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AlSb/InAs/AlSb W ë s – ¤ö n Ú  Œ º; c" e InSb-like 4 ì Å8 ý  ¹ ÅM X ì Ä — ¤V R Ë

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AlSb/InAs/AlSb W ë s – ¤ö n Ú  Œ º; c" e InSb-like 4 ì Å8 ý  ¹ ÅM X ì Ä — ¤V R Ë

{

¡* å # Ò · ™ »' Ö <%  

Ø 

æ z Œ ™@ /† < Ɠ § Ó ü t o † < Æõ , @ /„   305-764



¡< ‹ û B

ô

 ǀ ª œ@ /† < Ɠ § „  l „   ] j# Q> 8 £ ¤/ B N † < Æõ , î ß –í ß – 426-791

™ »* å g Y @

ô

 Dz D G ³ ðï  r õ † < ƃ  ½ ¨" é ¶, @ /„   305-340

™ » ö ¶ B~ ç ¡

× 

æ  Ò@ /† < Ɠ § & ñ ˜ Ð: Ÿ x’  † < Æõ , F K í ß – 312-702



™ »g ` @  ™ ¸

1 l

x² D G @ /† < Ɠ § ì ø ͕ ¸^ ‰õ † < Æõ , " fÖ  ¦ 100-715 (2007¸   3 Z 4 28{ 9  ~ à Î6 £ §)

‘

: r ƒ  ½ ¨\ " f  H GaAs l ó ø Í 0 A\  molecular beam epitaxy Z O Ü ¼– Ð $ í  © œ  ) a AlSb/InAs/AlSb € ª œ Ä ºÓ ü t

½

¨› ¸\ " f InAs G V ,  0 A,  A  InSb-like > €  `  ¦ + þ A$ í # Œ „  l & h , ½ ¨› ¸& h  : £ ¤$ í `  ¦ reflection high-energy electron diffraction, transmission electron microscopy, Hall ´ òõ  1 p x Ü ¼– Ð › ¸  % i  . 30 nm InAs G

V ,  0 A,  A  InSb-like > €   ½ ¨› ¸– РÒ'   © œ“ : r \ " f 20,700 cm

2

V·s _  „    s 1 l x • ¸\  ¦ % 3 % 3 Ü ¼ 9, ¢ ¸ô  Ç

“ :

r • ¸_ ” > r$ í 8 £ ¤& ñ Ü ¼– РÒ'  > €  \  InSb-like > €  s  + þ A$ í ÷ &% 3 6 £ §`  ¦ S X ‰ “   % i  .

PACS numbers: 73.61 Ey, 73.63.Hs, 81.15.Hi

Keywords: InAs, AlSb, > €  , TEM, Hall ´ òõ  8 £ ¤& ñ , „   s 1 l x • ¸

I. " e  ] Ø

III-V € ª œ Ä ºÓ ü t ½ ¨› ¸ ×  æ  “   AlSb/InAs/AlSb (s   InAs/AlSb – Ð ³ ðr ) € ª œ ½ ¨› ¸  H type II  ½ ™× ¼& ñ § > =`  ¦  9 1.35 eV _  Z  }“ É r „  • ¸@ / s _  ° ú כ`  ¦ ° ú   H  .  Ö  ¦  Q s 

½

¨› ¸  H Z  }“ É r „    x 9 • ¸ü < s 1 l x • ¸\  ¦ ° ú   H 2 " é ¶ „     Û

¼ (two-dimensional electron gases, 2DEG)8 £ x`  ¦ + þ A$ í  Ù

¼– Ð $ „  § 4  “ ¦5 Å q ™ è  6 £ x6   x \  & h ½ + Ëô  Ç ½ ¨› ¸s   [1–7].

