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As/GaAs “ ¦„ s 1 l x • ¸ à Ô ½ ™t Û ¼'  (high electron mobility transistor; HEMT) ½ ¨› ¸ _

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(2008¸  4 Z 4 25{  ~ Ã Î6 þ j7 r 8 Z 4 27{  ~ Ã Î6

Al

0.3

Ga

0.7

As/GaAs “ ¦„    s 1 l x • ¸ à Ô ½ ™t Û ¼'  (high electron mobility transistor; HEMT) ½ ¨› ¸ _

 : £ ¤$ í `  ¦ “ : r • ¸ 18-300 K # 3 0 A\ " f electroreflectance (ER) ~ ½ ÓZ O Ü ¼– Ð › ¸  % i  .  © œ“ : r ER ’    ñ\ " f

 

H €  • 1.41, 1.80 x 9 1.75 eV\ " f_  3> h_  x ß ¼ › ' a8 £ ¤ ÷ &% 3  . s  x ß ¼[ þ t“ É r GaAs, AlGaAs x 9 GaAs_  spin-orbital splitting \  › ' aº   ) a ’    ñs % 3  . Õ ªo “ ¦ 8 £ ¤& ñ  ) a Franz-Keldysh oscillations (FKO) – РÒ' ,

%

i ~ ½ ӆ ¾ Ó  s # QÛ ¼ „  · ú š (V

dc

) s  7 £ x † < Ê\     > €   „  l  © œ_  [ jl   H 7 £ x  % i  . ¢ ¸ô  Ç V

dc

=−7 V Â Ò



 H \ " f GaAs ’    ñ– РÒ'  2 " é ¶ „   Û ¼ (2DEG)_  ’    ñ ì  r o ÷ &% 3 Ü ¼ 9,  € ª œô  Ç “ : r • ¸\ " f 2DEG 0

l

x • ¸ (N

2D

)\  ¦ ½ ¨ % i  .

PACS numbers: 78.40.Fy

Keywords: AlGaAs/GaAs “ ¦„    s 1 l x • ¸ à Ô ½ ™t Û ¼' , „  l ì ø Í Ö  ¦, 2 " é ¶ „   Û ¼

I. " e  ] Ø

ì

ø ͕ ¸^ ‰\  Å Òl & h “   [ O 1 l x`  ¦  # Œ „  l  · F g † < Æ& h  “    _

    o\  ¦ 8 £ ¤& ñ   H   › ¸ ì  rF g † < Æ [1]“ É r V , o   6   x ÷ &“ ¦ e ” 



.   › ¸ ì  rF g † < Æ_  ô  Ç ì  r À ӓ   electroreflectance (ER)Z O 

“ É

r ì ø ͕ ¸^ ‰\  „  l  © œ`  ¦ “   # Œ / B N ç ß – „   8 £ x _  „  l  © œ

`

 ¦   › ¸r v “ ¦ s \    É r ì ø Í Ö  ¦ _     o\  ¦ 8 £ ¤& ñ   H ~ ½ Ó Z O

s  . ER ’    ñ\ " f Franz-Keldysh oscillations (FKO) _

 ”  1 l x Å Òl   H / B N ç ß – „   8 £ x ? /\ " f „  l  © œõ  › ' aº  s  e ”  Ü

¼ 9 [2], s 7 á x] X ½ + Ë ½ ¨› ¸\ " f      H FKO  H s 7 á x] X ½ + Ë

>

€  \  + þ A$ í  ) a / B N ç ß – „   8 £ x \  _ K  µ 1 ÏÒ q tô  Ç  [3].   

"

f  s # QÛ ¼ „  · ú š (V dc ) 7 £ x \    É r FKO _     o– РÒ'  AlGaAs/GaAs s 7 á x] X ½ + Ë ½ ¨› ¸_  / B N ç ß – „   8 £ x \ " f + þ A$ í

 )

a > €   „  l  © œ    o\  ¦ \ V8 £ ¤ ½ + É Ã º e ”  .

