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fact that high PCE can be achieved in a device without ETL poses the question of
how and to what extent an ETL can improve the electron-collecting ability of ITO
in inverted devices.
3.3.2 Anode Interlayer
Direct contact of the top high work-function metal to the active layer can lead to
degradation of the solar cell performance, therefore, a hole-transporting/electron-
blocking layer (HTL/EBL) is generally deposited between these two layers to
improve charge selectivity and collection of holes. The materials that have been
utilized as HTL are various high work-function transition metal oxides such as
MoO 3 , or denoted as MoO x because of oxygen vacancy formed during thermo-
evaporation [ 97 , 120 , 121 ], WO 3 [ 122 , 123 ] and V 2 O 5 [ 29 , 124 ], and solution-
processed organic materials including PEDOT:PSS [ 99 , 112 , 113 ], SPDPA [ 125 ],
dextran-doped poly(allylamine hydrochloride) (PAH-D) [ 126 ], and cross-linkable
molecule N,N 0 -diphenyl-N,N 0 -bis-(3-methylphenyl)-(1,1 0 )-biphenyl -4,4 0 - dia-
mine- bis (vinyl benzyl ether) (TPD-BVB) [ 127 ]. The chemical structures of the
organic HTL materials are shown in Scheme 3.5 (PEDOT:PSS and SPDPA are
shown in Scheme 3.3 ).
3.3.2.1 PEDOT:PSS as HTL or Anode
The literature on HTL design of inverted solar cells is relatively scarce compared to
ETL. For solution-processed HTL PEDOT: PSS is often used. The challenge of
using PEDOT:PSS as HTL in an inverted device is that PEDOT:PSS is an aqueous
dispersion and it is difficult to coat it onto an organic active layer due to its
hydrophobic property. Cosolvent [ 99 ] or surfactants [ 112 ] are added to improve
interfacial compatibility of PEDOT: PSS and active layer. However, the confor-
mation of PEDOT:PSS using these methods was different and consequently its
work function and conductivity would be changed. Another way to uniformly
O
NH 3 +
O
O
O
N
Cl -
O
HO
HO
N
O
N
N
HO
OH
x
+ H 3 N
y
Cl -
PAH-D
TPD-BVB
Scheme 3.5
Chemical structures of organic HTL materials for inverted polymer solar cells
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