• 검색 결과가 없습니다.

Dz D G K € ª œ@ /† < Ɠ § / B N õ @ /† < Æ 6 £ x6   x õ † < ÆÂ Ò,  Òí ß – 606-791 (2004¸ 8 Z 4 27{ 9 ~ à Î6 £ §)

N/A
N/A
Protected

Academic year: 2021

Share "Dz D G K € ª œ@ /† < Ɠ § / B N õ @ /† < Æ 6 £ x6   x õ † < ÆÂ Ò,  Òí ß – 606-791 (2004¸ 8 Z 4 27{ 9 ~ à Î6 £ §)"

Copied!
5
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

Si (111) M “ ˜ m; c" e W ë sù m Ç8 ý œ ÄT c l GaN • «8 ý V R ËX ê s ù p §  ü” X ¢ ZnO ! a( a • «8 ý  Œ ºX ì Ä — ¤V R Ë; c 6 ” X ¢ Ž ì ŏ Œ

T

® £* å  · ™ »ý — ¡Š û B · T + ä * × < · † ç ¡U ‡ Ú · ¼ ÿ ›0 ï F¬ £ · … è ¡ * > · T „ ‘ ž$ ß 

ô 

Dz D G K € ª œ@ /† < Ɠ § / B N õ @ /† < Æ 6 £ x6   x õ † < ÆÂ Ò,  Òí ß – 606-791 (2004¸   8 Z 4 27{ 9  ~ à Î6 £ §)

Si (111) l ó ø Í 0 A\  € ª œ| 9 _  GaN Ê ê} Œ •`  ¦ 7 £ x‚ Ã Ì l  0 Aô  Ç ZnO ! Q( 8 £ x_  ½ ¨› ¸& h  : £ ¤$ í › ¸| \  @ / # Œ

ƒ

 ½ ¨ % i  . Û ¼( ' a A ~ ½ ÓZ O Ü ¼– Ð ZnO ~ à Ì} Œ •`  ¦  © œ“ : r \ " f Si (111) l ó ø Í 0 A\  7 £ x‚ Ã Ì “ ¦ H

2

O ì  r0 Al \ 

"

f y Œ •y Œ • 700 ∼ 900

C_  “ : r • ¸– Ð \ P % ƒo ô  Ç Ê ê HVPE (hydride vapor phase epitaxy) ~ ½ ÓZ O Ü ¼– Ð GaN 8

£

x`  ¦ $ í  © œ % i  . ZnO ! Q( 8 £ x õ  GaN 8 £ x_  ½ ¨› ¸& h  : £ ¤$ í [ þ t`  ¦ AFM (atomic force microscope), XRD (X-ray diffraction), Õ ªo “ ¦ PL (photoluminescence)\  ¦ s 6   x # Œ › ' a¹ 1 Ï % i  . ‘ : r ƒ  ½ ¨   õ \ " f  H \ P 

%

ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í  © œ ) a GaN Ê ê} Œ •s  ZnO ! Q( 8 £ x_    & ñ $ í ˜ Ð   H  { 9  ½ ™× ¼ ß ¼l   ³ ð€  



} 9 l  1 p x \   8 ´ ú §“ É r % ò † ¾ Ó`  ¦ ~ à ΍  H  כ Ü ¼– Ð   z Œ ¤ .

PACS numbers: 81.14, 81.68

Keywords: GaN, ZnO, \ P % ƒo , AFM, PL

I. " e  ] Ø

þ

j  H  o½ + ËÓ ü t ì ø ͕ ¸^ ‰ ì  r  \ " f  © œ Å Ò3 l q ~ à ΍  H ' ‘ é ß – l  Õ

ü

t×  æ_   “   | 9  oÓ ü t >  ì ø ͕ ¸^ ‰\  › ' aô  Ç ƒ  ½ ¨  H ' õ AÒ  o µ 1 Ï F

g  s š ¸× ¼ü < ' õ AÒ  o Y Us $   s š ¸× ¼_  > hµ 1 Ï $ í / B N s Ê ê /

å

L5 Å qô  Ç ”  „  `  ¦ ˜ Ðs “ ¦ e ”   [1,2]. ‰ & ³F  GaN, ZnSe, SiC

>

: Ÿ x_  Ó ü t| 9 [ þ t s  ' õ AÒ  o µ 1 ÏF g ™ è \  s 6   x ÷ &“ ¦ e ” Ü ¼ 9, : £ ¤ y