InAs/AlSb € ª œ Ä ºÓ ü t ½ ¨› ¸  H GaAs/(Al,Ga)As, (Ga, In)As/(Al,In)As ½ ¨› ¸[ þ t õ    É r : £ ¤ s ô  Ç > €   ½ ¨› ¸\  ¦ + þ A

$ í

ô  Ç . Õ ª s Ä »  H € ª œ Ä ºÓ ü t`  ¦ s À ғ ¦ e ”   H ¿ º Ó ü t| 9 _  6 £ § s

“ : r õ  € ª œs “ : r s  — ¸¿ º  Ø Ôl  M :ë  H s  9 $ í  © œZ O \    

¿

º 7 á x À Ó_  > €  `  ¦ + þ A$ í ½ + É Ã º e ”  . AlSb ~ à Ì} Œ •_  þ j © œ8 £ x

`

 ¦ Sb – Ð = å Q ? /“ ¦ InAs ~ à Ì} Œ •`  ¦ $ í  © œ r ~  ´ M : In`  ¦ €  $  f  ¨

‚ Ã

Ì €   > €  \ " f In-Sb   ½ + Ës  Ò q tl >   ) a  . s  Qô  Ç   ½ + Ë

`

 ¦ s ê  r > €  `  ¦ “InSb-like” > €  s  “ ¦ ô  Ç . ¢ ¸ô  Ç AlSb

E-mail: [email protected]

~ Ã

Ì} Œ •_  Alõ  InAs ~ à Ì} Œ •_  Ass    ½ + Ë # Œ + þ A$ í  ) a Al-As

 

½ + Ë`  ¦ “AlAs-like” > €  s  “ ¦ ô  Ç . s  Qô  Ç ¿ º 7 á x À Ó_ 

>

€  “ É r InAs/AlSb € ª œ Ä ºÓ ü t ½ ¨› ¸\ " f „  l & h  : £ ¤$ í `  ¦   

&

ñ   H ×  æ כ ¹ô  Ç כ ¹™ è  ) a   [8]. AlAs-like > €  “ É r $ í  © œ r

 1 l x{ 9 ô  Ç “ : r • ¸\ " f ± ú “ É r ³ ð€   s 1 l x \  -t \  ¦ ° ú   H Al õ  Z

 }“ É r ³ ð€   s 1 l x \  -t \  ¦ ° ú   H As \  _ K  Al " é ¶    o \  As " é ¶   0 Au  >  ÷ &  H As antisite (AsAl) Ò q tl l 

~ 1

 . > €  \  + þ A$ í  ) a AsAl  H U  ·“ É r ï  r 0 A Å Ò> h (deep level donor) – Ð  Œ •6   x # Œ InAs_  î  r ì ø Í  0 l x • ¸\  ¦ 7 £ x  r v “ ¦ Å

Ò> h s “ : r \  _ K  î  r ì ø Í _  s 1 l x • ¸\  ¦ ± ú Æ ҍ  H í ß –ê ø Í " é ¶ “   s

  ) a   [8].   " f InAs/AlSb € ª œ Ä ºÓ ü t ½ ¨› ¸_  > €  \  AlAs-like > €   @ /’   InSb-like > €  `  ¦ + þ A$ í   H  כ s  Z  }

“ É

r „    s 1 l x • ¸\  ¦ ° ú   H € ª œ Ä ºÓ ü t`  ¦ $ í  © œ   H X < B Ä º ×  æ כ

¹ô  Ç כ ¹™ è  ) a   [9].

‘

: r ƒ  ½ ¨\ " f  H molecular beam epitaxy (MBE)Z O `  ¦ s  6

 

x # Œ InAs/AlSb € ª œ Ä ºÓ ü t ½ ¨› ¸\  ¦ GaAs l ó ø Í 0 A\  $ í



© œ % i Ü ¼ 9 InAs € ª œ Ä ºÓ ü t 0 A,  A  InSb-like > €   + þ A$ í

-555-

(2)

\

 @ /ô  Ç ½ ¨› ¸& h , „  l & h     o\  ¦ TEM õ  Hall ´ òõ  1 p x Ü ¼

–

Ð › ¸  % i  .

II. ÷ m Ç] M ö X ê sV  õ m Í U ê s0 n É

‘

: r ƒ  ½ ¨\   6   x ) a r « э  H — ¸¿ º MBE Z O Ü ¼– Ð ï  r q  

%

i  . l ó ø ÍÜ ¼– Ð ì ø Í „  \ P ^ ‰ (semi-insulating) GaAs(001) wafer\  ¦  6   x % i Ü ¼ 9 s “ : r* 3 á Ô\  ¦ s 6   x # Œ $ í  © œ ×  æ ”   /

