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 ƒ  ½ ¨ 7 Hë  H  Sae Mulli (The Korean Physical Society), Volume 57, Number 4, 2008¸   10 Z 4, pp. 287∼290

Si (111) M “ ˜ m ü; c V R ËX ê s” X ¢ GaN • «8 ý $ [Æ X Ø AlN ú n އ ˜ m • « ‘ ¤B s; c   \ ¥ — ¤V R Ë

™ »%  ¦ 

' õ

AÅ Ò@ /† < Ɠ § „   & ñ ˜ Ð/ B N † < ÆÂ Ò, ' õ AÅ Ò 360-746 (2008¸   7 Z 4 31{ 9  ~ à Î6 £ §)

Ä

»l  o† < Æl  © œ7 £ x ‚ à ÌZ O Ü ¼– Ð $ “ : r AlN ×  æ ç ß –8 £ x`  ¦ s 6   x # Œ Si (111) l ó ø Í0 A\  GaN ~ à Ì} Œ •`  ¦ $ í  © œ “ ¦

$

“ : r AlN ×  æ ç ß –8 £ x ¿ ºa \    É r : £ ¤$ í `  ¦ ƒ  ½ ¨ % i  . $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \     GaN 8 £ x _  ç  H\ P s 



 y Œ ™ >    † < Ê`  ¦ · ú ˜ à º e ” % 3 “ ¦ 10 nm ¿ ºa \ " f ç  H\ P x 9 • ¸ 5/cm _   © œ & h “ É r ç  H\ P `  ¦ % 3 % 3  . ¢ ¸ô  Ç, (002) X-ray rocking curve _  full width at half maximum 8 £ ¤& ñ   õ  651 arcsec _    & ñ $ í `  ¦ ° ú   H ~ Ã Ì }

Œ

•`  ¦ % 3 % 3 “ ¦ photoluminescence 8 £ ¤& ñ   õ  300 K \ " f 38.1 meV _  full width at half maximum `  ¦

% 3

% 3  .

PACS numbers: 68.55.-a, 62.20Mk, 81.40.Jj

Keywords: $ “ : r AlN ×  æ ç ß –8 £ x, ç  H\ P , z  ´o – B H (111), Ä »l  o† < Æl  © œ7 £ x ‚ à Ì

I. " e  ] Ø

þ

j   H \ , Si l ó ø Í“ É r $    o, @ /6   x | ¾ Ó o, Õ ªo “ ¦ a % ~“ É r \ P  x 9

„  l & h  „  • ¸$ í 1 p x _   © œ& h  M :ë  H \  GaN_  $ í  © œ l ó ø ÍÜ ¼

–

Ð ´ ú §“ É r › ' a d ” `  ¦ ~ à Î 𠏓 ¦ e ”  . t ë ß –, GaNü < Si l ó ø Í



s _   H     © œÃ º Ô  ¦{ 9 u ü < \ P Ø Ÿ ‚ ½ Ó > à º_  s – Ð “   K

 µ 1 ÏÒ q t   H GaN ç  H\ P  (crack) s  Si l ó ø Í`  ¦ s 6   x ô  Ç GaN _

 $ í  © œ\    a Ë >[  t ÷ &“ ¦ e ”  . ´ ú §“ É r ƒ  ½ ¨ [ þ t“ É r Si l ó ø Í\ 

"

f # Œ Q t  ! Q( 8 £ x (buffer layer)`  ¦  6   x # Œ “ ¦¾ ¡ §| 9 , Á

ºç  H\ P  GaN \  ¦ % 3 l  0 AK  ” ¸§ 4  % i Ü ¼ , 1 µms  © œ_  Á º ç

 H\ P  (crack-free) GaN $ í  © œ l  ' p é ß –{ 9  ! Q( 8 £ x ë ß –Ü ¼– Ѝ  H ô

 Ç>  e ” % 3  . s ü < ° ú  “ É r s Ä »– Ð ×  æ ç ß –8 £ x (interlayer) `  ¦

¶ ú

š{ 9    H ~ ½ ÓZ O s  • ¸{ 9 ÷ &% 3 “ ¦ ×  æ ç ß –8 £ x Ü ¼– Ð $ “ : r AlN [1], SiNx [2], Õ ªo “ ¦  ×  æ8 £ x (multilayer) [3] 1 p x`  ¦ s 6   x   H