 GaN  H 3.4 eV_  V , “ É r { ç ß –  `  ¦ t “ ¦ e ” “ ¦ 8 A# Qè ß – µ

1 ÏF g : £ ¤$ í , Ä ºÃ ºô  Ç \ P  „  • ¸• ¸,  o† < Æì ø Í6 £ x õ  ~ ½ Ó ‚   ” ¸Ø  ¦

\

 @ /ô  Ç | “ ¦$ í `  ¦ ° ú “ ¦ e ” l  M :ë  H \  F g ™ è  ÷  rë ß –  m 



 “ ¦5 Å q, “ ¦“ : r x 9 “ ¦Ø  ¦§ 4 `  ¦ € 9 כ ¹– Ð   H „   ™ è \  s  Ø

Ôl  t   € ª œ >  6 £ x6   x½ + É Ã º e ” # Q" f GaN\  ¦ l ì ø ÍÜ ¼– Ð

  H III-V7 á ¤ | 9  oÓ ü t ì ø ͕ ¸^ ‰\  › ' aô  Ç ƒ  ½ ¨ > 5 Å q à º' Ÿ ÷ &

“

¦ e ”  . ‰ & ³F  GaN_  $ í  © œ`  ¦ 0 AK  ŠҖ Ð   s # Q\  ¦ l  ó

ø ÍÜ ¼– Ð  6   x “ ¦ e ”   H X <,   s # Q  H GaN ü <_   H    



© œÃ º s ü < \ P Ø Ÿ ‚ ½ Ó > à º s  M :ë  H \    & ñ   † < Ê_  x 9 • ¸

 Z  } “ ¦ $ í  © œ Ê ê Í ‰ ty Œ • r \  ç  H\ P s  µ 1 ÏÒ q t # Œ € ª œ| 9 _  ~ Ã Ì }

Œ

•`  ¦ % 3 # Q? /l  # Q§ >  . s  Qô  Ç ë  H ] j& h `  ¦ K    l  0 AK  Si, GaAs, SiC, ZnO, MgAl

2

O

3

1 p x`  ¦ s 6   x # Œ € ª œ| 9 _  ~ Ã Ì }

Œ

•`  ¦ % 3 # Q? / 9  H ƒ  ½ ¨  Ö ¸µ 1 Ïy  à º' Ÿ ÷ &“ ¦ e ”   [3,4]. s 

×

 æ Si l ó ø Í“ É r GaN ü <_   H      © œÃ º s ü < \ P Ø Ÿ ‚ ½ Ó >  Ã

º s  M :ë  H \    & ñ $ í s  Ä ºÃ ºô  Ç | 9  oÓ ü t ì ø ͕ ¸^ ‰ $ í  © œs 

E-mail: [email protected];

Tel: +82-51-410-4378; Fax: +82-51-410-4784

#

Q§ > t ë ß – @ /€  & h  o 0 p x “ ¦   s   â ] j& h s  9, a % ~

“ É

r \ P  x 9 „  l  „  • ¸• ¸\  ¦ t “ ¦ e ” # Q" f [5, 6] Si l ó ø Íõ  GaN  s _       © œÃ º  \ P Ø Ÿ ‚ ½ Ó > à º_  s \  ¦ ×  ¦ # Œ×  ¦ Ã

º e ”   H & h ] X ô  Ç ! Q( 8 £ x`  ¦ ‚  × þ ˜ô  Ç €   € ª œ| 9 _  GaN ~ à Ì} Œ •

`

 ¦ $ í  © œ½ + É Ã º e ”  . Õ ª ×  æ ZnO  H GaN ü < q 5 p wô  Ç Ó ü t o & h  :

£

¤$ í `  ¦ t “ ¦ e ” Ü ¼ 9, ZnO ~ à Ì} Œ •õ  Si l ó ø Í`  ¦  o† < Æ& h Ü ¼

–

Ð ] j ½ + É Ã º e ” # Q freestanding GaN J ?s ( \  ¦ ~ 1 >  % 3 

`

 ¦ à º e ”    H  © œ& h `  ¦ t “ ¦ e ”  . Ä ºo   H s „   ƒ  ½ ¨\ 

"

f [7] ZnO ~ à Ì} Œ •_  \ P % ƒo  ´ òõ \  @ /ô  Ç ½ ¨› ¸& h , F g† < Æ& h  :

