ࡱ> Root EntrypC;'FileHeaderNDocInfo[WBodyText $;K;+ !"#$%&'()*,-./Root EntrypC;'FileHeaderNDocInfo[WBodyText $;K;  u^>smG/\q puJeG-w}Iޗx &/mgj_ՖxFn &xXp ]g|#Wa~hn51tw DTcҍ:5C=nԟz?vGPxbKLrģ|efXf倮!GeLSs!rXcg6މ! eGˆ*Eyfehh'nBz&OƗbB% ~1꩝Ŷh^5"hFa* bN*+h"杯n&qj [ Ze(-:yNƦ .B6UEJ.MHꋝ&_.YҚFRStfszh ri櫈 \o!Vr.kƭ:X1 6JGC*TX2\ 6IT>#ѷ˞̧/n'$Q8ܕ+i(5+7(ݒ-Aϙן=<+pҷ9$␤yˌ~,5JD +'0VrS}/>KU<*cD&8I~듙ld JKd-c@ٲt1+Es|yrc) r-l[&0fsYt|CwQl'-7#(f3~? "PbzY#hb Z8$}V):IVu>/Tآ8`=VW}iQo/_ kҮגn(IVS~4 3[9Αf0UG]xI_=,5c6J٫M+تx 0D[h̀^7ۭw'DNi2FQ̸83rus99S/ǁJ'wҗ;PԧN[XϺַ{`NhOHWP Document File;@DO 6C,H,#GB!k0~ 6*7=M*Z:ҙ`a``a`0x  p | ajou2010D 2 10| ”| $ 2:36:28USER,9, 0, 0, 562 WIN32LEWindows_Unknown_Version@m @K;@WkAf&DZb)hX hKmxzT)hDSԄ@peQTi+.~佶}^ 1jDI.s&c1ppXfYU6>g2g(F [` LZEviƇT]P¤?:,gpAXM[RJR="_i"Z\ʘw;뼿 Pf ̎fgG슮],م1~Q0MnmY>YϪcM"Il5gv]JZ}UkǴ`!T|S+v.iguj-72 p"OڵUlk8EBQ]Gfxj'X{&Nrnj`Ͽ,&zLAԼZ<9\E3)k)tw %Ӝ>;Ϥd'0Mձ̧Cb'ݘ!6/l?$S<51'N|'d4&$6^'<}MJc37E>zp3͊NLW0GiElݴɈ`Gc&3yu;Ҧl; 'I򰻌}9/h 98ַ[f%-s4Ʋ)c;풽KAߞ`>P v)S^r`SH4hDKmD  M8 6 v6 [8an4f# @ѝ @. u8 c0 m%ٟyU*Ȓ~_fT!!u@DO 6C,H,#GB!k0~ 6*7=M*Z:ҙ#?*?ӿT@Y~X+mj3'm[v|:j)%C$Mϼ5#cd߈ulate the experimental results with the same fitting parameter values from the presented model. The validity of this model is also proven by a combination of other independent, steady state, and transient experimental techniques. This new powerful analytica>W1lU=3, [D. 0N8@b(뻵ovun"T4.("!HH Ӡ4H),h"*Ey}^Vf2m93DrswTz-U@%~ͨ|NιK%ulܴ˼Ief4%C[g3F~.J'sg5yzşձӥ9qF?|yd]1nIλLnΓezhx@{4y͵jOSL[^)W;'TD49<׃KFrT‹$yu cu]w$tt `p7~mYc5D%N!q%=Ն!Fx| e=E Q>z9Ԗ]]~ Q̬FKR>4a;GyBc$+˾lH3i=cϲD0h\c(^J@#]Oc&_yoP0h3k 4C|d,aUVA h,- 6uX:o8i.!,3LYL1G1$Z#BxG32՝bfGv{2Yk1PsfcZ %!$Fi&TP?3v~v5c xTX[E?MDTkpe ߄ Sy{O '"65?=觬qrW:Z~Si -T![|AaEO5ٺȩ$g{T3Su|9N_߾QOꅜ1зn@RZ~-mVx,q+!h&}vݧ m~wh-:C{]wڻ}f j=nЋZ+8\M 6No%hZ|=AJ0J񂠵ک(!