ƒ

 ½ ¨ ”  ' Ÿ ÷ &“ ¦ e ”  . Õ ª ×  æ \ " f• ¸ $ “ : r AlN ×  æ ç ß –8 £ x`  ¦ s

6   x ô  Ç $ í  © œZ O “ É r ç ß –é ß – €  " f   & ñ   † < Ê (defect) õ  ç  H\ P 

`

 ¦ 1 l x r \  ×  ¦{ 9  à º e ”   H $ í  © œZ O Ü ¼– Ð · ú ˜ 94 R e ”  . Õ ª Q



, a % ~“ É r : £ ¤$ í `  ¦ ° ú   H $ í  © œZ O e ” \ • ¸ Ô  ¦ ½ ¨ “ ¦ $ “ : r AlN

×

 æ ç ß –8 £ x $ í  © œZ O \  @ /ô  Ç ƒ  ½ ¨  H  f ”  p q   .

‘

: r z  ´+ « >\ " f  H Ä »l  o† < Æl  © œ7 £ x ‚ à ÌZ O  (MOCVD) Z O Ü ¼

–

Ð $ “ : r AlN ×  æ ç ß –8 £ x`  ¦ s 6   x # Œ Si (111) l ó ø Í0 A\  GaN

~ Ã

Ì} Œ •`  ¦ $ í  © œ “ ¦ $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \    É r ç  H\ P x 9 

•

¸ x 9 ½ ¨› ¸& h , F g † < Æ& h  : £ ¤$ í `  ¦ › ' a ¹ 1 Ï % i  .

E-mail: [email protected]

II. ÷ m Ç] M öU ê s0 n É

—

¸Ž  H GaN ü < AlN 8 £ x“ É r MOCVD (Veeco  , D180GaN)



© œq \  ¦ s 6   x # Œ $ í  © œ ÷ &% 3  . GaN $ í  © œ`  ¦ 0 AK  (111)

~ ½

ӆ ¾ Ó Si (n+ þ A, 0.001 Ω·cm) l ó ø Í`  ¦ s 6   x % i  . í ß – oÓ ü t s 

\ O

  H ³ ð€  `  ¦ 0 AK  à º™ è7 á x é ß – Si ³ ð€   % ƒo \  ¦ % i   [4].

GaN ü < $ “ : r AlN 8 £ x“ É r TMGa, TMAl ü < NH

3

\  ¦ ™ èÛ ¼  Û

¼– Ð H

2

\  ¦ H o # Q Û ¼– Ð  6   x # Œ 1045

C, 200 Torr ü

< 720

C, 76 Torr \ " f y Œ •y Œ • $ í  © œ % i  . AlN ! Q(  8

£

x $ í  © œ\  @ /ô  Ç / B N& ñ › ¸| “ É r   É r ë  H‰  ³\   [ jy  [ O " î ÷ &

#

Qe ”   [5]. 35 nm AlN ! Q( 8 £ x`  ¦ s 6   x # Œ 200 nm 1  GaN 8 £ x`  ¦ $ í  © œ “ ¦ Õ ª 0 A\  $ “ : r AlN ×  æ ç ß –8 £ x`  ¦ $ í  © œô  Ç Ê

ê 1.5 µm 2  GaN 8 £ x`  ¦ $ í  © œ % i  . $ “ : r AlN ×  æ ç ß –8 £ x

¿

ºa \  ¦ 5 nm, 10 nm, Õ ªo “ ¦ 20 nm – Ð    o # Œ $ í  © œ 

%

i  . $ “ : r AlN ×  æ ç ß –8 £ x`  ¦ s 6   x # Œ $ í  © œ  ) a 8 £ x _  þ j7 á x ½ ¨

›

¸ Fig. 1 \     e ”  .

$

“ : r AlN ×  æ ç ß –8 £ x ¿ ºa \    É r 2  GaN _  ç  H\ P x 9 • ¸  H normalski ‰ & ³p  â (x50) `  ¦ s 6   x # Œ › ' a ¹ 1 Ï % i  . $ í  © œ  ) a 8

£

x _    & ñ $ í `  ¦ › ' a ¹ 1 Ï l 0 AK  X-ray diffraction (XRD) ü <

X-ray rocking curve (XRC) 8 £ ¤& ñ `  ¦ % i “ ¦ F g † < Æ& h “   : £ ¤

$ í

`  ¦ › ' a ¹ 1 Ï l 0 AK  photoluminescence (PL) 8 £ ¤& ñ `  ¦ 

% i  .