£

¤$ í \  @ /K  ƒ  ½ ¨ % i “ ¦ Õ ª   õ \  ¦  „ ½ ÓÜ ¼– Ð ‘ : r ƒ  ½ ¨\ 

"

f  H Si (111) l ó ø Í 0 A\  \ P % ƒo ô  Ç ZnO } Œ •`  ¦ ! Q( 8 £ x Ü ¼

–

Ð  6   x # Œ HVPE (hydride vapor phase epitaxy) ~ ½ ÓZ O 

`

 ¦ s 6   x # Œ Ê ê} Œ • GaN   & ñ `  ¦ $ í  © œ % i  . $ í  © œ ) a GaN _  ½ ¨› ¸& h , F g† < Æ& h  : £ ¤$ í `  ¦ › ' a¹ 1 Ï # Œ ! Q( 8 £ x Ü ¼– Ð+ ‹  6   x

 )

a ZnO ~ à Ì} Œ •[ þ t_  GaN Ê ê} Œ • $ í  © œ\  p u   H % ò † ¾ Ó`  ¦ › ¸ 

% i “ ¦ € ª œ| 9 _  GaN Ê ê} Œ • $ í  © œ`  ¦ 0 Aô  Ç ZnO ! Q( 8 £ x_  : £ ¤

$ í

\  @ /K   7 H_  % i  .

II. ÷ m Ç] M ö U ê s0 n É

‘

: r z  ´+ « >\ " f  H Si (111) l ó ø Í 0 A\  RF-Û ¼( '   © œu \  ¦ s

6   x # Œ ZnO ~ à Ì} Œ •`  ¦ 7 £ x‚ Ã Ì % i  .  ¿ Ü ¼– Ѝ  H ZnO 



6   x ÷ &% 3 Ü ¼ 9 Û ¼( ' a A Û ¼– Ѝ  H Ar s   6   x ÷ &% 3 “ ¦ 7 £ x

‚ Ã

Ì „   Õ þ ›! Q ? /\   H €  • 10

−6

Torr  t  ”  / B N`  ¦ Ä »t  % i 

-355-

(2)

Fig. 1. AFM surface images of ZnO films with different annealing temperatures (a) as-dep.ZnO (b) 700

C (c) 800

C and (d) 900

C annealing.



. 7 £ x‚ à ̓ É r  © œ“ : r \ " f s À Ò# Q& ’ Ü ¼ 9 RF 0 >  H 200 W, Ar Û ¼_  Ä »| ¾ ӓ É r 50 sccm, Õ ªo “ ¦ Õ þ ›! Q ? /_  · ú š§ 4 “ É r 5 mTorr – Ð Ä »t  # Œ 100 nm ¿ ºa _  ZnO ~ à Ì} Œ •`  ¦ 7 £ x‚ Ã Ì 

%

i  . 7 £ x‚ à Ìs  = å Qè ß – Ê ê\   H  – Ð \ P í ß – o– Ð (thermal oxi- dation furnace) \ " f H

2

O ì  r0 Al – Ð €  • 2r ç ß – 1 l xî ß – 700 ∼ 900

C_  “ : r • ¸– Ð \ P % ƒo  % i  . 7 £ x‚ à Ìõ  \ P % ƒo  = å Qè ß – ZnO ~ à Ì} Œ • 0 A\  HVPE ~ ½ ÓZ O `  ¦ s 6   x # Œ GaN ~ à Ì} Œ •`  ¦ $ í



© œ % i  . HVPE ~ ½ ÓZ O “ É r GaCl

3

ü < NH

3

\  ¦ q “ §& h  “ ¦“ : r

\

" f \ P ì  r K  # Œ ì ø Í6 £ x r &  GaN\  ¦ ½ + Ë$ í Ù ¼– Ð   & ñ $ í



© œ 5 Å q • ¸  Ø Ô“ ¦   & ñ $ í s  a % ~“ É r GaN\  ¦ % 3 `  ¦ à º e ”    H



© œ& h s  e ”   [8]. ¿ º î  r GaN ~ à Ì} Œ •`  ¦ $ í  © œ l  „  \  s  p

 7 £ x‚ à Ìr †   ZnO ~ à Ì} Œ • 0 A\  €  • 560

C_  “ : r • ¸\ " f €  • 25 nm ¿ ºa _  $ “ : r GaN 8 £ x`  ¦ $ í  © œ # Œ ! Q( 8 £ x Ü ¼– Ð   6

 

x % i  . ! Q( 8 £ x_  $ í  © œs  = å Q  €   “ : r • ¸\  ¦ 1050

C  t 



© œ5 p x r &  1r ç ß –1 l xî ß – 50 µm ¿ ºa _  Ê ê} Œ • GaN 8 £ x`  ¦ $ í



© œ % i “ ¦ $ í  © œ Ê ê ½ ¨› ¸& h  : £ ¤$ í `  ¦ · ú ˜ ˜ Ðl  0 A # Œ AFM (atomic force microscope)  © œq – Ð ³ ð€    © œI \  ¦ · ú ˜ ˜ Ѐ Œ ¤

