Ç
U ØT Ì ¦ R ¹ Å 4 8 ý ° Ë Ñ ¹ Åy ¢y ¢; c 6 X ¢ ° Ë ÑV R Ë ºÀ X Ø8 ý W _ Ë] §
~ ç
¡ ó j u ∗
x 9
ª @ / < Æ § § ª õ & ñ Â Ò, x 9 ª 627-702 (2005¸ 9 Z 4 30{ 9 ~ Ã Î6 £ §, 2006¸ 1 Z 4 2{ 9 þ j7 á x : r ~ Ã Î6 £ §)
ª : x > % i < Æ& h í ß @ /Ã º~ ½ ÓZ O ` ¦ 6 x # F g$ í í 7 H õ © ñ 6 x H ï r s " é ¶ > _ F g
¸ ¸\ ¦ Ä » ¸Ù þ ¡ . õ \ H ü < í 7 H _ ì r í < Êà º & h ] X y í < Ê÷ &# Q e # Q" f í 7 H` ¦ f ¨ à º
¢
¸ H ~ ½ ÓØ ¦ " f s H õ & ñ ` ¦ K $ 3 l ¼ # o < Ê` ¦ · ú Ã º e % 3 . ¢ ¸, Ã ºu > í ß _ õ \ _
, Ä ºÓ ü t ¿ ºa 7 £ x ì ø Í; ¤ u y è ¦ : r ¸ ` ¦ ì ø Í; ¤ u 7 £ x H כ Ü ¼ Ð z ¤ .
PACS numbers: 72.20.-i, 72.10.Di Keywords: l ¸ ¸, í 7 H í ß ê ø Í
I. " e  ] Ø
þ
j H \ ì ø Í ¸^ ] j ¸l Õ ü t _ µ 1 Ï Ü ¼ Ð K ¸ß ¼l _
$
" é ¶ ì ø Í ¸^ _ ] j s 0 p x > ÷ &% 3 . s $ " é ¶
>
_ : £ ¤$ í ` ¦ ¸ H ~ ½ ÓZ O × æ s [ þ t > ? /_
[ þ t _ à º5 Å x & ³ © \ % ò ¾ Ó` ¦ p u H í 7 H s Ô ¦í HÓ ü t 1 p x
\
_ ô Ç í ß ê ø Í´ òõ \ ¦ ½ ¨ H כ s . s ü < ' aº ) a ½ ¨
×
æ + þ A6 £ x ² ú s : r s [1-11]. ª : x > % i < Æ& h ~ ½ Ó Z O
` ¦ & h 6 x # % ò í ß ~ ½ ÓZ O [2-11]` ¦ 6 x + þ A 6
£
x ² ú s : r \ _ K Å Ò# Qt H l ¸ ¸\ ¦ ª ô Ç + þ AI Ð
½
¨½ + É Ã º e . s ~ ½ ÓZ O ` ¦ & h 6 x % ò í ß \ ¦ & ñ _
H ~ ½ ÓZ O \ ¸ ¸\ ¦ ª > > h½ + É Ã º e .
õ
\ H % ò í ß \ ¦ 6 x # l ¸ ¸\ ¦ > í ß ½ + É M
: Å Ò Ð é ß { 9 ³ ð & ³Ü ¼ Ð > í ß Ù þ ¡Ü ¼ [2-6], ^
% ò
í ß ~ ½ ÓZ O Ü ¼ Ð > í ß H כ s Ó ü t o & h Ü ¼ Ð K $ 3 l
¼ # o ¦ · ú 94 R e [7-11]. ¢ ¸ô Ç, © I 1 l qw n
% ò
í ß (state-independent projection operator) ~ ½ ÓZ O
É
r s 9 þ t Ðà Ô : r / B N" î õ ° ú É r \ -t ç ß s { 9 & ñ ô Ç â Ä
º\ ô Ç # & h 6 x ½ + É Ã º e H ì ø Í \ , © I _ > r % ò í ß
(state-dependent projection operator) ~ ½ ÓZ O É r \ -t ï
r 0 A s _ ç ß s { 9 & ñ t · ú § ¸ & h 6 x s 0 p x ¦
· ú
94 R e [10, 11].
: r 7 Hë H \ " f H © I 1 l qw n % ò í ß ~ ½ ÓZ O ` ¦ & h 6 x # ï
r s " é ¶ > _ F g ¸ ¸\ F g$ í í 7 H s p u H % ò ¾ Ó
`
¦ ª : x > % i < Æ& h ~ ½ ÓZ O Ü ¼ Ð > í ß ô Ç .
