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(1)

w

ŠA 0V ê sy ¢ Œ Ÿ «€ ¾X ì È ”  ôQ ß O Ë ù p § T “ Ó Þ” X ¢ w

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*

× <:   · T g ` @¬ £ · ™ »6 0Œ ‰ x · ™ »+ ä  ÷ 7 B

“

 …  ;@ /† < Ɠ § Ó ü t o † < Æõ , “  …  ; 406-772

ƒ

‘

š ò 6 B0 ² ? · ® £ . > ¬ £

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¦ 9@ /† < Ɠ § Ó ü t o † < Æõ , " fÖ  ¦ 136-713

(2010¸   5 Z 4 7{ 9  ~ à Î6 £ §, 2010¸   8 Z 4 26{ 9  à º& ñ ‘ : r ~ à Î6 £ §, 2010¸   9 Z 4 14{ 9  > F  S X ‰& ñ )

Ä

ºo   H µ 1 Ï F g “ ¦ì  r  “   poly(3-methylthiophene) (P3MT) ü < Au ” ¸# 4 Ü ¼– Ð s À Ò# Q”   “ ¦ì  r   /F K5 Å q s

7 á x  ” ¸‚  _  photoluminescence (PL) [ jl  ° ú   H { 9   F g _  ¼ # F g ~ ½ ӆ ¾ Ó\  @ /ô  Ç _ ” > r • ¸\  ¦ ƒ  ½ ¨ % i 



. { 9   F g _  ¼ # F g ~ ½ ӆ ¾ Ó`  ¦ ] j# Q½ + É Ã º e ”   H / B N œ í& h  ‰ & ³p  â `  ¦ s 6   x # Œ é ß –{ 9   ” ¸‚  _  / B N œ í& h  ‰ & ³p  â PL s p f ç `  ¦ à º' Ÿ † < ÊÜ ¼– Ð" f { 9   F g ¼ # F g \  @ /ô  Ç s 7 á x  ” ¸‚  _  PL [ jl  _ ” > r • ¸\  ¦ & ñ | ¾ Ó& h Ü ¼– Ð ì  r$ 3 ½ + É Ã

º e ” % 3  . ƒ  ½ ¨   õ  { 9   F g _  ¼ # F g ~ ½ ӆ ¾ Ós   ” ¸‚  õ  ¨ î ' Ÿ ½ + É M : à ºf ” { 9  M :˜ Ð   © œ@ /& h Ü ¼– Ð 30 ∼ 40

% PL [ jl  7 £ x ô  Ç  כ Ü ¼– Ð   z Œ ¤ . s  Qô  Ç ‰ & ³ © œ“ É r F K5 Å q  ” ¸# 4 s  \ O   H P3MT  ” ¸‚  \ " f• ¸ q 5 p w ô

 Ç Ã ºï  r Ü ¼– Ð 8 £ ¤& ñ ÷ &# Q { 9   F g ¼ # F g _ ” > r • ¸  H F K5 Å q  ” ¸# 4 _  Ä »Á ºü <  H › ' aº  s  \ O   H  כ Ü ¼– Ð   z Œ ¤ .

Ù þ

˜d ” # Q: / B N œ í& h ‰ & ³p  â , “ ¦ì  r    ” ¸‚  , + þ AF g, ¼ # F g

Study of the Dependence of the Photoluminescence Intensity of Hybrid Nanowires on the Polarization Direction by Using a High-resolution Laser

Confocal Microscope

Yun Saena · Hyunsoo Lee · Dae-chul Kim · Jenogyong Kim

Department of Physics, University of Incheon, Incheon 406-772

Dong Hyuk Park · Jinsoo Joo

Department of Physics, Korea University, Seoul 136-713

(Received 7 May, 2010 : revised 26 August, 2010 : accepted 14 September, 2010)

We studied the dependence of the photoluminescence (PL) intensity of poly (3-methylthiophene) (P3MT)-Au hybrid nanowires on the polarization direction of the input illumination. We used a high-resolution laser confocal microscope and obtained and quantitatively analyzed the PL images of P3MT-Au nanowires for various input illumination polarizations. We found that about 30 ∼ 40%

relative increase in the PL intensity when the polarization of the input illumination was parallel to the nanowires over as compared to when it was perpendicular to the nanowire. This result was similarly observed for P3MT nanowires without a Au nanowall, indicating that the input polarization dependence of PL intensity of P3MT nanowires has no correlation with the presence of the Au nanowall.

-1007-

(2)

PACS numbers: 42.25.Ja,07.60.Pb,78.30.Jw

Keywords: Confocal microscope, Polymer nanowire, Photoluminescence, Polarization

I. " e  ] Ø

µ

1 Ï F g “ ¦ì  r  – Ð @ /³ ð& h “   Ó ü t| 9 “   e  ¦ o   [ j 9 E $ ™“ É r π-/ B N Ó 

o½ ¨› ¸\  ¦ t Ù ¼– Ð • ¸^ ‰ü < ° ú  “ É r „  l & h  „  • ¸ $ í | 9 `  ¦ 

”

   [1]. ‘ : r ƒ  ½ ¨\ " f  6   x ô  Ç Poly(3-methylthiophene) (P3MT)  ” ¸‚  “ É r e  ¦ o   [ j 9 E $ ™õ   ð ø Ít – Ð π-/ B NÓ  o