AlGaAs/GaAs s 7 á x] X ½ + Ë ½ ¨› ¸\ " f 2 " é ¶ „   Û ¼ (two dimensional electron gas; 2DEG) \  @ /ô  Ç ƒ  ½ ¨  H t  5

Å

q ÷ &# Q M ® o  . Sydor 1 p x [4,5]“ É r GaAs cap8 £ x _  \ g A\   



É r AlGaAs/GaAs  â > €  \ " f_  + þ A    oü < differen- tial photoreflectance (DPR)Z O Ü ¼– Ð 8 £ ¤& ñ ô  Ç   õ \  ¦ q “ §

# Œ 2DEG_  ” > r F \  ¦ S X ‰ “   % i  . Hwang 1 p x [6]“ É r Al- GaAs/GaAs s 7 á x] X ½ + Ë_  \ g A ´ òõ \  ¦ photoreflectance (PR) – Ð ƒ  ½ ¨ % i “ ¦, Zamora 1 p x [7]“ É r Y Us $ _  g Ë >È Ò U  · s

\    É r PR ’    ñ_  s \  ¦ : Ÿ x K  AlGaAs/GaAs “ ¦„  



 s 1 l x • ¸ à Ô ½ ™t Û ¼'  (high electron mobility transistor;

E-mail: [email protected]

HEMT) _  2DEG ’    ñ\  ¦ › ' a ¹ 1 Ï % i  . 7 £ ¤, 2DEG ü < ×  æ^ o ?

 )

a ’    ñ_    H" é ¶`  ¦ ] j † < ÊÜ ¼– Ð+ ‹ 2DEG ’    ñ\  ¦ " î S X ‰ > 

› '

a ¹ 1 Ͻ + É Ã º e ”  . s ü < ° ú  s  AlGaAs/GaAs HEMT_  ƒ  

½

¨  H ŠҖ Ð PR, DPRõ  ° ú  “ É r F g& h  # Œl " é ¶`  ¦  6   x # Œ z  ´ +

« > % i Ü ¼ 9, ER`  ¦ s 6   x ô  Ç ì  r$ 3 “ É r p q ô  Ç z  ´& ñ s  .

‘

: r  7 Hë  H \ " f  H Al 0.3 Ga 0.7 As/GaAs HEMT ½ ¨› ¸\  @ / ô

 Ç : £ ¤$ í `  ¦ ERZ O Ü ¼– Ð › ¸  % i  . % i ~ ½ ӆ ¾ Ó V dc 7 £ x  r  FKO _  ”  1 l x Å Òl     o “ ¦ [ jl  y Œ ™™ è† < Ê\     GaAs _  ’    ñü < ×  æ^ o ?÷ &# Qe ” ~   2DEG ’    ñ GaAs {  ç

ß –   \  -t  Å Ò0 A\ " f # QL : x ß ¼– Ð › ' a8 £ ¤ ÷ &% 3  . Õ ªo “ ¦

“

: r • ¸    o\    É r 2DEG 0 l x • ¸\  ¦ › ¸  % i  .

II. ÷ m Ç ] M ö

‘

: r ƒ  ½ ¨\   6   x ) a r « э  H MBEZ O Ü ¼– Ð ì ø Í] X ƒ  $ í GaAs l

ó ø Í0 A\  $ í  © œ “ : r • ¸ 580 C \ " f ¢ - aØ  æ8 £ x Ü ¼– Ð Ô  ¦í  HÓ ü t s  ' ‘ 

÷ &t  · ú §“ É r GaAs\  ¦ 700 nm ¿ ºa – Ð $ í  © œ % i  . Õ ª 0 A

\

 Ô  ¦í  HÓ ü t s  ' ‘ ÷ &t  · ú §“ É r 10 nm _  Al 0.3 Ga 0.7 As / B N ç ß – 8

£

x`  ¦ $ í  © œô  Ç Ê ê, Sis  • ¸i ç  ) a 50 nm _  Al 0.3 Ga 0.7 As 8 £ x õ

 10 nm_  GaAs 8 £ x`  ¦ $ í  © œ % i  . ER 8 £ ¤& ñ `  ¦ 0 A # Œ H 3 PO 4 : H 2 O 2 : H 2 O (1 : 1 : 38) ™ D ¥ ½ + Ë 6   xÓ  o\ " f 6ì  r 1 l x î