∗
E-mail: [email protected]
II. X N Ë M X ê s ; c" e8 ý Ç U Ø T Ì ¦ R ¹ Å 4
&
ñ l © B = Bˆz K | 9 M : ï r s " é ¶ > _ K x 9
Ðm î ß É r 7 ' ( J $ [ > ` ¦ A = (0, Bx, 0) Ð × þ H e = (p+eA) 2m
2+ U (z)
= 2m 1 P
i=x,y,z p 2 i + ω c x ~ i ∂y ∂ + 1 2 mω 2 c x 2 + U (z) (1) s
. # l " f m É r _ Ä »´ ò| 9 | ¾ Ós ¦ p H _ î r 1
l
x | ¾ Ós 9 ω c = eB/m H s 9 þ t Ðà Ô : r 1 l x à º\ ¦ · p
. ï r s " é ¶ > _ ½ ¨5 Å q ( J $ [ > U (z) H > _ ß ¼l ´ ò õ
\ ¦ ¦ 9½ + É Ã º e ¸2 ¤ ¿ ºa L z Á ºô Ç y Ä ºÓ ü t` ¦ × þ ô
Ç .
d
(1)_ ¦Ä » < Êà º Ð
Ψ(x, y, z) = s 2
L y L z exp(ik y y)Φ(x) sin(k z z) (2)
\
¦ × þ ô Ç . L y H > _ y~ ½ Ó ¾ Ó_ ß ¼l s ¦ Ã º 7 ' k\
@
/K " f k z = nπL z s 9 n É r ª à ºs . d (1)` ¦ d (2) \ & h 6 x \ -t ¦Ä »u E\ @ /K " f
H e Ψ(x, y, z) = EΨ(x, y, z)
= ~ 2 k y 2
2m + ~ 2 k z 2 2m − ~ 2
2m
∂ 2
∂x 2 + 1
2 mω 2 c x 2 + ω c x~k y
Ψ(x, y, z) (3) s
÷ & ¦, x 1 = x + ~k y /eB Ð ¿ º 1
2 mω c 2 x 2 1 = 1
2 mω c 2 x 2 + ~ 2 k y 2
2m + ω c x~k y (4)
-125-
s
. " f d (2)-(4)\ ¦ 6 x (− 2m ~
2∂x ∂
221
+ 1 2 mω c 2 x 2 1 )Φ(x)
= (E − ~ 2m
2k
z2)Φ(x) ≡ E 1 Φ(x 1 ) (5)
\
¦ % 3 ` ¦ à º e . 0 A d É r ¸ o 1 l x _ ¦Ä »u ~ ½ Ó& ñ d Ü
¼ Ð Õ ª K H ¸ ú · ú 94 R e . " f d (1)_ ¦Ä »u ü <
¦Ä » < Êà º H 6 £ § õ ° ú .
E N,n = E N + n = (N + 1/2)~ω c + n 2 0 (6) N = 0, 1, 2, · · · , n = 1, 2, 3, · · ·
Ψ N,n,k
y(x, y, z)
= q 2
L
yL
zexp(ik y y)Φ N (x − x 0 ) sin(k z z) (7) Φ N (x − x 0 ) = 1
( √ π2
NN !l
c)
1/2× exp
− (x−x 2l
20)
2c
H N
x−x
0l
c(8)
#
l " f N É r & ñ l © \ _ K " f ì r o ) a © I \ ¦ ? /
H Landau t à º, n É r ½ ¨5 Å q ( J $ [ > \ _ K " f ì r o ) a © I
\
¦ ? / H t à ºs . H N H N − Hermite ½ Ód s
¦ 0 = ~ 2 π 2 /2mL 2 z , x 0 = −~k y /eB, l 2 c = ~/eBs . d (6) \ " f · ú Ã º e 1 p w s _ \ -t H x-y ~ ½ Ó ¾ ÓÜ ¼ Ð H
&
ñ l © \ _ K " f ª o÷ & ¦ z ~ ½ Ó ¾ ÓÜ ¼ Ð H ½ ¨5 Å q ( J $ [ >
\ _ K ª o ) a . ] j III] X \ " f H 0 Aü < ° ú É r > _
l ¸ ¸\ ¦ í 7 H õ _ © ñ 6 x s e H â Ä º\ @ /K " f
½
¨ô Ç .
III. ¹ ÅM ¹ Åy ¢y ¢8 ý ] k ùÅ k ÄX ì Äß Ã Å A 0
ü
@ Ò\ " f y 1 l x à º ω Ð 1 l x H l © E(t) = Ee iωt K | 9 M : l ¸ ¸ J $ " f H + þ A6 £ x ² ú s : r \ _
K [7-9]
σ xx (¯ ω) = −e lim
s→0
+X
α,β
X
γ,δ
(x) αβ (j x ) γδ A αβ (¯ ω) (9)
Ð Å Ò# Q . # l " f
A αβ (¯ ω) = T R {ρ eq [(~¯ ω − L eq ) −1 a † γ a δ , a † α a β ]} (10) s
. ¯ ω ≡ ω + is(s → 0 + ) s ¦ x H _ 0 Au 7 ' _ x$ í ì r, j x = (ie~/m)∂/∂x H é ß { 9 _ À Óx 9 ¸ í ß
, (x) αβ ≡< α|x|β > s ¦ L eq H e _ _ í ß X\ @ / K
L eq X = [H eq , X] Ð & ñ _ ÷ & H H eq \ @ /6 £ x H o Ä ºq
í ß s . a † α (a α ) H \ -t E α |α > © I \ " f_
_ Ò q t$ í ( èY > ) í ß s .
d
(10)` ¦ > í ß l 0 AK % ò í ß \ ¦ 6 £ § õ ° ú s
&
ñ _ ô Ç .