½

¨› ¸\  ¦ t   H µ 1 Ï F g “ ¦ì  r   Ó ü t| 9 – Ð „  l  x 9 F g ì ø Í6 £ x$ í s

 Ä ºÃ º  . : £ ¤ y   ” ¸‚   ü @# 4 \  F K5 Å q  ” ¸# 4 `  ¦ t • ¸ 2

Ÿ

¤ ] j Œ •ô  Ç “ ¦ì  r  /F K5 Å q s 7 á x  ” ¸‚  “ É r { 9 ì ø Í µ 1 Ï F g “ ¦ì  r  



” ¸‚  ˜ Ð  F g ì ø Í6 £ x$ í s  Ä ºÃ º # Œ, : £ ¤ y  PL [ jl  ß ¼

>

 7 £ x ô  Ç . s % ƒ! 3  µ 1 Ï F g “ ¦ì  r  ü < F K5 Å q Ü ¼– Ð ë ß –[ þ t # Q”   s

7 á x  ” ¸‚  “ É r Ä »l µ 1 Ï F g ™ è – Ð" f  € ª œô  Ç 6 £ x6   x s  l @ /÷ &



 H Ó ü t| 9 s   [2,3]. s 7 á x ½ ¨› ¸\  ¦ t   H µ 1 Ï F g “ ¦ì  r    

”

¸‚  _  PL: £ ¤$ í “ É r † ¾ ÓÊ ê  ” ¸ F g ™ è , ™ èF ì  r  \ " f 6 £ x6   x

| ¨

c  כ Ü ¼– Ð \ V © œ÷ &# Q “ ¦ì  r    ” ¸‚   PL[ jl   H ´ ú §“ É r ƒ  ½ ¨

 € 9 כ ¹  . s p  F K5 Å q  ” ¸‚  , F K5 Å q  ” ¸{ 9  _  ¼ # F g ~ ½ Ó

†

¾ Ó\    É r  ë ß –í ß –ê ø Íõ  PL: £ ¤$ í “ É r ´ ú §“ É r ƒ  ½ ¨ ˜ Г ¦ ÷ &% 3 



 [4–6]. t ë ß –  f ”  µ 1 Ï F g “ ¦ì  r   s 7 á x  ” ¸‚   PL: £ ¤$ í _

 ¼ # F g _ ” > r$ í \  @ /K " f  H ˜ Г ¦  ) a   \ O  . / B N œ í& h  ‰ & ³ p

 ⠓ É r { 9 ì ø Í F g † < Æ ‰ & ³p  â õ   Ø Ô>  œ í& h d ” • ¸ ± ú   œ í

&

h \ " f # Á # Qè ß –  © œ“ É r ] j  “ ¦ r « Ñ  © œ\  ë “ B“ É r œ í& h \ " f ë

ß –  © œ`  ¦  Ž Ø  ¦ K  ? /Ù ¼– Ð Z  }“ É r K  © œ• ¸ü < – B H à Ô Û ¼à Ô\  ¦  t

  H  © œ`  ¦ % 3 # Qè ­ q à º e ”   H F g † < Æ ‰ & ³p  â s  . Ä ºo   H é ß – { 9

 “ ¦ì  r  /F K5 Å q s 7 á x  ” ¸‚  `  ¦ “ ¦K  © œ• ¸ / B N œ í& h  ‰ & ³p  â

`

 ¦ s 6   x ô  Ç PL s p f ç `  ¦ : Ÿ x K  { 9   F g ¼ # F g _ ” > r$ í `  ¦ ƒ  

½

¨ % i  .

II. ÷ m Ç] M ö U ê s0 n É

1. P3MT Ñ ÷ P3MT-Au  x ¢š ½¬ Ž8 ý ¶  ¥V R Ë

‘

: r ƒ  ½ ¨\ " f  6   x ô  Ç µ 1 Ï F g “ ¦ì  r    ” ¸‚  õ  Au  ” ¸

# 4

`  ¦ t   H µ 1 Ï F g “ ¦ì  r   s 7 á x  ” ¸‚  “ É r „  l  o† < Æ ×  æ

½

+ Ë~ ½ ÓZ O `  ¦ s 6   x # Œ ] j Œ • % i   [7].  ” ¸ l / B N`  ¦  t

  H Al

2

O

3

template ô  ÇA á ¤ \  Á ºl  7 £ x ‚ à Ìl \  ¦  6   x # Œ F

K`  ¦ 7 £ x ‚ à Ìô  Ç Ê ê • ¸ˆ  à Ô, 6   x B ü < é ß –| ¾ Ó^ ‰– Ð s À Ò# Q”   6   x Ó 

o`  ¦ t “ ¦ template_   ” ¸l / B N î ß –\ " f $ í  © œr †   .



6   x ) a • ¸ˆ  à ԍ  H tetrabutylammonium hexafluorophos- phat s  9, acetonitrile`  ¦ 6   x B – Ð  6   x % i  . • ¸ˆ  à Ôü <

E-mail: [email protected]

Fig. 1. Schematic of the confocal microscope to control the direction of input polarization.

6  

x B – Ð s À Ò# Q”   6   xÓ  o\  cyclic voltammetry– Ð • ¸i ç  © œI 

\

 ¦ › ¸] X   9 F K5 Å q% i  6   xÓ  o`  ¦  6   x # Œ µ 1 Ï F g “ ¦ì  r    ” ¸

‚

 \  F K5 Å q  ” ¸ # 4 `  ¦ { 9 ˜ 2 ³ . s ü < ° ú  s  templateî ß –\ " f



” ¸‚  `  ¦ $ í  © œr †   Ê ê\  HF  NaOH à º6   xÓ  oÜ ¼– Ð tem- plate\  ¦ ] j  # Œ Au ” ¸# 4 `  ¦ t   H µ 1 Ï F g “ ¦ì  r   s 7 á x



” ¸‚  `  ¦ ] j Œ • % i  .