“

¦, XRD (X-ray diffraction)_  θ-2θ ~ ½ Ód ” Ü ¼– Ð 30 ∼ 65



t  8 £ ¤& ñ # Œ   & ñ $ í `  ¦ · ú ˜ ˜ Ѐ Œ ¤ . ¢ ¸ô  Ç He-Cd Y Us 

$

\  ¦  6   xô  Ç PL (photoluminescence)  © œq – Ð F g† < Æ& h  : £ ¤

$ í

`  ¦ · ú ˜ ˜ Ѐ Œ ¤ .

III. + s ÇÊ Ý õ m Í w в  o

Table 1“ É r s „   ƒ  ½ ¨\ " f [7] % 3 “ É r Si (111) l ó ø Í 0 A\ 



© œ“ : r \ " f 7 £ x‚ à Ìô  Ç ZnO ~ à Ì} Œ •_  \ P % ƒo  ´ òõ \  @ /ô  Ç : £ ¤$ í

`

 ¦   ? /  H  כ Ü ¼– Ð y Œ •y Œ •_  “ : r • ¸\ " f \ P % ƒo ô  Ç ZnO ~ à Ì

Fig. 2. Optical images of GaN surface grown on annealed ZnO buffer layer at different temperatures (a) as-dep.

ZnO (b) 700

C (c) 800

C and (d) 900

C annealing.

}

Œ

•“ É r \ P % ƒo  “ : r • ¸ Z  }  | 9 à º2 Ÿ ¤   & ñ $ í s  a % ~  t “ ¦ “ ¦

“

: r \ " f_  \ P % ƒo – Ð “  K  ³ ð€   7 £ xµ 1 Ï ‰ & ³ © œs  µ 1 ÏÒ q t % i  .

Fig. 1“ É r 7 £ x‚ à ̝ ) a ZnO ~ à Ì} Œ •[ þ t_  \ P % ƒo  › ¸| \  @ /ô  Ç ³ ð€  

‰ &

³ © œ`  ¦ AFM Ü ¼– Ð › ' a¹ 1 Ïô  Ç  ”  Ü ¼– Ð \ P % ƒo  “ : r • ¸ 7 £ x 

½ +

Éà º2 Ÿ ¤ ³ ð€    } 9 l   Œ • t “ ¦  { 9  ½ ™× ¼ ß ¼l  & t  t

ë ß – 900

C_  “ : r • ¸\ " f \ P % ƒo ô  Ç ZnO ~ à Ì} Œ •“ É r ³ ð€     } 9

l    t “ ¦  { 9  ½ ™× ¼ ß ¼l • ¸ ×  ¦ # Q× ¼  H  כ `  ¦ · ú ˜ à º e ”

 . s   H Wang [9] 1 p x s  ˜ Г ¦ô  Ç  כ ° ú  s  “ ¦“ : r_  \ P % ƒo 

\

" f í ß –™ è / B N/ B N[ þ t s   | ¾ ÓÜ ¼– Ð + þ A$ í ÷ &“ ¦ í ß –™ è\  q K  ± ú 

“ É

r 7 £ x l · ú š`  ¦ ”   Zn 7 £ xµ 1 Ï # Œ { 9 # Q   H ³ ð€   7 £ xµ 1 Ï ‰ & ³



© œÜ ¼– Ð ˜ Г   .

Fig. 2  H y Œ •y Œ •_  “ : r • ¸– Ð \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í



© œr †   Ê ê} Œ • GaN 8 £ x_  ³ ð€  `  ¦ 500 C – Ð › ' a¹ 1 Ïô  Ç F g† < Ɖ & ³ p

 â  ”  s  . \ P % ƒo  t  · ú §“ É r ZnO ! Q( 8 £ x 0 A\  $ í  © œ

 )

a GaN 8 £ x_  ³ ð€  “ É r ¨ î ò ø ̀  (P)s   _  › ' a¹ 1 Ï÷ &t  · ú §€ Œ ¤“ ¦

"

f– Ðç ß –\  é ß –  ´ ú §s  ” > r F    H €  (A)[ þ t – Ð s À Ò# Q4 R e ” 