ß – d ” y Œ •`  ¦ ô  Ç Ê ê, Schottkyü < ohmic ] X ½ + ËÜ ¼– Ð y Œ •y Œ • Auü <

Au-Ge`  ¦ ”  / B N 7 £ x ‚ Ã Ì % i  . r « Ñ_  é ß –€  • ¸  H Fig. 1 õ  ° ú  



. ER 8 £ ¤& ñ “ É r   › ¸„  · ú š (V ac )`  ¦ 0.8∼5 V – Ð    or &  ’    

ñ\  ¦ 8 £ ¤& ñ % i Ü ¼ 9, V ac \  ¦ { 9 & ñ >  ô  Ç Ê ê, dc  s # QÛ ¼

-200-

(2)

Fig. 1. A schematic sample structure with contact con- figuration.

„

 · ú š (V dc )`  ¦ −9∼4 V – Ð    or &  ER ’    ñ_     o\  ¦ › ' a 8

£

¤ % i  . 8 £ ¤& ñ r    › ¸ Å Ò à º  H 1 kHz – Ð “ ¦& ñ % i “ ¦,

›

¸  F g " é ¶ Ü ¼– Ð 250 W_  ) í Û ¼J $ ™-½ + ɖ Ð  p Ï þ ›á Ô\  ¦  6   x % i 



.

III. + s ÇÊ Ý õ m Í À X Ø8 ý

Fig. 2  H Al 0.3 Ga 0.7 As/GaAs HEMT ½ ¨› ¸_   © œ“ : r ER Û

¼& 7 ˜à Ô! 3 `  ¦   ? /% 3  . Õ ªa Ë >\ " f ˜ Ѝ  H  ü < ° ú  s  €  • 1.41, 1.80 x 9 1.75 eV\ " f › ' a8 £ ¤ ) a ’    ñ[ þ t“ É r y Œ •y Œ • GaAs, AlGaAs x 9 GaAs_  spin-orbital splitü < › ' aº   ) a ’    ñs 



. y Œ • ’    ñ_  & ñ S X ‰ ô  Ç \  -t  ° ú כ`  ¦ ½ ¨ l  0 AK   6 £ § õ 

° ú

 “ É r Aspnes _  $ „  l  © œ % ò % i \ " f_  3  p ì  r+ þ AI _  † < Ê Ã

ºd ”  [4]Ü ¼– Ð x h A`  ¦ % i  .

∆R R = Re

p

X

j=1

C j e

j

(E − E g + iΓ j ) −n (1)

#

Œl " f E g   H {  ç ß –   \  -t , Γ j   H ¨ î ò ø ͓   , C j   H ”  ; Ÿ ¤, θ j   H 0 A © œ`  ¦ y Œ •y Œ •    · p . n“ É r e ” > & h  + þ AI \  _ ” > r   H

‚

 + þ A“   – Ð n=2.5_  ° ú כ`  ¦  6   xÙ þ ¡“ ¦, s   H 3 " é ¶ { ç ß – „   s

\  K { © œ  ) a  . d ”  (1)`  ¦ s 6   x # Œ x h Aô  Ç   õ  1.413 eV _

 ’    ñ  H • ¸i ç ÷ &t  · ú §“ É r ¢ - aØ  æ8 £ x GaAs _  {  ç ß –   \  - t

 E g (GaAs) s  9, 1.755 eV  H GaAs _  spin-orbital split (E g + ∆E) ’    ñs  . Õ ªo “ ¦ AlGaAs_  {  ç ß –   \  -t  E g (AlGaAs)  H 1.804 eV s “ ¦, Al › ¸$ í q  (x)  H 0.30 s % 3 