2. w ŠA 0V ê sy ¢ Œ Ÿ «€ ¾X ì È ”  ôQ ß O ËÊ Ý ø m É  Ű Ë Ñ{ ¢ô o Ú

µ

1 Ï F g “ ¦ì  r   s 7 á x  ” ¸‚  \ " f PL_  [ jl _  ¼ # F g _ ” > r

$ í

`  ¦ ƒ  ½ ¨ l  0 AK  • ¸w n F g † < Æ ‰ & ³p  â `  ¦ > h› ¸ # Œ ] j Œ •

 )

a / B N œ í& h  ‰ & ³p  â `  ¦ s 6   x % i   [8, 9]. { 9   ¼ # F g \  @ / ô

 Ç PL[ jl _     o\  ¦ ˜ Ðl 0 A # Œ { 9   F g _  Y Us $  [ jl 



 H { 9 & ñ >  Ä »t  €  " f { 9   ¼ # F g ~ ½ ӆ ¾ Ó`  ¦  Ä »\  v >    



or ~  ´ à º e ”   H  © œu  € 9 כ ¹  . Fig. 1\  ‚  + þ A¼ # F g ó ø Í õ

 λ/4 0 A © œó ø Í\  ¦  6   x # Œ ] j Œ •ô  Ç { 9  ¼ # F g > _  F g † < Æ > h

¥ Æ

• ¸    e ”  . Single mode (SM) F g$ 3 Ä »\ " f ( 4 R



š ¸  H Y Us $  F g“ É r q ½ ¨€   E $ ™Ý ¼\  ¦ s 6   x K  ¨ î ' Ÿ F g`  ¦ ë ß –

Ž

 H Ê ê ‰ & ³p  â ? / Ò\  { 9  r v   H X < s  ¨ î ' Ÿ F g _  ¼ # F g ~ ½ Ó

†

¾ Ó`  ¦ › ¸] X  # Œ r « Ñ\  { 9   r †   . Ä º‚   ‚  + þ A¼ # F g ó ø Í`  ¦ SMF g$ 3 Ä » · ú ¡\  ¿ º# Q ‚  + þ A¼ # F g ~ ½ ӆ ¾ Ó`  ¦ t • ¸2 Ÿ ¤ ë ß –Ž  H  .

s

 ‚  + þ A¼ # F g ó ø Í`  ¦ 45

– Ð l Ö  ¦ # Œ λ/4 0 A © œó ø Í\  { 9   • ¸ 2

Ÿ

¤ €   " é ¶+ þ A¼ # F g s  ë ß –[ þ t # Q ”   . λ/4 0 A © œó ø Í + '\  ‚  + þ A

¼

# F g ó ø Í`  ¦ ¿ º# Q y Œ • ¼ # F g ~ ½ ӆ ¾ Ó   Y Us $ _  [ jl  { 9 & ñ

“ ¦ Õ ª ~ ½ ӆ ¾ Ó`  ¦  Ä »\  v >  › ¸] X s  0 p x ô  Ç { 9  ¼ # F g`  ¦ ë ß – [

þ t% 3  .

¿

º> h_  ‚  + þ A ¼ # F g ó ø Íõ  λ/4 0 A © œó ø Í`  ¦  5 g Ò q t$ í K  · p Y

Us $  F g“ É r r « Ñ\  { 9   l  „  \  ¼ # F g ~ ½ ӆ ¾ Ós  › ¸] X ÷ &

(3)

Fig. 2. Laser confocal PL images of P3MT-Au nanowires with two direct directions of input polarization. (a),(c) 0

(X-direction), (b)(d) 90

(Y-direction)

#

Q 50/50 beam splitter\  ¦  5 g r « Ñ\  • ¸² ú ˜ô  Ç . F g " é ¶ Ü ¼

–

Ð argon ion Y Us $ _  514 nm  © œ`  ¦  6   x % i Ü ¼ 9, { 9 

§ 4

F g [ jl   H 0.01 µW ∼ 0.04 µW% i  . r « Ñ\  ¦ # Œl  r 

† 

 Ê ê í ß –ê ø Í  ) a y n C“ É r  r  beam splitterü < long pass edge- filter\  ¦  5 g detector\  | 9 F g r &  F g [ jl \  ¦ 8 £ ¤& ñ % i 



. ‘ : r ƒ  ½ ¨\ " f  6   x ô  Ç detector– Ѝ  H current mode PMT ü

< photo counting APD\  ¦  6   x % i  . r « ѓ   P3MT 

”

¸‚  õ  P3MT-Au ” ¸‚  “ É r Ä »o l ó ø Í0 A\  ì  r í ß –r (  Ü ¼ 9, /

B

N œ í& h ‰ & ³p  â _  xy-stage 0 A\  `  ¦§ 4  . @ /Ó ü tE $ ™Ý ¼(N.A. = 1.4 Oil-immersion)\  ¦ s 6   x # Œ r « Ñ\  œ í& h `  ¦ ´ ú Æ Ò% 3  .

Ä

ºo   H x − y stage _  x» ¡ ¤ \  @ / # Œ ¼ # F g ~ ½ ӆ ¾ Ó`  ¦ y Œ •y Œ • 90

, 45

, 0

, −45

, −90

– Ð    o\  ¦ Å Ò# Q Õ ª\    É r r « Ñ_  PL s

p t \  ¦ % 3 # Q PL[ jl \  ¦ & ñ | ¾ Ó& h Ü ¼– Ð q “ § % i  .