%

3  . 700

C \ " f  H ¨ î ò ø ̀  s  „  ^ ‰_  30 % & ñ • ¸\  ¦ ˜ Ð# Œ Å

ғ ¦ e ” % 3 Ü ¼ 9 800

C \ " f \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\ 

$ í

 © œ ) a GaN 8 £ x_  ³ ð€  “ É r „  ^ ‰ €  & h _  50 % s  © œ ¨ î ò ø Í

€ 

s  › ' a¹ 1 Ï÷ &# Q é ß –  & ñ s  ¸ ú ˜ $ í  © œ ) a  כ `  ¦ · ú ˜ à º e ”  . 900

C \ " f• ¸ ¨ î ò ø ̀  s  50 %& ñ • ¸ › ' a¹ 1 Ï÷ &% 3 Ü ¼  ¨ î ò ø ̀     s

\  Si l ó ø Ís  \ g As   ) a  כ Ü ¼– Ð ˜ Ðs   H  Òì  r(E) s  V , 

>

 › ' a¹ 1 Ï÷ &% 3  . s   H “ ¦“ : r \ " f_  \ P % ƒo – Ð “  K  ³ ð€   7 £ x µ

1 Ïs  { 9 # Q >  ÷ &# Q  { 9  ½ ™× ¼_  ß ¼l  ×  ¦ # Q[ þ t “ ¦ ~ à Ì} Œ • _  ¿ ºa  y Œ ™™ è >  ÷ &# Q ! Q( 8 £ x Ü ¼– Ð  6   xô  Ç ZnO ~ à Ì} Œ • s

 Cll \  _ ô  Ç l ó ø Í_  \ g A`  ¦ } Œ • Å Òt  3 l wô  Ç  כ Ü ¼– Ð ó ø Í é

ß – ) a  .

Fig. 3“ É r 800

C ü < 900

C_  “ : r • ¸– Ð \ P % ƒo ô  Ç ZnO ! Q (

8 £ x 0 A\  $ í  © œ ) a Ê ê} Œ • GaN 8 £ x_  ¨ î ò ø Í t % i  ? /\ " f % 3 

“

É r AFM ³ ð€   + þ A © œs “ ¦ Table 2  H Fig. 3_    õ – РÒ' 

%

3 “ É r ³ ð€    } 9 l s  . ¿ º r « Ñ — ¸¿ º ¨ î ò ø ̀  _  ³ ð€    

(3)

Table 1. Properties of ZnO films with different annealing temperatures.

AFM XRD PL

Mean Diameter Relative intensity FWHM Main peak FWHM I

(main peak)

: / rms [nm] (I

(002)

/I

(002)as−dep

) [deg.] [nm] [nm] I

(deep level)

As-dep. ZnO 110/5.1 1 1.44 391 34.5 1:0.5

700

C 140/4.3 2.25 0.21 383 27 1:0.58

annealing 800

C 154/4.8 4 0.25 380 21.7 1:0.08

900

C 140/6.0 4.4 0.1 381.5 12 *

Fig. 3. AFM surface images of GaN grown on ZnO buffer layer which is annealed at (a) 800

C and (b) 900

C.

Table 2. Surface roughness of GaN grown on ZnO buffer layer which is annealed at 800 and 900

C.

800

C 900

C

rms [nm] 0.145 0.298

} 9

l   Å Ò a % ~“ É r   õ \  ¦ t “ ¦ e ” % 3 Ü ¼  800

C – Ð \ P 

%

ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í  © œ ) a GaN_  ³ ð€    } 9 l   H 0.14 nm“   ì ø ̀   900

C – Ð \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í



© œ ) a GaN 8 £ x_  ³ ð€    } 9 l   H 0.29 nm – Ð ¿ ºC  s  © œ_ 

s \  ¦ ”   . ½ ¨› ¸& h “   : £ ¤$ í s   © œ a % ~€ Œ ¤~   800

C \ 

"

f \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í  © œ ) a GaN 8 £ x“ É r ˜ Ð  V , 

“ É

r ¨ î ò ø ̀  `  ¦ t “ ¦ e ” “ ¦ l ó ø Ís  \ g A ) a t % i • ¸ & h “ ¦ ³ ð

€ 

  } 9 l • ¸  Å Ò  Œ •“ É r  כ Ü ¼– Ð ˜ Ð  \ P % ƒo ô  Ç ZnO ~ à Ì} Œ • _   { 9  ½ ™× ¼ ß ¼l , ³ ð€    } 9 l , Õ ªo “ ¦ ~ à Ì} Œ •_  ¿ ºa  1 p x s

 GaN $ í  © œ\   H % ò † ¾ Ó`  ¦ p u   H  כ Ü ¼– Ð ó ø Íé ß – ) a  .

