por camadas tais como grafite e o cristal hidratado da guanina mostraram que o funcional LDA fornece valores razoÃveis para as distÃncias atÃmicas, contrariando as limitaÃÃes desse funcional. Isso e o baixo custo computacional foram as motivaÃÃes que levaram a sua escolha em vez da adoÃÃo de funcionais mais sofisticados (e computacionalmente mais pesados). Os cristais de guanina e citosina (adenina e timina) sÃo previstos terem gaps diretos (indiretos), com os valores experimentais estimados a partir da absorÃÃo de 3,7 eV e 3,8 eV (3,8 eV e 4,0 eV), na mesma ordem. Os resultados LDA mostraram gaps de energia menores do que os valores experimentais, como esperado, e os gaps experimentais estimados a partir da absorÃÃo Ãtica sÃo, em geral, menores do que os valores experimentais disponÃveis na literatura (exceto, para a guanina). A ordem crescente nos valores calculados dos gaps de energia para os cristais à dada por G < A < C < T, enquanto os valores experimentais obtidos nesta tese (a partir da absorÃÃo Ãptica) seguem a ordem A < G < C < T em contraste com as medidas de raios-x, que indicam a sequÃncia G < C < A < T. Para os elÃtrons e buracos se movendo das ligaÃÃes de hidrogÃnio (paralelas ao plano molecular da base), as massas efetivas sÃo geralmente elevadas, exceto para a timina. Quando os mesmos elÃtrons se movimentam ao do eixo de empilhamento molecular, entretanto, as massas efetivas ficam entre 4,0 e 6,3m0, sugerindo estes cristais se comportam como semicondutores de gap largo ao longo das direÃÃes de empilhamento molecular. O transporte de buracos tambÃm à favorecido ao longo da direÃÃo de empilhamento, exceto para a timina. Finalmente, a funÃÃo dielÃtrica complexa foi calculada para cada cristal anidro das bases do ADN, sendo observada uma forte anisotropia para a incidÃncia de luz polarizada nos casos da guanina, adenina e timina, mas nÃo para a citosina. CoordenaÃÃo de AperfeiÃoamento de NÃvel Superiorhttp://www.teses.ufc.br/tde_busca/arquivo.php?codArquivo=9592application/pdfinfo:eu-repo/semantics/openAccessporreponame:Biblioteca Digital de Teses e Dissertações da UFCinstname:Universidade Federal do Cearáinstacron:UFC2019-01-21T11:22:51Zmail@mail.com -
dc.title.pt.fl_str_mv Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
dc.title.alternative..fl_str_mv Anhydrous cristals of DNA bases are wide gap semiconductors
title Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
spellingShingle Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
Francisco Francinà Maia JÃnior
Propriedades eletrÃnicas
DNA
ab initio
bases nucleotÃdicas
FISICA DA MATERIA CONDENSADA
title_short Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
title_full Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
title_fullStr Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
title_full_unstemmed Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
title_sort Cristais anidros das bases do ADN sÃo semicondutores de Gap largo
author Francisco Francinà Maia JÃnior
author_facet Francisco Francinà Maia JÃnior
author_role author
dc.contributor.advisor1.fl_str_mv Valder Nogueira Freire
dc.contributor.advisor1ID.fl_str_mv 12105473334
dc.contributor.advisor1Lattes.fl_str_mv http://lattes.cnpq.br/8647922327100953
dc.contributor.authorID.fl_str_mv 89107594372
dc.contributor.author.fl_str_mv Francisco Francinà Maia JÃnior
contributor_str_mv Valder Nogueira Freire
dc.subject.por.fl_str_mv Propriedades eletrÃnicas
DNA
ab initio
bases nucleotÃdicas
topic Propriedades eletrÃnicas
DNA
ab initio
bases nucleotÃdicas
FISICA DA MATERIA CONDENSADA
dc.subject.cnpq.fl_str_mv FISICA DA MATERIA CONDENSADA
dc.description.sponsorship.fl_txt_mv CoordenaÃÃo de AperfeiÃoamento de NÃvel Superior
dc.description.abstract..fl_txt_mv Guanine (G), adenine (A), cytosine (C), and thymine (T) nucleotide bases are the essential building blocks of DNA (deoxyribonucleic acid), which contains the genetic information used to build living cells. DNA strands are also promising candidates to fabricate molecular nanodevices, since they are stable polymers easy to replicate. Despite the early suggestion of the possibility of using DNA as a nanoscale conductor almost ten years after the elucidation of its helical structure, charge carrier transport through DNA-based structures is still a matter of debate. Here, we present the structural, electronic and optical properties of anhydrous crystals of DNA nucleobases found after DFT (Density Functional Theory) calculations, as well as experimental measurements of optical absorption for powders of these crystals. Experimental measurements of the UV absorption spectra for the anhydrous crystals were carried out on these pellets using a Varian Cary 5000 UV-visible NIR spectrophotometer. The absorption spectrum of the samples was recorded in the wavelength range between 200 and 800 nm (50000-12500 cm-1). The computational simulations of the present work were performed using the CASTEP code, which is based in the DFT approach. The Local Density Approximation (LDA) exchange-correlation potential developed by Ceperley and Alder and parametrized by Perdew and Zunger was adopted as well. With respect to our choice of functional, a note of caution