III. ÷ m Ç] M ö + s ÇÊ Ý õ m Í ‚ º8 ý

Figure 2  H { 9  ¼ # F g ~ ½ ӆ ¾ Ó`  ¦    or v €  " f S \ ‰1 p q ô  Ç P3MT-Au  ” ¸‚  _  / B N œ í& h ‰ & ³p  â PL s p t [ þ t s  .  © œ

@

/& h Ü ¼– Ð Ã ºf ” Ü ¼– Ð Z  ~“   ¿ º  ” ¸‚  `  ¦ ¹ 1 Ô  PLs p t \  ¦

% 3

% 3  . (a)ü < (b) Õ ªo “ ¦ (c)ü < (d)  H ° ú  “ É r % ò % i `  ¦ { 9  ¼ #  F

g ~ ½ ӆ ¾ Óë ß –`  ¦ ² ú ˜o  # Œ ƒ  5 Å q& h Ü ¼– Ð % 3 “ É r PL s p t s  .

U

 ´s  à º µm_  P3MT-Au ” ¸‚  s  Ì º§  s     e ”  .



” ¸‚  s  ] j Œ • | ¨ c M : Ô  ¦ç  H{ 9  >  • ¸i ç ÷ &# Q ° ú  “ É r  ” ¸‚  

?

/\ " f• ¸ PL[ jl   Òì  r& h Ü ¼– Ð › ¸F Km ”  s     H  כ Ü

¼– Ð Ò q ty Œ •  ) a  . Fig. 2  H s p t  Û ¼H { 9 `  ¦ e ” _ – Ð › ¸] X 

# Œ % 3 “ É r  © œ@ /& h  PL[ jl  s p t s  .

(a) ü < (c)  H { 9  ¼ # F g ~ ½ ӆ ¾ Ó 0

– Ð { 9   % i `  ¦ M :_  s p  t

s  9 (b)ü < (d)  H { 9  ¼ # F g ~ ½ ӆ ¾ Ós  90

“   PLs p t s 



. { 9  ¼ # F g ~ ½ ӆ ¾ Ós  0

“   (a)_  PLs p t \ " f ¼ # F g ~ ½ ӆ ¾ Ó õ

  ê ø Íô  Ç `   P3MT-Au ” ¸‚  _  PL [ jl   © œ@ /& h Ü ¼

–

Ð ¼ # F g ~ ½ ӆ ¾ Ó\  à ºf ” Ü ¼– Ð 0 Au K  e ”   H a   P3MT-Au 

”

¸‚  ˜ Ð   8  p u`  ¦ S X ‰ “   % i  . ì ø ̀  , a   P3MT-Au 

”

¸‚  “ É r  ê ø Í >  { 9     H ¼ # F g ~ ½ ӆ ¾ Ó`  ¦ t   H (b) \ " f

`   P3MT-Au ” ¸‚  ˜ Ð  PL[ jl   8¹ ¡ ¤ ß ¼ .  ð ø Í

t

– Ð { 9  ¼ # F g ~ ½ ӆ ¾ Ós  0

“   (c)\ " f ¼ # F g ~ ½ ӆ ¾ Óõ   ê ø Íô  Ç b   P3MT-Au ” ¸‚  s  c   P3MT-Au ” ¸‚  ˜ Ð  PL [

jl   © œ@ /& h Ü ¼– Ð ß ¼ 9, { 9  ¼ # F g ~ ½ ӆ ¾ Ós  90

“   (d)\ " f



 H s ü <  ê ø Í >  Z  ~“   c   P3MT-Au ” ¸‚  _  PL[ jl 

 b   P3MT-Au ” ¸‚  ˜ Ð  ß ¼ .

Figure 2 \    è ß – P3MT-Au ” ¸‚  [ þ t _  ¼ # F g ~ ½ ӆ ¾ Ó\ 



 É r PL [ jl \  ¦ Y-average l Z O `  ¦ s 6   x # Œ & ñ | ¾ Ó& h Ü ¼– Ð

% 3

“ É r   õ \  ¦ ³ ð 1\    ? /% 3  . z  ´] j– Ð 90

\ " f 0

– Ð { 9 



¼ # F g s   7 % 3 `  ¦ M : 7 £ x    H q Ö  ¦“ É r ì  r" î ô  Ç Æ Òs \  ¦



  · p . \ V\  ¦ [ þ t # Q `   P3MT-Au ” ¸‚  _   â Ä º 196 mV \ " f 407 mV– Ð 7 £ x  % i Ü ¼ , a   P3MT-Au ” ¸

‚

 _   â Ä º 241 mV\ " f 359 mV– Ð 1.49C  7 £ x    H X < Õ ª '

¬ I . s  כ “ É r 0

– Ð Z  ~“   `   P3MT-Au ” ¸‚  s  90

– Ð Z

 ~“   a   P3MT-Au ” ¸‚  ˜ Ð  { 9  ¼ # F g 0

\  @ /K  €  • 30 %  8 PL[ jl  7 £ x ô  Ç   H  כ `  ¦    · p . s  Qô  Ç ‰ & ³



© œ“ É r b   P3MT-Au ” ¸‚  õ  c   P3MT-Au ” ¸‚  \ 

"

f• ¸ q 5 p w ô  Ç Æ Òs – Ð › ' a ¹ 1 Ï÷ &% 3  .