. ô  Ǽ # , FKO  H • ¸i ç  ) a ì ø ͕ ¸^ ‰ r « Ñ_  / B N ç ß – „   8 £ x \ 

"

f › ' a ¹ 1 Ͻ + É Ã º e ”   H X < [8], E g (GaAs) Å Ò0 A_  FKO  H r « Ñ

$ í

 © œ õ & ñ ×  æ \  _ • ¸ t  · ú §“ É r ¢ - aØ  æ8 £ x _  • ¸i ç \  _ K   

è ß –  כ Ü ¼– Ð  « Ñ  ) a  .   " f E g (GaAs) Å Ò0 A_  FKO x

ß ¼[ þ t õ  x h A   õ  { 9 u  t  · ú §  H  . Fig. 3“ É r   › ¸

„

 · ú š (V ac ) _  7 £ x \    É r ER ’    ñ_     o\  ¦   ? /% 3 



. „  · ú šs  7 £ x † < Ê\     y Œ • ’    ñ_  + þ AI   H  _     o\ O  s

 [ jl ë ß – 7 £ x  % i  . s   H Bhattacharya 1 p x [9] _    õ 

Fig. 2. ER spectra of the Al 0.3 Ga 0.7 As/ GaAs HEMT at the room temperature.

ü

< { 9 u ô  Ç . Õ ª Q  E g (GaAs) s  © œ_  \  -t \ " f ¢ - a ë

ß –ô  Ç ’    ñ  =/ B G ÷ &# Q   z Œ ¤  H X <, s   H z  ´+ « >\   6   x ) a r

« Ñ_  ½ ¨› ¸ bulk ¢ ¸  H é ß –{ 9 8 £ x s       8 £ x ½ ¨› ¸\  ¦  t

l  M :ë  H s  . 7 £ ¤, “    ) a „  l  © œ\  @ /ô  Ç r « Ñ\  ¦ ½ ¨$ í

  H y Œ • 8 £ x _   ½ ™× ¼ … ô a & ñ • ¸ ² ú ˜ " f s [ þ t ç ß –_   © œ  ñ Œ • 6

 

x \  _ K  ’    ñ    o   H  כ s  .

Fig. 4 \ " f  H   › ¸ „  · ú šs  { 9 & ñ (V ac =1V) ½ + É M :, Al 0.3 Ga 0.7 As/GaAs HEMT r « Ñ_  í  H ~ ½ ӆ ¾ Ó V dc \    É r ER ’    ñ_     o\  ¦   ? /% 3  . V dc  7 £ x † < Ê\     y Œ •

’

   ñ[ þ t _  0 Au   H  _     o\ O s  [ jl ë ß – y Œ ™™ è % i  . Õ ª o

“ ¦ GaAs_  FKO ’    ñ  H ”  1 l x Å Òl   ú ª t “ ¦ [ jl • ¸ y

Œ

™™ è   H  כ `  ¦ ^  ¦ à º e ”  . s  Qô  Ç ‰ & ³ © œ“ É r í  H ~ ½ ӆ ¾ Ó V dc \  _

K  r « Ñ ? / Ò_  / B N ç ß – „   8 £ x ; Ÿ ¤ _  y Œ ™™ è– Ð > €   „  l  © œ s

 y Œ ™™ è l  M :ë  H s  . % i ~ ½ ӆ ¾ Ó V dc \    É r ER ’    ñ_ 



  o  H Fig. 5 ü < ° ú   . V dc  7 £ x † < Ê\     í  H ~ ½ ӆ ¾ Óõ    ð

ø Ít – Ð „  ì ø Í& h “   ’    ñ_  [ jl  y Œ ™™ è   H ì ø ̀  , FKO _

 ”  1 l x Å Òl  7 £ x  % i  . s   H V dc  7 £ x † < Ê\     r

« Ñ ? /\  + þ A$ í  ) a / B N ç ß – „   8 £ x _  ; Ÿ ¤ s  7 £ x  # Œ > €   „   l

 © œs  7 £ x  l  M :ë  H s   [9].