must be made: in anhydrous DNA bases crystals, van der Waals interactions along the molecular stacking axis and hydrogen bonding between molecules in the same stacking plane are relevant to explain their structural features, and it is well known that pure DFT methods are unable to give a good description of dispersive forces. Besides, the LDA approximation is not the best option to provide an accurate account of hydrogen bonds. However, some DFT studies of layered crystals such as graphite as well as guanine hydrated crystals have shown that the LDA gives reasonable values for atomic distances, notwithstanding the limitations of this functional. This and the relatively low cost of LDA computations have motivated us to its adoption instead of more sophisticated (and computationally expensive) means. Guanine and cytosine (adenine and thymine) anhydrous crystals are predicted from the DFT simulations to be direct (indirect) band gap semiconductors, with values 2.68 eV and 3.30 eV (2.83 eV and 3.32 eV), respectively, while the experimentally estimated band gaps we have measured are 3.7 eV and 3.8 eV (3.5 eV and 4.0 eV), in the same order. Our LDA figures for the energy gaps are smaller than experimental values, as expected, and the gaps estimated from the optical absorption measurements presented in this work are in general smaller than experimental data available in the literature (except for guanine). The LDA ordering of increasing band gaps is G < A < C < T, while the ordering of gaps obtained experimentally is not settled: our work finds (from optical absorption measurements) A < G < C < T in contrast with the X-ray measurements, that indicate the energy gap sequence G < C < A < T. For electrons and holes moving along selected hydrogen bonds (parallel to the molecular plane of a given nucleobase), effective masses are in general large, exception made to thymine. When the same electrons move along the pi-stacking axis, however, effective masses stay between 4.0 and 6.3 free electron masses (m0), which suggests that stackings of nucleobases behave like wide gap semiconductors for electrons. The perpendicular transport of holes is also favored for nucleobase stackings without thymine. Finally, the complex dielectric function was calculated for each anydrous DNA base crystal, and a very pronounced anisotropy was observed for polarized incident light in the cases of guanine, adenine, and thymine, but not for cytosine.
dc.description.abstract.por.fl_txt_mv As bases nucleotÃdicas guanina (G), adenina (A), citosina (C) e timina (T) sÃo bases nucleotÃdicasos blocos essenciais da molÃcula do Ãcido desoxiribonucleico (ADN), que contÃm a as informaÃÃes genÃticas usadas pelas cÃlulas vivas. Filamentos de ADN sÃo tambÃm candidatos promissores para fabricaÃÃo nanodispositivos moleculares, visto que polÃmeros estÃveis e de fÃcil replicaÃÃo. Apesar desta sugestÃo inicial da possibilidade de usar o ADN como condutor em nanoescala apenas dez anos apÃs a elucidaÃÃo da estrutura helicoidal do ADN, o transporte de portadores de cargas atravÃs de estruturas baseadas no ADN ainda sÃo matÃria de debate. Aqui, sÃo apresentadas as propriedades estruturais, eletrÃnicas e Ãpticas dos cristais anidros das bases do ADN obtidas apÃs cÃlculos baseados na teoria do funcional da densidade (DFT, do inglÃs Density Functional Theory), assim como medidas de absorÃÃo Ãtica para o pà desses cristais. Os experimentos do espectro absorÃÃo UV para os cristais foram realizadas sobre pastilhas usando o espectrometro Varian Cary 5000 UV-visible NIR, considerando o intervalo de 200 and 800 nm (50000-12500 cm-1). Os cÃlculos teÃricos da presente tese foram desenvolvidos usando o pacote CASTEP, baseado na teoria DFT. Na descriÃÃo do potencial de troca e correlaÃÃo, foi utilizada aproximaÃÃo local da densidade (LDA, do inglÃs Local Density Approximation) desenvolvida por Cerpeley e Alder e parametrizado por Perdew e Zunger (CA-PZ). Sobre a escolha do funcional, uma observaÃÃo deve ser feita: nos cristais anidros das bases do ADN, interaÃÃes de van der Waals ao longo do eixo de empilhamento molecular e as ligaÃÃes de hidrogÃnio entre as molÃculas do mesmo plano sÃo relevantes na explicaÃÃo das suas caracterÃsticas, e à bem conhecido que os mÃtodos de DFT puro sÃo incapazes de uma boa descriÃÃo das forÃas dispersivas. AlÃm disso, a aproximaÃÃo LDA nÃo à a melhor opÃÃo para cÃlculos precisos das ligaÃÃes de hidrogÃnio. Entretanto, alguns trabalhos DFT de cristais formados por camadas tais como grafite e o cristal hidratado da guanina mostraram que o funcional LDA fornece valores razoÃveis para as distÃncias atÃmicas, contrariando as limitaÃÃes desse funcional. Isso e o baixo custo computacional foram as motivaÃÃes que levaram a sua escolha em vez da adoÃÃo de funcionais mais sofisticados (e computacionalmente mais pesados). Os cristais de guanina e citosina (adenina e timina) sÃo previstos terem gaps diretos (indiretos), com os valores experimentais estimados a partir da absorÃÃo de 3,7 eV e 3,8 eV (3,8 eV e 4,0 eV), na mesma ordem. Os resultados LDA mostraram gaps de energia menores do que os valores experimentais, como esperado, e os gaps experimentais estimados a partir da