ô

 Ç s p t  ? /\ " f_  — ¸Ž  H  ” ¸‚  “ É r  ê ø Íô  Ç { 9  ¼ # F g

~ ½

ӆ ¾ Ó`  ¦ | 9  M : PL[ jl   © œ@ /& h Ü ¼– Ð ß ¼>    z Œ ¤ .

Fig. 2(a)  H { 9  ¼ # F g ~ ½ ӆ ¾ Ó 0

– Ð ¼ # F g ~ ½ ӆ ¾ Óõ   ê ø Íô  Ç `



  P3MT-Au ” ¸‚  \ " f  H 407 mV, à ºf ” Ü ¼– Ð Z  ~“   a   P3MT-Au  ” ¸‚  \ " f 263 mV– Ð 8 £ ¤& ñ ÷ &% 3  . (a)ü < ° ú  “ É r



” ¸‚  \  @ /K  { 9  ¼ # F g ~ ½ ӆ ¾ Ó`  ¦ 90

– Ð    or †   (b)\ " f



 H    oô  Ç { 9  ¼ # F g õ   ê ø Í >  Z  ~“   a   P3MT-Au 

”

¸‚  \ " f 322 mV, à ºf ” Ü ¼– Ð Z  ~“   `   P3MT-Au ” ¸

‚

 \ " f  H 263 mV – Ð 8 £ ¤& ñ ÷ &% 3  . { 9  ¼ # F g ~ ½ ӆ ¾ Óõ   ê ø Í

>  { 9  ½ + É M : PL[ jl   © œ@ /& h Ü ¼– Ð 7 £ x  % i  .  ð ø Í

t – Ð Fig. 2(c)\ " f• ¸ { 9  ¼ # F g ~ ½ ӆ ¾ Óõ   ê ø Í >  Z  ~“   b   P3MT-Au ” ¸‚  s  711 mV– Ð Ã ºf ” Ü ¼– Ð Z  ~“   c   P3MT-Au  ” ¸‚  _  602 mV˜ Ð  Z  } >    z Œ ¤ . ¢ ¸ô  Ç { 9 



¼ # F g ~ ½ ӆ ¾ Ós  90

– Ð { 9   # Œ c   P3MT-Au ” ¸‚  õ 



ê ø Í >  Z  ~ s   Õ ª PL[ jl   H 322 mV – Ð 8 £ ¤& ñ ÷ &% 3 Ü ¼ 9 b   P3MT-Au ” ¸‚  “ É r 263 mV – Ð { 9  ¼ # F g ~ ½ ӆ ¾ Óõ    ê

ø Íô  Ç  ” ¸‚  ˜ Ð  PL[ jl  ± ú >  8 £ ¤& ñ ÷ &% 3  .

{ 9

 ¼ # F g ~ ½ ӆ ¾ Ó\  @ /ô  Ç  ” ¸‚  _  PL[ jl   H  ê ø Íô  Ç ¼ #  F

g ~ ½ ӆ ¾ Ó`  ¦ t   H  ” ¸‚  \  @ /K " f  © œ@ /& h Ü ¼– Ð Õ ª [ jl 

 [ j# Qf ” `  ¦ S X ‰ “   % i  . Õ ª Q  ì  r$ 3  ) a  ” ¸‚   4> h — ¸

(4)

Table 1. Measured PL values and the ratios of P3MT-Au nanowires with direct direction of input polarization.

Input polarization direction

P3MT-Au nanowires 90

45

0

−45

−90

PL intensity of the nanowire ` 263 373 407 283 196

PL intensity of the nanowire a 241 378 359 293 241

Intensity ratio between ` and a 0.817 0.987 1.13 0.966 0.813

PL intensity of the nanowire b 452 661 771 515 360

PL intensity of the nanowire c 549 623 602 520 444

Intensity ratio between b and c 0.823 1.06 1.18 0.990 0.811

Fig. 3. Laser confocal PL images of P3MT nanowires with two direct directions of input polarization. (a) 0

(X-direction), (b) 90

(Y-direction)

¿

º { 9  ¼ # F g ~ ½ ӆ ¾ Ós   ” ¸‚  _  U  ´s ~ ½ ӆ ¾ Óõ  ¨ î ' Ÿ     à º f ”

“    כ õ  › ' a > \ O s  ] X @ /& h “   PL[ jl   H — ¸¿ º 90

˜ Ð   H 0

\ " f  8 Z  }“ É r  כ Ü ¼– Ð   z Œ ¤ . s  כ “ É r z  ´+ « >\ " f  6   x

 )