Fig. 4  H 800

C ü < 900

C “ : r • ¸– Ð \ P % ƒo ô  Ç ZnO ! Q(  8

£

x 0 A\  $ í  © œ ) a Ê ê} Œ • GaN 8 £ x_  XRD J ‡  s  . ZnO ! Q (

8 £ x 0 A\  $ í  © œ ) a GaN 8 £ x_  XRD J ‡  \ " f 2θ  H 30

Â Ò '

 65

 t  1 l x{ 9  >  34.6

_   _  x ß ¼      H X <

s

 כ “ É r ¹ ¢ ¤~ ½ Ó& ñ (hexagonal) GaN   & ñ ½ ¨› ¸_  (002) €  \  _

ô  Ç x ß ¼ü < { 9 u    H  כ s  . GaN (002) x ß ¼_  ì ø Íu 

;

Ÿ

¤ õ  y © œ• ¸\  ¦ q “ §K ˜ Ѐ   800

C_  x ß ¼ y © œ• ¸ 900

C _  x ß ¼ y © œ• ¸˜ Ð  ¿ ºC  & ñ • ¸  8 ß ¼“ ¦ ì ø Íu ; Ÿ ¤“ É r 800

C  0.12

, 900

C  0.13

– Ð 0.01

& ñ • ¸  8  Œ •  800

C \ " f

\ P

% ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í  © œ ) a GaN 8 £ x s    & ñ $ í % i  r

  8 a % ~    H  כ `  ¦ · ú ˜ à º e ” % 3  .

Fig. 4. XRD spectra of GaN grown on ZnO buffer layer which is annealed at 800 and 900

C.

Fig. 5. PL spectra of GaN grown on ZnO buffer layer with different annealing temperatures.

Fig. 5“ É r y Œ • “ : r • ¸ › ¸| \ " f \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\ 

$ í

 © œ ) a Ê ê} Œ • GaN 8 £ x_  PL Û ¼& 7 ˜à Ô! 3 s “ ¦ s – РÒ'  % 3 “ É r x

ß ¼_   © œ_     oü < þ j@ / ì ø Íu ; Ÿ ¤ s  Fig. 6\ " f ˜ Ð# Œ Å

ғ ¦ e ”  . 800

C – Ð \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í  © œ ) a GaN_  ì ø Íu ; Ÿ ¤ s  20.7 nms “ ¦ 900

C – Ð \ P % ƒo ô  Ç ZnO

!

Q( 8 £ x 0 A\  $ í  © œ ) a GaN_  ì ø Íu ; Ÿ ¤ s  26.3 nm“    כ `  ¦ q 

“

§ # Œ ^  ¦ M : 800

C – Ð \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\  $ í  © œ

(4)

Fig. 6. PL peak position and FWHM variation of GaN grown on ZnO buffer layer with different annealing tem- peratures.

 )

a GaN 8 £ x s   © œ  Œ •“ É r ì ø Íu ; Ÿ ¤`  ¦ t  9 · ú ¡_    õ [ þ t õ 



ð ø Ít – Ð  © œ a % ~“ É r ~ à Ì} Œ • : £ ¤$ í `  ¦ ”   .

s

„   ƒ  ½ ¨ [7]\ " f ZnO ~ à Ì} Œ •s  800

C \ " f \ P % ƒo  

%

i `  ¦ M :  { 9  ½ ™× ¼ ß ¼l   © œ ß ¼“ ¦  } 9 l • ¸  Œ • " f ½ ¨

›

¸& h  : £ ¤$ í s   © œ a % ~ “ ¦ 900

C \ " f \ P % ƒo  % i `  ¦ M : PL _

 ì ø Íu ; Ÿ ¤ s  / å L  y  y Œ ™™ è   H  כ Ü ¼– Ð ˜ Ð  ? / Ò  † < Ês 

×

 ¦ # Q[ þ t “ ¦   & ñ $ í s  † ¾ Ó © œ÷ &  H  כ Ü ¼– Ð   z Œ ¤ . Õ ª Q 

!