absorÃÃo Ãtica sÃo, em geral, menores do que os valores experimentais disponÃveis na literatura (exceto, para a guanina). A ordem crescente nos valores calculados dos gaps de energia para os cristais à dada por G < A < C < T, enquanto os valores experimentais obtidos nesta tese (a partir da absorÃÃo Ãptica) seguem a ordem A < G < C < T em contraste com as medidas de raios-x, que indicam a sequÃncia G < C < A < T. Para os elÃtrons e buracos se movendo das ligaÃÃes de hidrogÃnio (paralelas ao plano molecular da base), as massas efetivas sÃo geralmente elevadas, exceto para a timina. Quando os mesmos elÃtrons se movimentam ao do eixo de empilhamento molecular, entretanto, as massas efetivas ficam entre 4,0 e 6,3m0, sugerindo estes cristais se comportam como semicondutores de gap largo ao longo das direÃÃes de empilhamento molecular. O transporte de buracos tambÃm à favorecido ao longo da direÃÃo de empilhamento, exceto para a timina. Finalmente, a funÃÃo dielÃtrica complexa foi calculada para cada cristal anidro das bases do ADN, sendo observada uma forte anisotropia para a incidÃncia de luz polarizada nos casos da guanina, adenina e timina, mas nÃo para a citosina.
description Guanine (G), adenine (A), cytosine (C), and thymine (T) nucleotide bases are the essential building blocks of DNA (deoxyribonucleic acid), which contains the genetic information used to build living cells. DNA strands are also promising candidates to fabricate molecular nanodevices, since they are stable polymers easy to replicate. Despite the early suggestion of the possibility of using DNA as a nanoscale conductor almost ten years after the elucidation of its helical structure, charge carrier transport through DNA-based structures is still a matter of debate. Here, we present the structural, electronic and optical properties of anhydrous crystals of DNA nucleobases found after DFT (Density Functional Theory) calculations, as well as experimental measurements of optical absorption for powders of these crystals. Experimental measurements of the UV absorption spectra for the anhydrous crystals were carried out on these pellets using a Varian Cary 5000 UV-visible NIR spectrophotometer. The absorption spectrum of the samples was recorded in the wavelength range between 200 and 800 nm (50000-12500 cm-1). The computational simulations of the present work were performed using the CASTEP code, which is based in the DFT approach. The Local Density Approximation (LDA) exchange-correlation potential developed by Ceperley and Alder and parametrized by Perdew and Zunger was adopted as well. With respect to our choice of functional, a note of caution must be made: in anhydrous DNA bases crystals, van der Waals interactions along the molecular stacking axis and hydrogen bonding between molecules in the same stacking plane are relevant to explain their structural features, and it is well known that pure DFT methods are unable to give a good description of dispersive forces. Besides, the LDA approximation is not the best option to provide an accurate account of hydrogen bonds. However, some DFT studies of layered crystals such as graphite as well as guanine hydrated crystals have shown that the LDA gives reasonable values for atomic distances, notwithstanding the limitations of this functional. This and the relatively low cost of LDA computations have motivated us to its adoption instead of more sophisticated (and computationally expensive) means. Guanine and cytosine (adenine and thymine) anhydrous crystals are predicted from the DFT simulations to be direct (indirect) band gap semiconductors, with values 2.68 eV and 3.30 eV (2.83 eV and 3.32 eV), respectively, while the experimentally estimated band gaps we have measured are 3.7 eV and 3.8 eV (3.5 eV and 4.0 eV), in the same order. Our LDA figures for the energy gaps are smaller than experimental values, as expected, and the gaps estimated from the optical absorption measurements presented in this work are in general smaller than experimental data available in the literature (except for guanine). The LDA ordering of increasing band gaps is G < A < C < T, while the ordering of gaps obtained experimentally is not settled: our work finds (from optical absorption measurements) A < G < C < T in contrast with the X-ray measurements, that indicate the energy gap sequence G < C < A < T. For electrons and holes moving along selected hydrogen bonds (parallel to the molecular plane of a given nucleobase), effective masses are in general large, exception made to thymine. When the same electrons move along the pi-stacking axis, however, effective masses stay between 4.0 and 6.3 free electron masses (m0), which suggests that stackings of nucleobases behave like wide gap semiconductors for electrons. The perpendicular transport of holes is also favored for nucleobase stackings without thymine. Finally, the complex dielectric function was calculated for each anydrous DNA base crystal, and a very pronounced anisotropy was observed for polarized incident light in the cases of guanine, adenine, and thymine, but not for cytosine.
publishDate 2011
dc.date.issued.fl_str_mv 2011-01-20
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