III. + s ÇÊ Ý õ m Í À X Ø8 ý

Fig. 2   H $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \     $ í  © œô  Ç 2 

GaN 8 £ x \  @ /ô  Ç θ − 2θ Û ¼ ± pô  Ç XRD   õ s  . — ¸Ž  H GaN

-287-

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-288- ô  Dz D GÓ ü t o † < Æ rt  “D hÓ ü t o ”, Volume 57, Number 4, 2008¸   10 Z 4

Fig. 1. Schematic of the GaN structure with LT AlN interlayer.

Fig. 2. XRD traces of the GaN films grown on Si (111) substrate with LT AlN interlayer thickness.

8

£

x s  é ß –  & ñ Ü ¼– Ð $ í  © œ† < Ê`  ¦ · ú ˜ à º e ” Ü ¼ 9, GaN (0002) €   õ

 › ' a >   ) a y © œô  Çx ß ¼ › ' a ¹ 1 Ï÷ &% 3  . s [ þ t   õ   H GaN 8 £ x s

 $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \   © œ › ' a\ O s  Z  }“ É r c−» ¡ ¤ C † ¾ Ó

$ í

õ  “ ¦¾ ¡ §| 9 _    & ñ $ í `  ¦ f ” `  ¦ ˜ Ð# Œï  r  . $ “ : r AlN ×  æ ç

ß –8 £ x ¿ ºa  5 nm, 10 nm, Õ ªo “ ¦ 20 nm { 9  M : 2θ ° ú כ

“

É r 33.85

, 34.5

, Õ ªo “ ¦ 34.55

– Ð    % i   H X < s   H 2  GaN 8 £ x _  6 £ x§ 4  (stress) s     o H † d`  ¦    · p . strain relaxation  ) a GaN _  2θ ° ú כ“   33.63

õ  q “ § €   5 nm Ò 

re  ¦ \ " f  H ´ ú §“ É r 6 £ x§ 4 s   Œ •6   x † < Ê`  ¦ · ú ˜ à º e ” % 3  .

Fig. 3   H normalski ‰ & ³p  â (x 50) Ü ¼– Ð › ' a ¹ 1 Ï  ) a $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \     $ í  © œô  Ç 2  GaN 8 £ x _  ³ ð€   

”

 s  . Fig. 2 (a) ∼ (c)   H $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa 

5 nm, 10 nm, Õ ªo “ ¦ 20 nm { 9  M : €  • 1.5 µm $ í  © œô  Ç 2  GaN ~ à Ì} Œ •\  @ /ô  Ç ³ ð€  s  . — ¸Ž  H Ò  re  ¦ \ " f Ä »o  o (mirror-like) ³ ð€  `  ¦ ˜ Ðs “ ¦ e ”  . $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa 

\

   É r ç  H\ P  x 9 • ¸  H 5 nm { 9  M :  © œ ´ ú §“ É r ç  H\ P s  ˜ Ð s

t ë ß – 10 nm ¿ ºa \ " f  H  _  — ¸Ž  H ç  H\ P s    & ’  

Fig. 3. Photomicrographs of the 1.5-¼m-thick GaN sur- face for LT AlN interlayer thicknesses of (a) 5 nm, (b) 10 nm, and (c) 20nm.

20 nm ¿ ºa  ÷ &€    r  ç  H\ P s  › ¸F K 7 £ x    H  ⠆ ¾ Ó`  ¦

˜

Ð% i  . s    õ \ " f ˜ Ѝ  H  % ƒ! 3  $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa  _

 p [ jô  Ç    o\ • ¸ GaN _  ç  H\ P x 9 • ¸  © œ{ © œy    y Œ ™ 

>

   † < Ê`  ¦ · ú ˜ à º e ” % 3  . 7 £ ¤, $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa    



o €  " f 2  GaN _  6 £ x§ 4 s     o÷ &% 3 l  M :ë  H“    כ Ü ¼– Ð ó

ø Íé ß –  ) a   [5]. z  ´] j ç  H\ P x 9 • ¸  H # Qb  G>     o % i   H t  · ú ˜



˜ Ðl  0 AK  ç  H\ P x 9 • ¸\  ¦ 8 £ ¤& ñ % i  . 5 nm, 10 nm, Õ ª o

“ ¦ 20 nm Ò  re  ¦ _  ç  H\ P x 9 • ¸  H y Œ •y Œ • 70 /cm, 5 /cm, Õ ª o

“ ¦ 30 /cm s % 3  .