Q( 8 £ x Ü ¼– Ð" f_  % i ½ + É`  ¦ ˜ Ѐ Œ ¤`  ¦ M : 800

C \ " f \ P % ƒo ô  Ç ZnO ~ à Ì} Œ •\ " f  H  { 9  ½ ™× ¼ ß ¼“ ¦ ³ ð€    © œI • ¸ a % ~  " f

#

Œ Q “ : r • ¸– Ð \ P % ƒo ô  Ç ZnO ! Q( 8 £ x[ þ t ˜ Ð  V , “ É r GaN ¨ î ò

ø ̀  `  ¦ % 3 `  ¦ à º e ” % 3 “ ¦ Si l ó ø Ís  Cll \  _ K  \ g A÷ &  H

 כ

`  ¦ } Œ • Å Ò# Q € ª œ| 9 _  Ê ê} Œ • GaN 8 £ x`  ¦ % 3 `  ¦ à º e ” % 3  .

t ë ß – 900

C \ " f \ P % ƒo ô  Ç  â Ä º\   H “ ¦“ : r \ " f_  \ P % ƒ o

– Ð “  K  ³ ð€  + þ A © œs   å ԓ ¦  { 9  ½ ™× ¼_  ß ¼l   Œ •l  M

:ë  H \  € ª œ| 9 _  GaN8 £ x`  ¦ % 3 `  ¦ à º \ O % 3  . s  כ Ü ¼– Ð ˜ Ð 

€

ª œ| 9 _  Ê ê} Œ • GaN 8 £ x_  $ í  © œ\ " f  H ZnO ! Q( 8 £ x_  ? / Ò

 

† < Êx 9 • ¸    & ñ $ í ˜ Ð   H  { 9  ½ ™× ¼_  ß ¼l   ³ ð€    } 9  l

 1 p x s   8 ´ ú §“ É r % ò † ¾ Ó`  ¦ Šҍ  H  כ Ü ¼– Ð ó ø Íé ß –÷ &# Q ”   .

IV. + s Ç Â ] Ø

Si (111) l ó ø Í 0 A\  7 £ x‚ Ã Ì Ê ê \ P % ƒo ô  Ç ZnO } Œ •`  ¦ Ê ê} Œ • GaN 8 £ x_  $ í  © œ`  ¦ 0 Aô  Ç ! Q( 8 £ x Ü ¼– Ð  6   x # Œ ZnO ! Q(  8

£

x s  GaN $ í  © œ\  p u   H % ò † ¾ Ó\  @ / # Œ ½ ¨› ¸& h , F g† < Æ& h  :

£

¤$ í `  ¦ ƒ  ½ ¨ % i  . Û ¼( ' a A ~ ½ ÓZ O `  ¦ s 6   x # Œ ZnO } Œ •

`

 ¦ 100 nm_  ¿ ºa – Ð 7 £ x‚ Ã Ì “ ¦ \ P í ß – o– Ð\ " f H

2

O ì  r0 A l

– Ð 700 ∼ 900

C_  “ : r • ¸– Ð 2r ç ß – 1 l xî ß – \ P % ƒo  % i “ ¦ Õ

ª 0 A\  HVPE ~ ½ ÓZ O `  ¦ s 6   x # Œ 1050

C \ " f 1r ç ß – 1 l x î

ß – Ê ê} Œ • GaN 8 £ x_  $ í  © œ % i  . ZnO ~ à Ì} Œ •“ É r 800

C \ " f

\ P

% ƒo Ù þ ¡`  ¦ M : ½ ¨› ¸& h  : £ ¤$ í s   © œ a % ~ “ ¦ 900

C \ " f \ P 

%

ƒo  % i `  ¦ M :   & ñ $ í s   © œ a % ~€ Œ ¤Ü ¼  ! Q( 8 £ x Ü ¼– Ð   6

 

x % i `  ¦ M : 800

C \ " f \ P % ƒo ô  Ç ZnO ! Q( 8 £ x 0 A\ " f

 © œ V , “ É r ¨ î ò ø ̀  õ   © œ a % ~“ É r   & ñ $ í `  ¦ t   H GaN 8 £ x s

 $ í  © œ÷ &  H  כ `  ¦ › ' a¹ 1 Ͻ + É Ã º e ” % 3  . € ª œ| 9 _  Ê ê} Œ • GaN 8

£

x_  $ í  © œ`  ¦ 0 AK " f  H ZnO ! Q( 8 £ x_    & ñ $ í ˜ Ð   H   { 9

 ½ ™× ¼_  ß ¼l   ³ ð€    } 9 l  1 p x s   8 ´ ú §“ É r % ò † ¾ Ó`  ¦ ï  r



.

Y c

p w Š à U Ø ”  ô

[1] S. Nakamura, M. Senoh, S. Nagahama, N. Iwasa, T.

Yamada, T. Matsushita, H. Kiyoku, Y. Sugimoto, T.