B

N`  ¦ 1 × 10

−9

– Ð Ä »t  % i  . ¢ ¸ô  Ç As õ  Sb cell“ É r S X ‰ í

ß – (effusion)`  ¦ s 6   x % i  . GaAs l ó ø Í 0 A\  + þ A$ í  ) a í ß –



o} Œ •`  ¦ ] j  l  0 AK  $ í  © œz  ´\ " f 560

C – Ð 20ì  r ç ß – \ P 

%

ƒo  % i  . s M : GaAs l ó ø Í ³ ð€  \ " f As ì  r   \ P \  _

K  ì  r K ÷ &# Q ³ ð€  s  ’ < H  © œ÷ &  H  כ `  ¦ } Œ •l  0 AK  \ P % ƒo  1

l

x î ß – As cell`  ¦ \ P # Q As ì  r  \  ¦ > 5 Å q / B N/ å L % i  . í ß – o} Œ •

`

 ¦ ] j ô  Ç Ê ê l ó ø Í “ : r • ¸\  ¦ 540

C – Ð ± ú Æ Ò# Q GaAs ¢ - aØ  æ 8

£

x`  ¦ 0.7 µm/h _  $ í  © œÒ  ¦ – Ð 0.2 µm $ í  © œ % i  .

Fig. 1“ É r MBEZ O Ü ¼– Ð GaAs l ó ø Í 0 A\  $ í  © œ  ) a InAs/AlSb € ª œ Ä ºÓ ü t _  ½ ¨› ¸s  .      Ò& ñ ½ + Ës  €  • 8 %

“

  GaAs l ó ø Í 0 A\  InAs/AlSb € ª œ Ä ºÓ ü t ½ ¨› ¸\  ¦ $ í  © œ  l

 0 AK  AlSbü < GaSb ¢ - aØ  æ8 £ x`  ¦ y Œ •y Œ • 0.3 µm, 1.6 µm $ í



© œ % i  . ¢ ¸ô  Ç ³ ð€  _   } 9 l  x 9 ¾ º[ O  „  À Ó\  ¦ ± ú Æ Òl  0 A K

 GaSb ¢ - aØ  æ8 £ x 0 A\  AlSb (2 nm)/GaSb (2 nm) œ í  



 20Å Òl \  ¦ 500

C \ " f $ í  © œ % i  . InAs/AlSb € ª œ Ä º Ó

ü

t % i r  500

C \ " f $ í  © œ % i Ü ¼ 9 € ª œ Ä ºÓ ü t _  > €   $ í  © œ r

 Sbü < In_  f  ¨ ‚ Ã Ì r ç ß –`  ¦    or &  > €  _  : £ ¤$ í `  ¦ ² ú ˜o 

% i  . > €  $ í  © œ › ¸| \    É r ½ ¨› ¸& h  : £ ¤$ í “ É r reflection high-energy electron diffraction (RHEED), transmission electron microscopy (TEM) Ü ¼– Ð, „  l & h  : £ ¤$ í “ É r Hall ´ ò õ

 8 £ ¤& ñ Ü ¼– Ð › ¸  % i  .

III. ÷ m Ç] M ö+ s ÇÊ Ý õ m Í ‚ º8 ý

Fig. 2  H InSb-like > €  `  ¦ $ í  © œ l  0 Aô  Ç $ í  © œ ½ ¨› ¸ü <

3

9'   Œ •1 l x Y V (shutter sequence) s  . InAs/AlSb € ª œ



Ä ºÓ ü t \ " f InSb-like (Fig. 2(a)) > €  `  ¦ + þ A$ í   H  כ “ É r

“

¦5 Å q „  5 Å x : £ ¤$ í `  ¦ % 3   H X < ×  æ כ ¹ô  Ç כ ¹™ èe ” `  ¦ · ú ¡" f [ O " î 