 " f Fig. 4ü < 5_  z  ´+ « >   õ   H Aspnes [11]  Šҁ © œ ô

 Ç  ü < ° ú  s  V dc \    É r r « Ñ_  „  l  x 9 F g † < Æ& h  ´ òõ   H

~

½ ӆ ¾ Ó\  › ' a > \ O s  Õ ª ß ¼l \  _ ” > r % i  . Õ ªo “ ¦ V dc 7 £ x

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Fig. 3. ER spectra of Al 0.3 Ga 0.7 As/ GaAs HEMT for various modulation voltages (V ac ) at room temperature.

\    É r ’    ñ_  y Œ ™™ èÖ  ¦“ É r í  H ~ ½ ӆ ¾ Ó_   â Ä º % i ~ ½ ӆ ¾ Ó_ 

 â

Ä º ˜ Ð   8 ß ¼ . s  Qô  Ç   õ   H Wang 1 p x [2] _    õ ü <

{ 9

u  % i  .

%

i ~ ½ ӆ ¾ Ó V dc  7 £ x † < Ê\     E g (GaAs) \ " f “ ¦\  - t

– Ð €  • 30 meV & ñ • ¸ b  # Q”   / B M \ " f Æ Ò& h “   + þ A (A) s

 › ' a8 £ ¤ ÷ &% 3  . A_    H" é ¶“ É r Al 0.3 Ga 0.7 As/GaAs  â > €  

\

 + þ A$ í  ) a 2DEG \  › ' aº   ) a ’    ñs   [4–7]. t F K  t  2DEG ’    ñ\  ¦ ì  r o  l  0 Aô  Ç ~ ½ ÓZ O Ü ¼– Ѝ  H Y Us $ _  g Ë >È Ò U

 ·s , r « Ñ_  \ g A 1 p x`  ¦  6   x % i  . 7 £ ¤, 2DEG ü < ×  æ^ o ? ) a

’

   ñ_    H" é ¶`  ¦ ] j † < ÊÜ ¼– Ð+ ‹ 2DEG_  ’    ñ\  ¦ " î S X ‰ > 

› '

a ¹ 1 Ïô  Ç  כ s  . % i ~ ½ ӆ ¾ Ó V dc 7 £ x \     FKO_  ”  1 l x Å Ò l

  H 7 £ x  “ ¦ [ jl   H y Œ ™™ è % i   [10].   " f Fig. 2\ 

"

f ˜ Ѝ  H  ü < ° ú  s  GaAs ’    ñü < ×  æ^ o ?÷ &# Q e ” ~   2DEG

’

   ñ Fig. 5_    õ ü < ° ú  s  ì  r o ÷ &# Q   z Œ ¤ . s % ƒ! 3  2DEG ’    ñ GaAs ’    ñü < ×  æ^ o ?÷ &# Q e ” l  M :ë  H \  Fig.

5 \ " f 1 p x ç ß –  Ü ¼– Ð     ½ + É FKO_  ”  1 l x Å Òl  { 9 & ñ

t  · ú §>       H  כ s  . ì  r o   ) a 2DEG ’    ñ_  \  - t

ü < · ú ¡" f ½ ¨K ”   E g (GaAs) – РÒ'  AlGaAs/GaAs  â > 

€

 \  + þ A$ í  ) a 2DEG % ò % i _  0 l x • ¸  H

E 2DEG i = E c GaAs − E v GaAs + E W i (2)

= E GaAs g + (2m∗) −1/3 (~e 2 N 2D /) 2/3 r i

Fig. 4. ER spectra of Al 0.3 Ga 0.7 As/ GaAs HEMT at various forward dc bias voltages.

Fig. 5. ER spectra of Al 0.3 Ga 0.7 As/ GaAs HEMT at

various reverse dc bias voltages.

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Fig. 6. The temperature dependence of Al 0.3 Ga 0.7 As/

GaAs HEMT.