$

“ : r AlN ×  æ ç ß –8 £ x ¿ ºa \    É r 2  GaN 8 £ x _    & ñ $ í

`

 ¦ · ú ˜ ˜ Ðl  0 AK  XRC 8 £ ¤& ñ `  ¦ % i  . Fig. 4 \  (002) FWHM 8 £ ¤& ñ   õ      e ”  . $ “ : r AlN ×  æ ç ß –8 £ x ¿ º a

 7 £ x † < Ê\    , GaN 8 £ x _    & ñ $ í s  † ¾ Ó © œ H † d`  ¦ ˜ Ðs 



 20 nm ¿ ºa \ " f ° ú š l    & ñ $ í s  $  ÷ &  H  ⠆ ¾ Ó`  ¦

˜

Ðs “ ¦ e ”  . s   õ   H   • ¸ e ” >  ¿ ºa \  ¦  Å # Q€     r

 6 £ x§ 4 `  ¦ ~ à Î  ç  H\ P s  µ 1 ÏÒ q t €  " f   & ñ $ í s    t l  M

:ë  H Ü ¼– Ð ó ø Íé ß –  ) a  . 5 nm, 10 nm, Õ ªo “ ¦ 20 nm _  $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \ " f (002) FWHM “ É r y Œ •y Œ • 933 arcsec, 651 arcsec, Õ ªo “ ¦ 825 arcsec s % 3  . ¢ ¸ô  Ç, XRC x ß ¼ y

© œ• ¸  H (002) FWHM 8 £ ¤& ñ   õ ü < { 9 u   9 $ “ : r AlN

×

 æ ç ß –8 £ x ¿ ºa  10 nm { 9  M :  © œ Z  }“ É r x ß ¼y © œ• ¸\  ¦ ˜ Г  



. $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa  10 nm { 9  M :  © œ a % ~“ É r   

&

ñ $ í `  ¦ ˜ Ð% i  .

$

“ : r AlN ×  æ ç ß –8 £ x ¿ ºa  F g † < Æ& h “   : £ ¤$ í \  p u   H % ò

†

¾ Ó`  ¦ › ' a ¹ 1 Ï l 0 AK  PL 8 £ ¤& ñ `  ¦ % i  . Õ ªa Ë > 5   H  © œ“ : r

\

" f 8 £ ¤& ñ  ) a $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \    É r 2  GaN 8 £ x _

 PL : £ ¤$ í `  ¦   ? /“ ¦ e ”  . PL x ß ¼ 0 Au   H 5 nm − 3.376 eV, 10 nm − 3.376 eV, Õ ªo “ ¦ 20 nm − 3.385 eV

#

3 0 A\  ¦ t “ ¦ e ” Ü ¼ 9 $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \     x 

(3)

 ƒ  ½ ¨ 7 Hë  H  Si (111) l ó ø Í0 A\  $ í  © œô  Ç GaN 8 £ x _  $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \    É r : £ ¤$ í – ^ ”  ü ½ © -289-

Fig. 4. (002) X-ray rocking curves of GaN layer with LT AlN interlayer thickness.

Fig. 5. PL properties of GaN layer with LT AlN inter- layer thickness at RT.

ß

¼ 0 Au  › ¸F Km ”  blue-shift ÷ &% 3  . s  PL x ß ¼ 0 Au   H



 s # Q l ó ø Í0 A\ " f strain relaxation  ) a GaN _  x ß ¼

˜

Ð  €  • 35 ∼ 45 meV ± ú “ É r ° ú כs   [6]. $ “ : r AlN ×  æ ç ß – 8

£

x ¿ ºa \    " f      H blue-shift ‰ & ³ © œ“ É r Si l ó ø Íõ  _

 \ P Ø Ÿ ‚ ½ Ó> à º s \  _ K  biaxial strain  ) a GaN 8 £ x \ 

"

f ˜ Ðs   H PL x ß ¼   s s  9 s  Qô  Ç ‰ & ³ © œ“ É r GaN \   Œ • 6

 

x   H stress _     o\  _ ô  Ç  כ Ü ¼– Ð ó ø Íé ß –  ) a   [5]. ¢ ¸ô  Ç,

$

“ : r AlN ×  æ ç ß –8 £ x ¿ ºa  7 £ x † < Ê\     x ß ¼ y © œ• ¸  H 7 £ x

, PL FWHM “ É r & h & h  y Œ ™™ è† < Ê`  ¦ ˜ Ðs   20 nm ¿ ºa 

\

" f x ß ¼ y © œ• ¸  H y Œ ™™ è, PL FWHM “ É r 7 £ x † < Ê`  ¦ ˜ Ðs “ ¦ e ”