%

i  .   " f Fig. 2(a)ü < ° ú  s  > €  \ " f In " é ¶  ü < Sb " é ¶



_    ½ + Ë`  ¦ ½ ©g Ë :& h Ü ¼– Ð + þ A$ í l  0 AK  Fig. 2(b)ü < ° ú  

“ É

r 3 9'  1 l x  Œ •s  € 9 כ ¹  . Fig. 2(b)\ " f  A A á ¤ > €  _  t

Sb

  H AlSb _  ³ ð€  `  ¦ Sb 8 £ x Ü ¼– Ð + þ A$ í l  0 Aô  Ç Sb f  ¨ ‚ Ã Ì r

ç ß –`  ¦ _ p   9 t

In

“ É r Sb ³ ð€  \  In`  ¦ f  ¨ ‚ à Ìr v   H r  ç

ß –`  ¦ _ p ô  Ç . ¢ ¸ô  Ç 0 AA á ¤ > €  _  t

In

  H InAs ³ ð€  `  ¦ In 8

£

x Ü ¼– Ð + þ A$ í l  0 Aô  Ç In f  ¨ ‚ à Ìr ç ß –s “ ¦ t

Sb

  H In ³ ð€  \  Sb\  ¦ f  ¨ ‚ à Ìr v   H r ç ß –s  .

Fig. 1. InAs/AlSb quantum well structure on GaAs sub- strate.

Fig. 2. Interface structures for (a) InSb-like interface and (b) shutter sequencing with InSb-like interface on top and bottom.

Fig. 3“ É r InAs G V ,   © œ8 £ x  Ò\ " f Sb f  ¨ ‚ à Ì\  _ K  InSb- like > €  s  ë ß –[ þ t # Qt   H õ & ñ `  ¦    · p  כ s   [10]. €  

$

 Fig. 3(b)ü < ° ú  s  InAs ³ ð€  \  Sb\  ¦ f  ¨ ‚ à Ìr v €   Asõ 

Sb   o  À D K`  ¦ K " f InSb   ½ + Ë`  ¦ + þ A$ í >   ) a  . Sb\  ¦

(3)

Fig. 3. (a)-(d) schematic diagram of inSb-like interface on InAs surface (top interface). RHEED pattern of (e) InAs and (f) InSb layer.

>

5 Å q f  ¨ ‚ Ã Ì €   Fig 3(d)ü < ° ú  s  InSb   ½ + Ës  ç  H{ 9  >  + þ A

$ í

 ) a  . s  Qô  Ç   õ   H RHEED ³ ð€   ì  r$ 3    õ – Ð S X ‰ “  

½

+ É Ã º e ”  . Fig. 3(e)ü < (f)  H InSb-like > €   $ í  © œ „  , Ê ê _

 RHEED ½ ¨› ¸– Ð" f Fig. 3(e)  H InAs ³ ð€  `  ¦   ? /  H (2 × 1) ½ ¨› ¸s “ ¦ Fig. 3(f)  H InSb ³ ð€  `  ¦   ? /  H (1

× 3) ½ ¨› ¸s  .   " f Sb f  ¨ ‚ Ã Ì Ê ê InAs ³ ð€  \  InSb 8 £ x s

 + þ A$ í ÷ &% 3    H  כ `  ¦ · ú ˜ à º e ”  . s  כ “ É r InAs G V ,  0 A A

á

¤ > €  $ í  © œ r  Sb f  ¨ ‚ à Ìë ß –Ü ¼– Е ¸ InAs ³ ð€  \  InSb-like

>

€  `  ¦ + þ A$ í r ~  ´ à º e ”    H  כ `  ¦ _ p   9 ‘ : r ƒ  ½ ¨\ " f



 H InAs G V ,   © œ8 £ x  Ò_  InSb-like > €   + þ A$ í r  In f  ¨ ‚ à Ìr  ç

ß –õ  Sb f  ¨ ‚ Ã Ì r ç ß –`  ¦ 0 œ í x 9 15œ í– Ð y Œ •y Œ • “ ¦& ñ % i  .

#

Œl " f Sb f  ¨ ‚ Ã Ì 15œ í  H z  ´+ « >`  ¦ : Ÿ x K  þ j& h  o % i  .

Fig. 4  H InAs G V ,   A _  In f  ¨ ‚ à Ìr ç ß –õ  Sb f  ¨ ‚ à Ìr  ç

ß –    o\    É r „    s 1 l x • ¸ x 9 0 l x • ¸\  ¦    · p Õ ªA á Ô s

 . s M : In f  ¨ ‚ à Ìr ç ß –õ  InAs G V , _  ¿ ºa   H y Œ •y Œ • 1œ í ü

< 15 nm– Ð : Ÿ x{ 9  % i  . Fig. 4(a)\ " f ˜ Ѝ  H  ü < ° ú  s  Sb\  ¦ f  ¨ ‚ Ã Ì t  · ú §“ É r  â Ä º „    s 1 l x • ¸ 8,067 cm

