IndiumV3, Main, Repository, bibRecord, 000087

Interfacial charging originated from the conductivity decrease of C60 layer in IZO/pentacene/C60/Al organic double-layer solar cells

Identifieur interne : 000087 ( Main/Repository ); précédent : 000086; suivant : 000088

Interfacial charging originated from the conductivity decrease of C60 layer in IZO/pentacene/C60/Al organic double-layer solar cells

Auteurs : RBID : Pascal:14-0045689

Descripteurs français

Pascal (Inist)
- Cellule solaire organique, Couche double, Champ optique, Effet électrooptique, Effet champ électrique, Génération harmonique 2, Distribution charge électronique, Accumulation charge, Centre donneur, Centre accepteur, Evaluation performance, Dégradation, Endommagement, Revêtement protecteur, Fullerènes, Pentacène, Oxyde d'indium, Oxyde de zinc, Interface, Couche protectrice, 8105T, 4265K, C60.

English descriptors

KwdEn :
- Acceptor center, Charge accumulation, Damaging, Degradation, Donor center, Double layers, Electric field effect, Electron charge distribution, Electrooptical effect, Fullerenes, Indium oxide, Interface, Optical field, Organic solar cells, Pentacene, Performance evaluation, Protective coatings, Protective layer, Second harmonic generation, Zinc oxide.

Abstract

The origin of interfacial charging process in double-layer organic solar cells (OSCs) was studied by using the normal structure of Indium-Zinc-Oxide/pentacene/C₆₀/Al and its inverted double-layer system. Optical electric-field-induced second-harmonic generation (EFISHG) measurement was employed and results suggested that interfacial charging in these two kinds of OSCs led to charge accumulation with opposite charge polarity, owing to the conductivity decrease of C₆₀ layer. Applying the EFISHG measurements to the inverted OSCs also showed that the significant charge accumulation on donor-acceptor interface is responsible for the low I-V performance of the inverted OSCs. Thus, Maxwell-Wagner type interfacial charging, which is governed by the conductivity of C₆₀, can cause the degradation of the I-V performance of OSCs. The protection of C₆₀ layer from the conductivity decrease is a way to improve OSCs performance.

Links toward previous steps (curation, corpus...)

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Links to Exploration step

Pascal:14-0045689

Le document en format XML

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 layer in IZO/pentacene/C<sub>60</sub>
/Al organic double-layer solar cells</title>
<author><name>XIANGYU CHEN</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physical Electronics, Tokyo Institute of Technology</s1>
<s2>Meguro-ku, Tokyo 152-8552</s2>
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<author><name sortKey="Taguchi, Dai" uniqKey="Taguchi D">Dai Taguchi</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physical Electronics, Tokyo Institute of Technology</s1>
<s2>Meguro-ku, Tokyo 152-8552</s2>
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<wicri:noRegion>Meguro-ku, Tokyo 152-8552</wicri:noRegion>
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<author><name sortKey="Manaka, Takaaki" uniqKey="Manaka T">Takaaki Manaka</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physical Electronics, Tokyo Institute of Technology</s1>
<s2>Meguro-ku, Tokyo 152-8552</s2>
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<country>Japon</country>
<wicri:noRegion>Meguro-ku, Tokyo 152-8552</wicri:noRegion>
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</author>
<author><name sortKey="Iwamoto, Mitsumasa" uniqKey="Iwamoto M">Mitsumasa Iwamoto</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Physical Electronics, Tokyo Institute of Technology</s1>
<s2>Meguro-ku, Tokyo 152-8552</s2>
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<term>Charge accumulation</term>
<term>Damaging</term>
<term>Degradation</term>
<term>Donor center</term>
<term>Double layers</term>
<term>Electric field effect</term>
<term>Electron charge distribution</term>
<term>Electrooptical effect</term>
<term>Fullerenes</term>
<term>Indium oxide</term>
<term>Interface</term>
<term>Optical field</term>
<term>Organic solar cells</term>
<term>Pentacene</term>
<term>Performance evaluation</term>
<term>Protective coatings</term>
<term>Protective layer</term>
<term>Second harmonic generation</term>
<term>Zinc oxide</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Cellule solaire organique</term>
<term>Couche double</term>
<term>Champ optique</term>
<term>Effet électrooptique</term>
<term>Effet champ électrique</term>
<term>Génération harmonique 2</term>
<term>Distribution charge électronique</term>
<term>Accumulation charge</term>
<term>Centre donneur</term>
<term>Centre accepteur</term>
<term>Evaluation performance</term>
<term>Dégradation</term>
<term>Endommagement</term>
<term>Revêtement protecteur</term>
<term>Fullerènes</term>
<term>Pentacène</term>
<term>Oxyde d'indium</term>
<term>Oxyde de zinc</term>
<term>Interface</term>
<term>Couche protectrice</term>
<term>8105T</term>
<term>4265K</term>
<term>C60</term>
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<front><div type="abstract" xml:lang="en">The origin of interfacial charging process in double-layer organic solar cells (OSCs) was studied by using the normal structure of Indium-Zinc-Oxide/pentacene/C<sub>60</sub>
/Al and its inverted double-layer system. Optical electric-field-induced second-harmonic generation (EFISHG) measurement was employed and results suggested that interfacial charging in these two kinds of OSCs led to charge accumulation with opposite charge polarity, owing to the conductivity decrease of C<sub>60</sub>
 layer. Applying the EFISHG measurements to the inverted OSCs also showed that the significant charge accumulation on donor-acceptor interface is responsible for the low I-V performance of the inverted OSCs. Thus, Maxwell-Wagner type interfacial charging, which is governed by the conductivity of C<sub>60</sub>
, can cause the degradation of the I-V performance of OSCs. The protection of C<sub>60</sub>
 layer from the conductivity decrease is a way to improve OSCs performance.</div>
</front>
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 layer in IZO/pentacene/C<sub>60</sub>
/Al organic double-layer solar cells</s1>
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/Al and its inverted double-layer system. Optical electric-field-induced second-harmonic generation (EFISHG) measurement was employed and results suggested that interfacial charging in these two kinds of OSCs led to charge accumulation with opposite charge polarity, owing to the conductivity decrease of C<sub>60</sub>
 layer. Applying the EFISHG measurements to the inverted OSCs also showed that the significant charge accumulation on donor-acceptor interface is responsible for the low I-V performance of the inverted OSCs. Thus, Maxwell-Wagner type interfacial charging, which is governed by the conductivity of C<sub>60</sub>
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<s5>22</s5>
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<fN44 i1="01"><s1>OTO</s1>
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Interfacial charging originated from the conductivity decrease of C60 layer in IZO/pentacene/C60/Al organic double-layer solar cells

Interfacial charging originated from the conductivity decrease of C60 layer in IZO/pentacene/C60/Al organic double-layer solar cells

Descripteurs français

English descriptors

Abstract

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