Ü

¼– Ð   è ­ q à º e ”  . # Œl " f E g GaAs   H GaAs _  {  ç ß –  

\

 -t s “ ¦, m “ É r Ä »´ ò | 9 | ¾ Ó, ~  H Planck  © œÃ º, N 2D   H 2DEG 0 l x • ¸s  9, r 0 = 2.238, r 1 = 4.087, r 2 = 5.520, ... s   [12]. d ”  (2)  H E g GaAs ü < E i 2DEG _  \  -t \  ¦ · ú ˜ M

:, 2DEG 0 l x • ¸\  ¦ > í ß –½ + É Ã º e ” 6 £ §`  ¦ _ p ô  Ç . Õ ªo “ ¦ „   s

 \  -t   H d ”  (1)`  ¦ s 6   x % i Ü ¼ 9, E g GaAs ü < E i 2DEG _  n“ É r y Œ •y Œ • 2.5ü < 3`  ¦ @ /{ 9  % i  . V dc =−9 V \ " f " î S X ‰ 

>

 ì  r o   ) a A ’    ñ– РÒ'  ½ ¨ô  Ç 2DEG_  0 l x • ¸ (N 2D )  H 1.6

× 10 11 /cm 2 s % 3 Ü ¼ 9, s  ° ú כ“ É r Hwang 1 p x [6] s  ½ ¨ô  Ç 3.92

× 10 11 /cm 2 ˜ Ð  €  •ç ß – & h % 3  . ’    ñ A_  “ : r • ¸ _ ” > r$ í `  ¦

›

¸  l  0 AK  “ : r • ¸ 18-300 K_  # 3 0 A\ " f › ' a8 £ ¤ ) a ER Û ¼

&

7 ˜à Ô! 3 [ þ t`  ¦ Fig. 6 \    ? /% 3  . “ : r • ¸ y Œ ™™ è† < Ê\     x

ß ¼ A_  [ jl  7 £ x  “ ¦, GaAs ’    ñü < " î S X ‰ >  ì  r o 

÷

&# Q   z Œ ¤ . s   H $ “ : r Ü ¼– Ð ° ú ˜Ã º2 Ÿ ¤ \ P \  -t \  _ K 



    H \ P & h  Ÿ í 7 H _  y Œ ™™ è– Ð “  K  2DEG ? /Â Ò „   ü <

_

  © œ  ñ Œ •6   x s  y Œ ™™ è # Œ „   _  s 1 l x • ¸ 7 £ x  l  M : ë

 H s   [13]. Õ ªo “ ¦ E g (GaAs) ü < x ß ¼ A_  \  -t   s

  H “ : r • ¸\     7 £ x  % i  . d ”  (2)\  ¦ s 6   x # Œ 2DEG _

 0 l x • ¸\  ¦ “ : r • ¸\       ? /€   Fig. 7õ  ° ú   . Õ ªa Ë >Ü ¼

–

РÒ'  2DEG_  0 l x • ¸  H $ “ : r \ " f  © œ“ : r Ü ¼– Ð ° ú ˜Ã º2 Ÿ ¤ 7 £ x 

†

< Ê`  ¦ · ú ˜ à º e ”  .

Fig. 7. Temperature dependence of the 2DEG concen- tration.

IV. + s Ç Â ] Ø

Al 0.3 Ga 0.7 As/GaAs HEMT r « Ñ_   © œ“ : r ER z  ´+ « >    õ

 1.413, 1.755, 1.804 eV\ " f › ' a8 £ ¤ ) a x ß ¼  H y Œ •y Œ • GaAs, spin-split orbital, Al 0.3 Ga 0.7 As ü < › ' aº   ) a ’    ñs  .   › ¸