2

/V·s

–

Ð  © œ ± ú € Œ ¤Ü ¼ 9 0 l x • ¸  H 5.78 × 10

12

cm

−2

– Ð  © œ Z  }

€

Œ

¤ . s  כ “ É r > €  \  InSb 8 £ x s  ç  H{ 9  >  + þ A$ í ÷ &t  3 l w 

“

¦ AlAs < ʓ É r AlSbAs8 £ x 1 p x s  + þ A$ í ÷ &# Q   + þ Aõ  U  ·“ É r   

†

< Ê`  ¦ + þ A$ í , „   _  0 l x • ¸\  ¦ Z  } s “ ¦ s 1 l x • ¸\  ¦ ± ú Æ ҍ  H כ ¹“   Ü

¼– Ð # Œ ”   . t ë ß – Sb\  ¦ 15 œ í s  © œ f  ¨ ‚ Ã Ì   H  â Ä º

„

   s 1 l x • ¸ü < 0 l x • ¸ ° ú כ“ É r y Œ • y Œ • 12,000 ∼ 13,000 cm

2

V·s ü

< 1.0 × 10

12

∼ 2.0 × 10

12

cm

−2

 s _  ° ú כ`  ¦ & ’ Ü ¼ 9 f

 ¨ ‚ à Ìr ç ß –s  45œ í s  © œÜ ¼– Ð U  ´# Q4 R• ¸ „    s 1 l x • ¸ü < 0 l x

•

¸  H  8 s  © œ    t  · ú §“ ¦ Ä »t  ÷ &  H  ⠆ ¾ Ó`  ¦ ˜ Ð% i  . s 

 כ

“ É r Sb  1 monolayer (ML) f  ¨ ‚ Ã Ì  ) a Ê ê\   H l ó ø Í³ ð€  _ 

Fig. 4. Electron mobility and sheet carrier concentration at 300 K in dependence of the bottom (a) Sb and (b) In soaking time.

\ P

\  -t \  _ K  ~ 1 >  ì  r K ÷ &  H Sb-Sb   ½ + Ës  ³ ð€  \  + þ A

$ í

÷ &# Q  8 s  © œ f  ¨ ‚ à Ì÷ &t  · ú §l  M :ë  H Ü ¼– Ð # Œ ”   .   

"

f Sb f  ¨ ‚ à Ìr ç ß –`  ¦ Z þ t # Œ• ¸ „    s 1 l x • ¸ü < 0 l x • ¸ Ä »t ÷ &



 H  ⠆ ¾ Ó`  ¦ ˜ Ðs >   ) a  . Fig 4(b)  H  A A á ¤ > €  \ " f Sb f

 ¨ ‚ Ã Ì Ê ê In f  ¨ ‚ à Ìr ç ß –\    É r „    s 1 l x • ¸ü < 0 l x • ¸\  ¦   



· p Õ ªA á Ôs  . s M :  A A á ¤ > €  _  t

Sb

“ É r 30 œ í– Ð ½ ©  



o % i “ ¦ InAs G V , _  ¿ ºa  % i r  15 nm– Ð : Ÿ x{ 9  % i  .

Fig. 4(b) \ " f    1 p w s  In f  ¨ ‚ à Ìr ç ß –s  3œ í“    â Ä º\ 

„

  s 1 l x • ¸ €  • 18,000 cm

2

/V·s – Ð þ j@ /° ú כ`  ¦ ˜ Ðs  

7 œ í\   H „   s 1 l x • ¸  r  ± ú  ”   . „   _  0 l x • ¸ % i r  In f  ¨ ‚ à Ìr ç ß –s  3œ í { 9  M : 1.2 × 10

12

cm

−2

– Ð  © œ ± ú “ É r

° ú

כ`  ¦ ˜ Ð% i  .