$95۵"/Y<<p8P.aJNͬ.zt (#dR5O od֒2̷Ӯ9 6݆ 0t~[+zW#f`KlqUb[O g 5CMl u7:n;JXL=";#T6V[N^ 숻/) < ~)u*JV?J'G?oM.Z)VF k>S[ x_C~(SK< ]|fZSTq87"rnK&T4 h,Q3m!QVLR ğ)l005wyУUs"iN5V9]9V5 97qI$cO-98zĘp%/oMWwyCXˢ&TLpF\ŒTGaH?O1w3c9%(q&&rzt"YͿ$T#'qmiHwpSummaryInformation.SPrvImage PrvTextDocOptions pC;pC;Scripts pC;pC;JScriptVersion p DefaultJScriptm_LinkDocq Section0z !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMROPQTUVWXYZ\]^_`abcdefghijklnorstuvwxy{|}~ !"#$%&'()*+,-./0123456789:;<=>?@ABCDEFGHIJKLMROPQTUVWXYZ\]^_`abcdefghijklnorstuvwxy{|}~HwpSummaryInformation.SPrvImage PrvTextDocOptions pC;pC;Section0zScripts pC;pC;JScriptVersion p DefaultJScriptm_LinkDocq 8] <\><Quantifying the Nongeminate Recombination Dynamics in Nonfullerene Bulk Heterojunction Organic Solar Cells> <\Դ><In this study, a comprehensive analytical model to quantify the total nongeminate recombination losses, originating from bimolecular as well as bulk and surface trap assisted recombination mechanisms in nonfullerene based bulk heterojunction organic solar cells is developed. This proposed model is successfully employed to obtain the different contributions to the recombination current of the investigated solar cells under different illumination intensities. Additionally, the model quantitatively describes the experimentally measured open circuit voltage versus light intensity dependence. Most importantly, it is possible to calculate the experimental results with the same fitting parameter values from the presented model. The validity of this model is also proven by a combination of other independent, steady state, and transient experimental techniques. This new powerful analytica>GIF89aɻxxxkkk]]]PPPCCC555((( d`LH00`Hذ̘`H0|pdXL@`0H `H0`dHL`H0xp`XH@0d LȰ``HH00dLؘȀ`H0xp`XH@d0L `H0d`LH`H0|pdXL@0`$H`dHL00`HذȘdL0xp`XH@0` HdH0ȳ``HHdL0xp`XH@`0H Ը̰ĠऀؘpȈXxHp@h@d8`8X0xT0pH dxddxd`d`p`|``x`p``x`!, H*\ȰÇ#JHŋ3jȱǏ CIɓ(S\ɲ˗0cʜI͛8sɳϟ@ JѣH*]ʴӧPJJիXjʵׯ`ÊKYv`iTݵtʥ-[uẃ+^̸1Ð#KL˘/ ЯhIfHzewz.