a / B N œ í& h  ‰ & ³p  â ? / Ò_  50/50 beam splitter 90

˜ Ð 



 H 0

\  ¦ ‚    ñ l  M :ë  H s  . z  ´] j– Ð r ï  r ) a Y Us $  F g`  ¦ { 9

 r &  ‰ & ³p  â ? / Ò_  50/50 beam splitter_  ì ø Í Ö  ¦

`

 ¦ 8 £ ¤& ñ ô  Ç   õ  s¼ # F g  © œI “   90

 p¼ # F g  © œI “   0

˜ Ð 

€



• 1.4C   8 ì ø Í Ö  ¦ s  Z  }“ É r  כ Ü ¼– Ð 8 £ ¤& ñ ÷ &% 3  . ¢ ¸, ³ ð1`  ¦

˜

Ѐ   90

ü < −90

\ " f_  PL[ jl   H { 9  ¼ # F g ~ ½ ӆ ¾ Ós  ° ú   Ü

¼Ù ¼– Ð ° ú  “ É r   õ   ü <  † < Ê\ • ¸ Ô  ¦ ½ ¨ “ ¦ „  ì ø Í& h “  



” ¸‚  _  PL[ jl  y Œ ™™ è % i  .  ” ¸‚  s  { 9   F g \  # Œ



Q   ” ¸Ø  ¦ ÷ &# Q „  ì ø Í& h Ü ¼– Ð PL[ jl  y Œ ™™ èô  Ç  כ Ü ¼– Ð s 



 H Bleaching ´ òõ  ” > r F † < Ê`  ¦ € Œ ™r ô  Ç .  _   ” ¸‚  

`

 ¦ { 9   F g \  # Œ Q   ” ¸Ø  ¦ r &  z  ´] j z  ´+ « >° ú כ\   H à ºu & h  Ü

¼– Ð p [ j ˜ Ð& ñ s  # Q 9î  r כ ¹“  [ þ t s  0 l q  e ”  . Õ ª QÙ ¼– Ð PL [ jl \  ¦ 8 £ ¤& ñ ô  Ç z  ´+ « >° ú כ  ^ ‰\  ¦ q “ § l ˜ Ð   H   _

 PLs p t  ? /\ " f " f– Ð Ã ºf ” `  ¦ s À ҍ  H  ” ¸‚  `  ¦ s 6   x

# Œ PL[ jl  7 £ x y Œ ™`  ¦  © œ@ /& h “   q Ö  ¦ – Ð q “ §   H  כ s   

| Ã

Ðf ”   . 90

ü < 0

– Ð Z  ~“   " f– Ð Ã ºf ” ô  Ç ¿ º  ” ¸‚  \  @ /

# Œ ¼ # F g ~ ½ ӆ ¾ Ó`  ¦  Ë ¨# Q 9 PL s p t \  ¦ % 3 `  ¦  â Ä º z  ´ ]

j { 9  ÷ &  H Y Us $  F g | ¾ Ós  s  e ”    8 • ¸ ¿ º  

”

¸‚  s  ° ú  “ É r F g | ¾ Ó`  ¦ ~ à Î>  ÷ &Ù ¼– Ð, ¿ º  ” ¸‚  ç ß –_   © œ@ /& h 

“

  PL [ jl   H { 9   F g | ¾ Ó_  % ò † ¾ Ó`  ¦ ~ à Ît  · ú §  H  .

Table 1 \  0

\  à ºf ” ô  Ç P3MT-Au ” ¸‚  `  ¦ l ï  r Ü ¼– Ð



© œ@ /& h “   PL[ jl  7 £ x y Œ ™q Ö  ¦`  ¦ ³ ð1\  I

1

/I

2

ü < I

3

/I

4

– Ð  

? /% 3  . " f– Ð Ã ºf ” `  ¦ s À ғ ¦ e ”   H  ” ¸‚  _  y Œ •y Œ •_  { 9 



¼ # F g ~ ½ ӆ ¾ Ó\    É r  © œ@ /& h “   PL[ jl _  7 £ x y Œ ™ q Ö  ¦“ É r   6

£

§ õ  ° ú  “ É r ~ ½ ÓZ O Ü ¼– Ð ½ ¨ % i  .

{ 9

 ¼ # F g 90

_  `   P3MT ” ¸‚   PL[ jl  (mV) { 9

 ¼ # F g 90

_  a   P3MT ” ¸‚   PL[ jl  (mV) = 263mV

322mV = 0.817 { 9

 ¼ # F g 0

_  `   P3MT ” ¸‚   PL[ jl  (mV) { 9

 ¼ # F g 0

_  a   P3MT ” ¸‚   PL[ jl  (mV) = 407mV 359mV = 1.13

0

Aü < ° ú  “ É r ~ ½ ÓZ O Ü ¼– Ð { 9  ¼ # F g y Œ •• ¸\    É r  © œ@ /& h “   PL [ jl _  7 £ x y Œ ™q Ö  ¦`  ¦ ½ ¨ % i  . s ü < ° ú  “ É r ~ ½ ÓZ O Ü ¼– Ð 



_  s p t  ? /\ " f " f– Ð Ã ºf ” `  ¦ s À ҍ  H P3MT-Au  ” ¸

‚

 [ þ t s  { 9   ¼ # F g ~ ½ ӆ ¾ Ó\    É r  © œ@ /& h “   PL[ jl   H  ê ø Í ô

 Ç ¼ # F g ~ ½ ӆ ¾ Ós  [ þ t # Q𠏀   à ºf ” “   ¼ # F g ~ ½ ӆ ¾ Ós  { 9  ½ + É M :

˜

Ð  €  • 30 ∼ 40 % 7 £ x ô  Ç “ ¦ ^  ¦ à º e ”  .

° ú

 “ É r ~ ½ Ód ” Ü ¼– Ð F K  ” ¸# 4 `  ¦ t t  · ú §  H P3MT  ” ¸

‚

  PL[ jl \  @ /ô  Ç { 9  ¼ # F g _ ” > r$ í `  ¦ ƒ  ½ ¨ % i  . Fig.

3“ É r { 9   ¼ # F g ~ ½ ӆ ¾ Ó\    É r P3MT  ” ¸‚  _  PLs p t s 



. (a)\ " f  H `   P3MT ” ¸‚  õ  { 9   ¼ # F g ~ ½ ӆ ¾ Ós   

(5)

Fig. 4. Dependence of relative PL intensities of P3MT- Au nanowires and P3MT nanowires on the input polar- ization direction. (Three pairs of P3MT-Au nanowires and two pairs of P3MT nanowires are used for this plot).