Fig. 5  H In f  ¨ ‚ à Ìr ç ß –\    É r > €  _  : £ ¤$ í `  ¦ TEM Ü ¼

–

Ð 8 £ ¤& ñ ô  Ç é ß –€    ”  s  .   õ \     1 p w s  In f  ¨ ‚ à Ìr  ç

ß –s  3œ í“    â Ä º > €  s   © œ L :  F M >  + þ A$ í ÷ &% 3 Ü ¼ 9 f  ¨

‚ Ã

Ì r ç ß –s  U  ´# Q| 9 à º2 Ÿ ¤ & h & h  > €  s   } 9 # Qt   H ^  ¦ à º e ” 



. s ü < ° ú  “ É r s Ä »  H In f  ¨ ‚ à Ìr ç ß –s  U  ´# Q| 9 à º2 Ÿ ¤ F K5 Å q$ í _

 In " é ¶  [ þ t s  Ó ü æ u >  ÷ &# Q > €   : £ ¤$ í s    t l  M :ë  H s

 9 TEM   õ \  ¦ : Ÿ x K " f s \  ¦ S X ‰ “  ½ + É Ã º e ”  .

Fig. 6(a)  H InAs G V ,  ¿ ºa    oü <  A A á ¤ > €  _  In f

 ¨ ‚ à Ìr ç ß –\    É r „   _  s 1 l x • ¸ü < 0 l x • ¸\  ¦    · p Õ ªA 

(4)

Fig. 5. Cross-sectional TEM images of InAs/AlSb quan- tum well in dependence of the bottom In soaking time.

Sb soaking times are 30 sec. In soaking times are (a) 1 sec, (b) 3 sec, (c) 5 sec, and (d) 7 sec.

á

Ôs  . InAs G V , _  ¿ ºa  15 nm\ " f 30 nm– Ð ¿ º  0

>f ” \     „   _  s 1 l x • ¸ Z  }  & ’ Ü ¼ 9 In f  ¨ ‚ à Ìr ç ß –

\

   É r    o  H InAs _  ¿ ºa ü <  © œ › ' a \ O s  Ä » ô  Ç  ⠆ ¾ Ó

`

 ¦ ˜ Ð% i  . s  כ “ É r InAs G V , _  ¿ ºa  ¿ º 0 >f ” \   



 > €  \ " f µ 1 ÏÒ q t÷ &  H î  r ì ø Í _  í ß –ê ø Í % ò † ¾ Ós  ×  ¦ # Q[ þ t l  M

:ë  H s  . Fig. 6(a)\    Í Ç x1 p w s  InAs G V , _  ¿ ºa 

30  s “ ¦ In f  ¨ ‚ à Ìr ç ß –s  3œ í{ 9  M : „    s 1 l x • ¸ 20,700 cm

2

/V·s Ü ¼– Ð þ j@ /° ú כ`  ¦   ? /% 3  .

Fig. 6(b)-(c)  H 0 A,  A  > €  7 á x À Ó\    É r “ : r • ¸ _ ” > r

$ í

(10 k ∼ 300 k) Hall ´ òõ  8 £ ¤& ñ   õ s  . Fig. 6(b)- (c) \ " f  Ž “ É rÒ  o " é ¶ s  z  ´‚  Ü ¼– Ð ƒ     ) a Õ ªA á ԍ  H · ú ¡" f

„

   s 1 l x • ¸ þ j@ /– Ð 8 £ ¤& ñ  ) a r « Ñ_  “ : r • ¸_ ” > r$ í 8 £ ¤& ñ

 

õ s  . Fig. 6(b)\ " f ˜ Ѝ  H  ü < ° ú  s  8 £ ¤& ñ “ : r • ¸

± ú

 f ” \     „   s 1 l x • ¸ Z  }  4 R 10 k \ " f 65,860 cm

2

/V·s  t  7 £ x  % i  . 8 £ ¤& ñ “ : r • ¸ ± ú  f ” \     „  



 s 1 l x • ¸ 7 £ x    H  כ “ É r Å Ò> h s “ : r \  _ ô  Ç î  r ì ø Í _  í

ß –ê ø Ís  \ O    H  כ `  ¦ _ p   9   " f InAs/AlSb € ª œ Ä º Ó

ü

t \ " f InSb-like > €  s  ¸ ú ˜ + þ A$ í ÷ &% 3    H  כ `  ¦ _ p ô  Ç



. G. Tuttle et al [3]\  _ K  ˜ Г ¦  ) a   õ   H 10 k \ " f 121,000 cm

2

/V·s _  Z  }“ É r ° ú כ`  ¦ ˜ Ð% i   H X < ‘ : r ƒ  ½ ¨\ " f  H InAs ü < AlSb_  ¿ ºa  þ j& h  o÷ &t  · ú §  ± ú “ É r ° ú כ`  ¦ ˜ Г  