„

 · ú š (V ac ) _  7 £ x \     y Œ • x ß ¼_  0 Au   H  _      t

 · ú §t ë ß –, E g (GaAs) s  © œ_  \  -t \ " f ¢ - a ë ß –ô  Ç ’    ñ

  =/ B G ÷ &  H ‰ & ³ © œ“ É r   › ¸ „  l  © œ\  _ ô  Ç  8 £ x ½ ¨› ¸ ? /Â Ò _

  ½ ™× ¼ … ô a s \  l “  ô  Ç .  s # QÛ ¼ „  · ú š (V dc ) s  7 £ x

½ + Éà º2 Ÿ ¤ „  ^ ‰& h “   ’    ñ í  H ~ ½ ӆ ¾ Óõ  % i ~ ½ ӆ ¾ Ó — ¸¿ º y Œ ™™ è

% i  . Õ ªo “ ¦ FKO_  ”  1 l x Å Òl   H % i ~ ½ ӆ ¾ Ó „  · ú šs  7 £ x

½ + Éà º2 Ÿ ¤ U  ´# Qt “ ¦ Õ ª [ jl   H y Œ ™™ èô  Ç . s   H / B N ç ß – „    8

£

x ; Ÿ ¤ s  % i ~ ½ ӆ ¾ Ó „  · ú š 7 £ x \     V , # Q4 R r « Ñ_  F gf  ¨ Ã

º_  7 £ x – Ð > €   „  l  © œs  7 £ x  l  M :ë  H s  . % i ~ ½ ӆ ¾ Ó V dc 7 £ x \    É r FKO _     o\  ¦ : Ÿ x K  GaAs ’    ñü < ×  æ

^ o

?÷ &# Q e ” ~   2DEG › ' aº   ’    ñ\  ¦ › ' a8 £ ¤ ½ + É Ã º e ” Ü ¼ 9,  © œ“ : r

\

" f V dc =−9V{ 9  M : ½ ¨ô  Ç 2DEG_  0 l x • ¸ (N 2D )  H 1.6 × 10 11 /cm 2 s % 3 “ ¦, “ : r • ¸ 7 £ x ½ + Éà º2 Ÿ ¤ N 2D   H & h  – Ð 7 £ x

 % i  .

Y

c p w Š à U Ø ”  ô

[1] O. J. Glembocki, Appl. Phys. Lett. 46, 970 (1985).

(5)

[6] I. Hwang, Solid State Communications 103, 1 (1997).

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Electroreflectance Spectroscopy of an Al 0.3 Ga 0.7 As/GaAs High Electron Mobility Transistor Structure

Byoung-Soo Ko and In-Ho Bae

Department of Physics, Yeungnam University, Gyeongsan 712-749 (Received 25 April 2008, in final form 27 August 2008)

Electroreflectance (ER) studies of the Al

0.3

Ga

0.7

As/GaAs high electron mobility transistor (HEMT) structure were performed in the temperature range of 18-300 K. The room-temperature ER spectra showed three signals: 1.41, 1.80 and 1.75 eV. These were attributed to the band edges of GaAs and AlGaAs and to the spin-orbital splitting of GaAs, respectively. From the measured Franz-Keldysh oscillations (FKO), we found that the strength of the interfacial electric field in- creasesd as the reverse dc bias voltage (V

dc

) was increased. We also observed that two-dimensional electron gas (2DEG) was separated from the GaAs signal of about V

dc

=-7 V, and we determined the 2DEG concentrations were taken at various temperatures.

PACS numbers: 78.40.Fy

Keywords: AlGaAs/GaAs HEMT, Electroreflectance, 2DEG

E-mail: [email protected]

수치

Fig. 1. A schematic sample structure with contact con- con-figuration. „ ·ú š (V dc )`¦ −9∼4 V – Ð   or &amp;  ER ’   ñ_    o\¦ ›'a 8£¤ 
 %i  
Fig. 3. ER spectra of Al 0.3 Ga 0.7 As/ GaAs HEMT for various modulation voltages (V ac ) at room temperature.
Fig. 6. The temperature dependence of Al 0.3 Ga 0.7 As/ GaAs HEMT. Ü ¼– Ð   è­ q à º e”  

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