ê

ø Í “ ¦ (b)\ " f  H a   P3MT ” ¸‚  \   ê ø Íô  Ç ¼ # F g ~ ½ ӆ ¾ Ó _

 y n Cs  { 9  ô  Ç . P3MT-Au ” ¸‚  _  { 9  ¼ # F g _  _ ” > r

$ í

õ   ð ø Ít – Ð ¼ # F g ~ ½ ӆ ¾ Ós  P3MT ” ¸‚  õ   ê ø Íô  Ç ~ ½ Ó

†

¾ ÓÜ ¼– Ð [ þ t # Q`  ¦ M : PL_  [ jl   © œ@ /& h Ü ¼– Ð 7 á §  8 [ j# Q t

  H  כ `  ¦ S X ‰ “   % i  . a   P3MT ” ¸‚  “ É r (b) \ " f [ þ t

#

Qš ¸  H { 9   ¼ # F g ~ ½ ӆ ¾ Óõ   ê ø Í Ù ¼– Ð Ã ºf ” Ü ¼– Ð { 9     H (a) \ " f_  PL[ jl ˜ Ð  (b)\ " f_  PL[ jl   © œ@ /& h Ü ¼– Ð



8 y © œK t   H  ⠆ ¾ Ó`  ¦ ˜ Г   . s    õ   H P3MT-Au  ” ¸‚   õ

 P3MT ” ¸‚  “ É r { 9  ¼ # F g ~ ½ ӆ ¾ Ó\    É r PL [ jl   

”

¸‚  \   ê ø Íô  Ç ~ ½ ӆ ¾ ÓÜ ¼– Ð { 9     H ¼ # F g ~ ½ ӆ ¾ Ó`  ¦ ‚    ñ # Œ PL [ jl  7 £ x ô  Ç   H  כ `  ¦ ˜ Ð# Œï  r  .

Figure 4 \  { 9   ¼ # F g ~ ½ ӆ ¾ Ó\  @ /ô  Ç P3MT-Au ” ¸‚   õ

 P3MT ” ¸‚   PL[ jl _   © œ@ /& h  [ jl q Ö  ¦ _     o\  ¦ Õ

ªA á Ԗ Ð   ? /% 3  .  _  s p t  î ß –\ " f " f– Ð Ã ºf ” 

`

 ¦ s À ҍ  H ¿ º  ” ¸‚  _   © œ@ /& h  [ jl q Ö  ¦`  ¦ { 9  ¼ # F g ~ ½ Ó

†

¾ Ó 90

\ " f_  ° ú כÜ ¼– Ð ½ ©   o # Œ  © œ@ /& h “   q Ö  ¦ – Ð   



· p Õ ªA á Ôs  . y Œ • PLs p t     © œ@ /& h “   [ jl q Ö  ¦  



o\  ¦  6 £ § õ  ° ú  “ É r ~ ½ ÓZ O Ü ¼– Ð ½ ¨ % i  . Fig. 2ü < Fig. 3\ 



 è ß – 3Š © œ_   ” ¸‚  ü @\  ô  Ç Š © œ_  P3MT-Au ” ¸‚  õ  ô  Ç

Š

© œ_  P3MT ” ¸‚  `  ¦ Æ Ò– Ð ì  r$ 3  # Œ Õ ªA á Ô\  Ÿ í† < Ê 

% i  .

{ 9

 ¼ # F g 90

\ " f ` ” ¸‚  õ  a ” ¸‚  _   © œ@ /& h  Intensity I

1

/I

2

= 0.82 0.82 = 1.00 { 9

 ¼ # F g 45

\ " f ` ” ¸‚  õ  a ” ¸‚  _   © œ@ /& h  Intensity I

1

/I

2

= 0.99 0.82 = 1.21 { 9

 ¼ # F g 0

\ " f ` ” ¸‚  õ  a ” ¸‚  _   © œ@ /& h  Intensity I

1

/I

2

= 1.13 0.82 = 1.38 { 9

 ¼ # F g -45

\ " f ` ” ¸‚  õ  a ” ¸‚  _   © œ@ /& h  Intensity I

1

/I

2

= 0.97 0.82 = 1.18 { 9

 ¼ # F g -90

\ " f ` ” ¸‚  õ  a ” ¸‚  _   © œ@ /& h  Intensity I

1

/I

2

= 0.81

0.82 = 0.988

Õ

ªA á Ô\ " f " î S X ‰ y  × ¼ Q 1 p w s  P3MT-Auü < P3MT ” ¸

‚

 “ É r { 9  ¼ # F g ~ ½ ӆ ¾ Ós  à ºf ” Ü ¼– Ð { 9  ½ + É M : ˜ Ð  { 9   ¼ #  F

g s   ” ¸‚  õ   ê ø ͽ + É M : Õ ª [ jl   H €  • 30 ∼ 40% 7 £ x  ô

 Ç   H  כ `  ¦ · ú ˜ à º e ”  .