 כ

Ü ¼– Ð ó ø Íé ß –  ) a  . Fig. 6(b)-(c)\ " f š ¸˜ É r  ) a " é ¶ õ   rÒ  o

"

é

¶ Ü ¼– Ð    · p Õ ªA á ԍ  H G. Tuttle et al. \ " f ˜ Г ¦  ) a  

«

і Ð" f y Œ •y Œ •  A A á ¤ > €  \  AlAs-like > €  s  + þ A$ í  ) a  â Ä

ºü < 0 A,  A A á ¤ — ¸¿ º AlAs-like > €  s  + þ A$ í  ) a  â Ä º_  “ : r

•

¸_ ” > r$ í f . Ë 8 £ ¤& ñ   õ s  9 8 £ ¤& ñ “ : r • ¸ ± ú  f ” \ • ¸ „  



 s 1 l x • ¸_     o  _  \ O    H  כ `  ¦ ^  ¦ à º e ”  . ¢ ¸ô  Ç

Fig. 6. (a) Electron mobility and sheet carrier concentra- tion at 300 K in dependence of the InAs channel thick- ness. Comparison of (b) mobility and (c) sheet carrier concentration for quantum wells utilizing the three com- binations of InSb-like and AlAs-like interface.

Fig. 6(c) \ " f ^  ¦ à º e ” 1 p w s  „   _  0 l x • ¸ % i r  0 A,  A  A

á

¤ > €  \  InSb-like > €  s  + þ A$ í ÷ &% 3 `  ¦ M :\   H  © œ“ : r \ 

"

f_  „    0 l x • ¸ 1.7 × 10

12

cm

−2

Ü ¼– Ð AlAs-like > €   s

 + þ A$ í ÷ &% 3 `  ¦ M : ˜ Ð  ± ú Ü ¼ 9 8 £ ¤& ñ “ : r • ¸ ± ú  f ” \   



 ‚  + þ A& h Ü ¼– Ð 0 l x • ¸ ± ú  ”   . t ë ß – AlAs-like > €   s

 + þ A$ í  ) a  â Ä º\   H €  • 100 k ü < 250 k \ " f Å Ò> h_  1 l x

 

 (freeze-out) ‰ & ³ © œs       H  כ `  ¦ ^  ¦ à º e ” Ü ¼ 9 s   H AlAs-like > €  s  Å Ò> h\  ¦ + þ A$ í # Œ î  r ì ø Í  í ß –ê ø Í_  " é ¶ “   s

  ) a    H  כ `  ¦ _ p ô  Ç .

(5)

IV. + s Ç Â ] Ø

MBE Z O Ü ¼– Ð GaAs l ó ø Í 0 A\  InAs/AlSb € ª œ Ä ºÓ ü t

`

 ¦ $ í  © œr &  InAs> €   $ í  © œ › ¸| \    É r : £ ¤$ í `  ¦ TEM õ

 Hall ´ òõ  8 £ ¤& ñ Ü ¼– Ð › ¸  % i  .

InAs/AlSb € ª œ Ä ºÓ ü t ½ ¨› ¸_  > €  \ " f Sbü < In_  f  ¨ ‚ Ã Ì r

ç ß –`  ¦    or &  InSb-like > €  `  ¦ + þ A$ í % i  . InAs G  V ,

_  0 AA á ¤ > €  \ " f  H Sb f  ¨ ‚ à Ìë ß –Ü ¼– Е ¸ InSb-like > €  s  + þ

A$ í ÷ &% 3  .  A A á ¤ > €  \ " f  H Sb f  ¨ ‚ à Ì_   â Ä º\  15œ í s

 © œ f  ¨ ‚ à Ì÷ &€    8 s  © œ > €   : £ ¤$ í s     o t  · ú §€ Œ ¤ .

t ë ß – In f  ¨ ‚ Ã Ì r ç ß –    o\     î  r ì ø Í _  s 1 l x • ¸ü <

>

€   : £ ¤$ í s  / å L   >     o % i Ü ¼ 9 InAs Ä ºÓ ü t _  ¿ ºa 

\

 ¦ 15 nm \ " f 30 nm– Ð 7 £ x r (  `  ¦ M :  © œ“ : r \ " f 20,700 cm

2

/V·s _  „   s 1 l x • ¸\  ¦ % 3 % 3 `  ¦ à º e ” % 3  . ¢ ¸ô  Ç “ : r • ¸ _

” > r$ í Hall´ òõ  8 £ ¤& ñ `  ¦ : Ÿ x # Œ > €  \  InSb-like > €  s  + þ

A$ í ÷ &# Q s “ : r  o Å Ò> h\  _ ô  Ç í ß –ê ø Ís  µ 1 ÏÒ q t t  · ú §  H  



 H  כ `  ¦ S X ‰ “   % i  .