چk;/oܿΞ-u^>smG/\q puJeG-w}Iޗx &/mgj_ՖxFn &xXp ]g|#Wa~hn51tw DTcҍ:5C=nԟz?vGPxbKLrģ|efXf倮!GeLSs!rXcg6މ! eGˆ*Eyfehh'nBz&OƗbB% ~1꩝Ŷh^5"hFa* bN*+h"杯n&qj [ Ze(-:yNƦ .B6UEJ.MHꋝ&_.YҚFRStfszh ri櫈 \o!Vr.kƭ:X1 6JGC*TX2\ 6IT>#ѷ˞̧/n'$Q8ܕ+i(5+7(ݒ-Aϙן=<+pҷ9$␤yˌ~,5JD +'0VrS}/>KU<*cD&8I~듙ld JKd-c@ٲt1+Es|yrc) r-l[&0fsYt|CwQl'-7#(f3~? "PbzY#hb Z8$}V):IVu>/Tآ8`=VW}iQo/_ kҮגn(IVS~4 3[9Αf0UG]xI_=,5c6J٫M+تx 0D[h̀^7ۭw'DNi2FQ̸83rus99S/ǁJ'wҗ;PԧN[XϺַ{`NhOHWP Document File;@DO 6C,H,#GB!k0~ 6*7=M*Z:ҙ`a``a`0x  p | ajou2010D 2 10| ”| $ 2:36:28USER,9, 0, 0, 562 WIN32LEWindows_Unknown_Version@m @K;@WkAf&DZb)hX hKmxzT)hDSԄ@peQTi+.~佶}^ 1jDI.s&c1ppXfYU6>g2g(F [` LZEviƇT]P¤?:,gpAXM[RJR="_i"Z\ʘw;뼿 Pf ̎fgG슮],م1~Q0MnmY>YϪcM"Il5gv]JZ}UkǴ`!T|S+v.iguj-72 p"OڵUlk8EBQ]Gfxj'X{&Nrnj`Ͽ,&zLAԼZ<9\E3)k)tw %Ӝ>;Ϥd'0Mձ̧Cb'ݘ!6/l?$S<51'N|'d4&$6^'<}MJc37E>zp3͊NLW0GiElݴɈ`Gc&3yu;Ҧl; 'I򰻌}9/h 98ַ[f%-s4Ʋ)c;풽KAߞ`>P v)S^r`SH4hDKmD  M8 6 v6 [8an4f# @ѝ @. u8 c0 m%ٟyU*Ȓ~_fT!!u@DO 6C,H,#GB!k0~ 6*7=M*Z:ҙ#?*?ӿT@Y~X+mj3'm[v|:j)%C$Mϼ5#cd߈ulate the experimental results with the same fitting parameter values from the presented model. The validity of this model is also proven by a combination of other independent, steady state, and transient experimental techniques. This new powerful analytica>W1lU=3, [D. 0N8@b(뻵ovun"T4.("!HH Ӡ4H),h"*Ey}^Vf2m93DrswTz-U@%~ͨ|NιK%ulܴ˼Ief4%C[g3F~.J'sg5yzşձӥ9qF?|yd]1nIλLnΓezhx@{4y͵jOSL[^)W;'TD49<׃KFrT‹$yu cu]w$tt `p7~mYc5D%N!q%=Ն!Fx| e=E Q>z9Ԗ]]~ Q̬FKR>4a;GyBc$+˾lH3i=cϲD0h\c(^J@#]Oc&_yoP0h3k 4C|d,aUVA h,- 6uX:o8i.!,3LYL1G1$Z#BxG32՝bfGv{2Yk1PsfcZ %!$Fi&TP?3v~v5c xTX[E?MDTkpe ߄ Sy{O '"65?=觬qrW:Z~Si -T![|AaEO5ٺȩ$g{T3Su|9N_߾QOꅜ1зn@RZ~-mVx,q+!h&}vݧ m~wh-:C{]wڻ}f j=nЋZ+8\M 6No%hZ|=AJ0J񂠵ک(!$95۵"/Y<<p8P.aJNͬ.zt (#dR5O od֒2̷Ӯ9 6݆ 0t~[+zW#f`KlqUb[O g 5CMl u7:n;JXL=";#T6V[N^ 숻/) < ~)u*JV?J'G?oM.Z)VF k>S[ x_C~(SK< ]|fZSTq87"rnK&T4 h,Q3m!QVLR ğ)l005wyУUs"iN5V9]9V5 97qI$cO-98zĘp%/oMWwyCXˢ&TLpF\ŒTGaH?O1w3c9%(q&&rzt"YͿ$T#'qmi