P3MT  ” ¸‚  _  U  ´s ~ ½ ӆ ¾ Ó ¼ # F g { 9   F g \  @ /ô  Ç PL [ j l

_  7 £ x ‰ & ³ © œ“ É r í ß –ê ø Í´ òÖ  ¦ _  s \  _ ô  Ç  כ Ü ¼– Ð Æ Ò8 £ ¤

 )

a  . ò ø ͙ è ” ¸‚  _   â Ä º s ü < q 5 p w ô  Ç ‰ & ³ © œs  s p  ˜ Г ¦

 )

a   e ”   [10,11]. P3MT  ” ¸‚  s  Au  ” ¸# 4 _  Ä »Á º ü

< › ' a > \ O s  q 5 p w ô  Ç { 9  ¼ # F g _ ” > r • ¸\  ¦ ° ú   H  כ Ü ¼– Ð ˜ Ð



 › ' a8 £ ¤ ) a PL [ jl _  { 9  ¼ # F g _ ” > r • ¸  H Au F K5 Å q  ” ¸# 4  _

 % i ½ + ɘ Ð   H  ” ¸‚  _  l  † < Æ& h “   + þ AI \  l “  ô  Ç  כ Ü

¼– Ð \ V8 £ ¤ ) a  .

IV. + s Ç Â ] Ø

Ä

ºo   H “ ¦K  © œ• ¸ / B N œ í& h  ‰ & ³p  â `  ¦ s 6   x # Œ µ 1 Ï F g  ” ¸

‚

 “   P3MT ” ¸‚  õ  F K  ” ¸# 4 `  ¦ t   H P3MT-Au  

”

¸‚  _  { 9  ¼ # F g \  @ /ô  Ç _ ” > r$ í `  ¦ S X ‰ “   % i  . ƒ  ½ ¨   õ  { 9   F g ¼ # F g ~ ½ ӆ ¾ Ó\     PL_  [ jl   2 £ §`  ¦ 8 £ ¤& ñ 

%

i Ü ¼ 9, Õ ª [ jl   H  ” ¸‚  _   ê ø Íô  Ç ~ ½ ӆ ¾ ÓÜ ¼– Ð { 9     H

¼

# F g { 9  M : à ºf ” Ü ¼– Ð { 9  ½ + É M : ˜ Ð  €  • 30 ∼ 40% 7 £ x 

†

< Ê`  ¦ ˜ Ð% i  . s  Qô  Ç ‰ & ³ © œ“ É r F K5 Å q  ” ¸# 4 s  \ O   H P3MT



” ¸‚  \ " f• ¸ q 5 p w ô  Ç Ã ºï  r Ü ¼– Ð 8 £ ¤& ñ ÷ &# Q { 9   F g ¼ # F g \ 

@

/ô  Ç PL[ jl _  _ ” > r • ¸  H F K5 Å q  ” ¸# 4 _  Ä »Á ºü <  H  © œ › ' a

› '

a >  \ O   H  כ Ü ¼– Ð   z Œ ¤ .

(6)

P

c p 8 ý ò k >

‘

: r ƒ  ½ ¨  H “  …  ;@ /† < Ɠ § 2008¸  • ¸  ^ ‰ƒ  ½ ¨q  t " é ¶ \  _ 

# Œ à º' Ÿ ÷ &% 3 6 £ §

Y

c p w Š à U Ø ”  ô

[1] H. Shirakawa, E. J. Louis, A. G. MacDiarmid, C. K.

Chiang and A. J. Heeger, J. C. S. Chem. Comm., 578 (1977).

[2] D. H. Park, B. H. Kim, M. G. Jang, K. Y. Bae and J. Joo, App. Phys. Lett. 86, 113 (2005).

[3] D. H. Park, J. Joo, M. Y. Jeong, Y. B. Lee, H. S.

Kim, W. J. Choi, Q. H. Park, H. J. Kim, D. -C. Kim and J. Kim, Adv. Mater. 19, 2824 (2007).

[4] H. Wei, F. Hao, Y. Huang, W. Wang, P. Nordlander and H. Xu, Nano Lett. 8, 2497 (2008).

[5] H. -Y. Li, S. Ruhle, R. Khedoe, A. F. Koenderink and D. Vanmaekelbergh, Nano Lett. 9, 3515 (2009).

[6] D. H. Park, Y. B. Lee, M. Y. Cho, B. H. Kim, S.

H. Lee, Y. K. Hong, J. Joo, H. C. Cheong and S. R.

Lee, App. Phys. Lett. 90, 093122 (2007).

[7] S. H. Lee, D. H. Park, K. Kim, J. Joo, D.-C. Kim, H.-J. Kim and J. Kim, Appl. Phys. Lett. 91, 263102 (2007).

[8] H.-J. Kim, D.-C. Kim, R. Kim and J. Kim D. H.

Park, H. S. Kim and J. Joo, Sae Mulli 55, 97 (2007).

[9] S. H. Back, H. Song, D. -C. Kim and J. Kim, Sae Mulli 59, 44 (2009).

[10] Z. M. Li, Z. K. Tang, H. J. Liu, N. Wang, C. T.

Chan, R. Saito, S. Okada, G. D. Li, J. S. Chen, N. Nagasawa and S. Tsuda, Phys. Rev. Lett. 87, 127401 (2001).

[11] Y. Kim, N. Minami and S. Kazaoui, Appl. Phys.

Lett. 86, 073103 (2005).

수치

Fig. 1. Schematic of the confocal microscope to control the direction of input polarization.
Fig. 2. Laser confocal PL images of P3MT-Au nanowires with two direct directions of input polarization
Table 1. Measured PL values and the ratios of P3MT-Au nanowires with direct direction of input polarization.
Fig. 4. Dependence of relative PL intensities of P3MT- P3MT-Au nanowires and P3MT nanowires on the input  polar-ization direction

참조

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