P

c p 8 ý ò k >

‘

: r ƒ  ½ ¨  H ô  Dz D G † < ÆÕ ü t F é ß – ‚  • ¸õ ] j (KRF-2004-041- D00433) ü < õ † < ÆF é ß – : £ ¤& ñ l œ í (R01-2006-000-10874- 0) t " é ¶ \  _ K  ”  ' Ÿ ÷ &% 3 6 £ §.

Y

c p w Š à U Ø ”  ô

[1] A. Nakagawa, H. Kroemer and J. H. English, Appl.

Phys. Lett. 54, 1893 (1989).

[2] L. F. Luo, R. Beresford, W. I. Wang and H.

Munekata, Appl. Phys. Lett. 55, 789 (1989).

[3] J. Werking, G. Tuttle, C.Nguyen, E. L. Hu and H.

Kroemer, Appl. Phys. Lett. 57, 905 (1990).

[4] K. Yoh, T. Moriuchi and M. Inoue, Jpn. J. Appl.

Phys. Part 2 29, L2455 (1990).

[5] J. B. Boss, W. Kruppa, B. V. Shanabrook, D. Park, J. L. Davis and H. B. Dietrich, Electron. Lett. 29, 1888 (1993).

[6] C. R. Bolignesi, E. J. Canine and H. Kroemer, IEEE Electron Device Lett. 15, 16 (1994).

[7] G. Tuttle and H. Kroemer, IEEE Trans. Electron Device ED-34, 2358 (1987).

[8] G. Tuttle, H. Kroemer and J. H. English, J. Appl.

Phys. 67, 3032 (1990).

[9] J. Shen, H. Goronkin, J. D. Dow and S. Y. Ren. J.

Appl. Phys. 77, 1576 (1995).

[10] Takeshi Miura, Takanori Nakai and Koichi Yam-

aguchi, Appl. Surf. Sci. 237, 242 (2004).

(6)

Electrical Properties of the InSb-like Interface in an AlSb/InAs/AlSb Quantum Well

Y. K. Noh and M. D. Kim

Department of Physics, Chungnam National University, Daejeon 305-764

J. E. Oh

Division of Electrical and Computer Engineering, Hanyang University, Ansan 426-791

Y. H. Kim

Korea Research Institute of Standards And Science, Daejeon 305-340

S. G. Kim

Department of Information and Communications, Joongbu University, Gumsan-gun 132-940

H. S. Im

Department of Semiconductor Science, Dongguk University, Seoul 100-715 (Received 28 March 2007)

We researched the electrical and the structural properties of the InSb-like top and bottom in- terfaces of an InAs layer in an AlSb/InAs/AlSb quantum-well structure grown on a GaAs (001) substrate by using molecular beam epitaxy. We investigated these properties by using reflection high-energy electron diffraction, transmission election microscopy, and Hall effect measurements.

We obtained an electron mobility of 20,700 cm

2

/V·s at room temperature by using a combina- tion of a 30-nm InAs well and InSb-like top and bottom interfaces. In addition, according to the measurement of the temperature dependence, the InAs well interface formed an InSb-like layer.

PACS numbers: 73.61.Ey, 73.63.Hs, 81.15.Hi

Keywords: InAs, AlSb, Interface, TEM, Hall effect, Mobility

E-mail: [email protected]

수치

Fig. 2. Interface structures for (a) InSb-like interface and (b) shutter sequencing with InSb-like interface on top and bottom.
Fig. 4. Electron mobility and sheet carrier concentration at 300 K in dependence of the bottom (a) Sb and (b) In soaking time
Fig. 6. (a) Electron mobility and sheet carrier concentra- concentra-tion at 300 K in dependence of the InAs channel  thick-ness

참조

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