Kozaki, H. Umemoto, M. Sano and K. Chocho, Jpn.

J. Appl. Phys. 36, L1586 (1997).

[2] S. Nakamura, M. Senoh, N. Iwasa, S. Nagahama, T. Yamada, T. Matsushita, H.Kiyoku, Y. Sugimoto, T.Kozaki, H. Umemoto, M. Sano and K. Chocho, Appl. Phys. Lett. 72, 211 (1998).

[3] S. Strite and K. Morkoc, J. Vac. Sci, Technol. B 10, 1237 (1992)

[4] Y. H. Song, J. H. Kim, H. J. Jang, S. R. Joon, J. W.

Yang, K. Y. Lim and G. M. Yang, J. Korean Phys.

Soc. 38, 242 (2001).

[5] J. W. Yang, A. Lunev, G. Smin, A. Chitnis, M. Shat- alov, M. A. Khan, J. E. Von Nostr and R. Gaska, Appl. Phys. Lett. 76, 273 (2000).

[6] H. Zhang, Z. Ye and B. Zhao, Solid State Electronics 46, 301 (2002).

[7] J. Y. Lee, H. S. Kim, J. Y. Yi, J. H. Chang, H. S.

Ahn, M. Yang and S. N. Yi, Sae Mulli, 48, 5 (2004) [8] S. T. Kim, Y. J. Lee, D. C. Moon, Chul Lee and H.

Y. Park, J. Electronic Materials 27, 1112 (1998) [9] Y. G. Wang, S. P. Lau, X. H. Zhang, H. H. Hug, H.

W. Lee, S. F. Yu and B. K. Tay, J. Cryst. Growth

259, 335 (2003).

(5)

A Study on the Structural Properties of ZnO Buffer Layers for Growth of High-Quality GaN Thick Layer on Si (111) Substrates

J. Y. Lee, H. S. Kim,

J. Y. Yi, J. H. Chang, H. S. Ahn, M. Yang and S. N. Yi Department of Applied Sciences, Korea Maritime University, Busan 606-791

(Received 27 August 2004)

Zinc-oxide(ZnO) films were deposited on Si (111) substrates by radio-frequency (rf) sputtering at room temperature and were annealed in a H

2

O ambient at temperatures between 700 and 900

C for 2 hrs; then, GaN thick layers were grown on the ZnO buffer layers by using hydride vapor phase epitaxy (HVPE). The structural and the optical properties of the ZnO buffer layers and the GaN thick layers were investigated by atomic force microscop (AFM), X-ray diffraction (XRD) and photoluminescence (PL). According to our experiments, the GaN thick layer grown on a thermally annealed ZnO buffer layer was influenced by the island size in and the surface roughness of the ZnO buffer layer rather than by its crystallinity.

PACS numbers: 81.14, 81.68

Keywords: GaN, ZnO, Annealing, AFM, PL

E-mail: [email protected]

수치

Fig. 1. AFM surface images of ZnO films with different annealing temperatures (a) as-dep.ZnO (b) 700 ◦ C (c) 800 ◦ C and (d) 900 ◦ C annealing.
Table 2. Surface roughness of GaN grown on ZnO buffer layer which is annealed at 800 and 900 ◦ C.
Fig. 6. PL peak position and FWHM variation of GaN grown on ZnO buffer layer with different annealing  tem-peratures

참조

관련 문서

→ Turbulent boundary layer is established near the leading edge of the boundary without a preceding stretch of laminar flow... • Interior of the turbulent

Average tensile stress of 1.3μm thick GaN layer grown on 12nm thick AlN buffer.. - Relaxed AlN buffer at

Although a large compressive residual stress was generated in the surface layer due to the peening process, shot peening showed –23 MPa, unlike laser... shock peening

Figure 8 Diffuse reflectance FT-IR spectra of (A) fresh DBR PSi, (B) thermally oxidized DBR PSi, (C) the wafer after functionalization of the DBR PSi

A series of experiments was conducted from March 16 to July 12 in 2004 in Jeju Island to investigate the effects of sowing date, sowing rate, sand

In addition, attention was paid to the high damping characteristics of the constrained layer laminated structure to which the viscoelastic tape was applied in

They suggested that vaporization of a thin layer of liquid between the growing bubble and the heating surface caused removal of heat from the surface, thus lowing

(a) dextran chip surface (b) HBsAg antibody chip surface Fig. 4-17 Uniformity of dextran and antibody layer by AFM.. HBsAg의 NRC에서는 바이오 박막 두께가 증가함에 따라 