 . s    õ   H · ú ¡_  XRC   õ ü < { 9 u  “ ¦ V−/ B G‚    â

†

¾ Ó`  ¦ ˜ Ð% i  . PL FWHM “ É r 5 nm − 43.7 meV, 10 nm

− 38.1 meV, Õ ªo “ ¦ 20 nm − 47.1 meV `  ¦ % 3 % 3  . $ 

“

: r AlN ×  æ ç ß –8 £ x ¿ ºa  10 nm { 9  M :  © œ a % ~“ É r PL : £ ¤$ í

`

 ¦ ˜ Ð% i  .

IV. + s Ç Â ] Ø

‘

: r ƒ  ½ ¨\ " f  H MOCVD Z O Ü ¼– Ð $ “ : r AlN ×  æ ç ß –8 £ x ¿ º a

› ¸] X `  ¦ : Ÿ x K  Si l ó ø Í0 A\  “ ¦¾ ¡ §| 9  GaN ~ à Ì} Œ •`  ¦ $ í  © œ 

%

i  . $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa \     GaN _  ç  H\ P  x 9 • ¸

   y Œ ™ >    † < Ê`  ¦ · ú ˜ à º e ” % 3 “ ¦ 10 nm $ “ : r AlN ×  æ ç ß – 8

£

x ¿ ºa \ " f  © œ & h “ É r ç  H\ P  x 9 • ¸\  ¦ S X ‰ “   % i  . s     õ

  H $ “ : r AlN ×  æ ç ß –8 £ x ¿ ºa  2  GaN $ í  © œ\  e ” # Q" f

×

 æ כ ¹ô  Ç % i ½ + É`  ¦ † < Ê`  ¦    · p .

Y

c p w Š à U Ø ”  ô

[1] G. Cong, Y. Lu, W. Peng, X. Liu, X. Wang and Z.

Wang, J. Crystal Growth 276, 381 (2005).

[2] K. Engl, M. Beer, N. Gmeinwieser, U. T. Schwarz, J. Zweck, W. Wegscheider, S. Miller, A. Miler, H.-J.

Lugauer, G. Br¨ uderl, A. Lell and V. H¨ arle, J. Crystal Growth 289, 6 (2006).

[3] Y. L. Tsai and J. R. Gong, Opt. Mater. 27, 425 (2004).

[4] G. S. Higashi, Y. J. Chabal, G. W. Trucks and K.

Laghavachari, Appl. Phys. Lett. 56, 656 (1990).

[5] Deok Kyu Kim, SAEMULLI (New Phys.) 55, 43 (2007).

[6] S. Chichibu, H. Okumura, S. Nakamura, G. Feuillet, T. Azuhata, T. Sota and S. Yoshida, Jpn. J. Appl.

Phys. 36, 1976 (1997).

(4)

-290- ô  Dz D GÓ ü t o † < Æ rt  “D hÓ ü t o ”, Volume 57, Number 4, 2008¸   10 Z 4

Properties of GaN on a Si(111) substrate for Various LT AlN Interlayer Thicknesses

Deok Kyu Kim

Division of Electronics and Information Engineering, Cheongju University, Cheongju 360-746 (Received 31 July 2008)

GaN layers were grown on silicon (111) substrates with low-temperature (LT) AlN interlayers by using metalorganic vapor-phase epitaxy, and the properties of the GaN layers were investigated for various LT AlN interlayer thicknesses. With LT AlN interlayer, cracks in the GaN layer changed sensitively. For 10-nm-thick LT AlN, the density of cracks was 5/cm, the full width at half maximum of the (002) X-ray rocking curve was 651 arcsec, and the full width at half maximum of the bound exciton line was as low as 38.1 meV at 300 K.

PACS numbers: 68.55.-a, 62.20Mk, 81.40.Jj

Keywords: Low-temperature AlN layer, Crack, Silicon (111), Metalorganic chemical vapor deposition

E-mail: [email protected]

수치

Fig. 2. XRD traces of the GaN films grown on Si (111) substrate with LT AlN interlayer thickness.
Fig. 5. PL properties of GaN layer with LT AlN inter- inter-layer thickness at RT.

참조

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