P X ≡ <X>
<a
†γa
δ> a † γ a δ (11) Q ≡ 1 − P (12)
#
l " f
< X >≡ T R {ρ eq [X, a † α a β ]} (13) s
. ρ eq H ¨ î + þ Aì r í_ x 9 ¸, T R H ^ traces .
% ò
í ß _ & ñ _ ÐÂ Ò' 1 = (P + Q)s Ù ¼ Ð d (10)\ " f L eq · 1 = L eq (P + Q) Ð Ë ¨ ¦ ½ Ó1 p xd
(A − B) −1 = A −1 + A −1 B(A − B) −1 (14)
`
¦ 6 x # > h
1
~ ¯ ω−L
eqa † γ a δ = 1
~ ¯ ω a † γ a δ + 1
~ ¯ ω−L
eqQ L eq a † γ a δ A
αβ<a
†γa
δ> (15) s
) a . # l " f Qa † γ a δ = 0` ¦ 6 xÙ þ ¡ . s ] j L eq = L d + L v Ð ì r o ¦ (L d ü < L v H y y @ /y K x 9 Ðm î ß H d ü < © ñ 6 x ½ Ó V \ @ /6 £ x H o Ä ºq í ß )
L d a † γ a δ = (E γ − E δ )a † γ a δ ≡ E γδ a † γ a δ (16)
\
¦ 6 x
A αβ (¯ ω) = <a
† γ
a
δ>
~ ¯ ω−E
γδ−B
αβ( ¯ ω) (17) B αβ (¯ ω) =< (~¯ ω − L eq Q) −1 L v a † γ a δ > ~ ¯ ω
<a
†γa
δ> (18) s
) a . E γ H © I |γ >≡ |N, n >_ \ -t s . # l
\
< a † γ a δ >= T R {ρ eq [a † γ a δ , a † α a β ]}
= (f β − f α )δ βγ δ αδ (19)
\
¦ ¦ 9 ¦ d (17)` ¦ d (9)\ @ /{ 9 6 £ §` ¦ % 3 H
.
σ xx (¯ ω) = −e lim s→0
+P
αβ (x) αβ (j x ) βα
× f
β−f
α~ ¯ ω−E
βα−Γ
αβ( ¯ ω) . (20)
#
l " f f α H |α > © I _ _ ` Ø Ôp -n Ï þ _ ì r í < Ê Ã
ºs ¦
Γ αβ (s) = T R {ρ eq
(~¯ ω − L eq Q) −1
× L v a † β a α , a † α a β
} f ~ ¯ ω
β
−f
α(21)
s
. # l \ ½ Ó1 p xd
T R {ρ eq [L eq QX, a † α a β ]} = T R {ρ eq [L v a † α a β , X]}
−T R {ρ eq [L v P X, a † α a β ]} (22)
\
¦ ¦ 9 # [s כ É r T R (ABC) = T R (BCA) ü < H eq H ρ eq ü < § ¨ 8 0 p x < Ê` ¦ s 6 x ~ 1 > Ä » ¸ ) a ] X ≡ (~¯ ω−
L eq Q) −1 L v a † β a α Ð ¿ º
Γ αβ (¯ ω) = −T R {ρ eq [L v a † α a β , (~¯ ω − L d ) −1 L v a † β a α ]} 1
f β − f α (23) s
) a . # l " f © ñ 6 x _ [ jl ¦ & ñ # L v ( ¢ ¸ H V ) _ ] jY L ½ Ó t ë ß ¦ 9Ù þ ¡ . d (23) É r V ( ¢ ¸
H L v ) ½ ¨^ & h Ü ¼ Ð Å Ò# Qt > í ß s 0 p x ô Ç + þ AI s .
]
j IV ] X \ " f H s כ ` ¦ - í 7 H > \ @ /K " f ½ ¨ô Ç .
IV. ¹ Å - ºÀ X Ø4 8 ý ¹ ÅM ¹ Åy ¢y ¢
_ Ã º5 Å x & ³ © \ í 7 H s ' a # H â Ä º, ¨ î + þ A © I
\
" f_ K x 9 Ðm î ß H eq H 6 £ § õ ° ú s _ K x 9 Ðm î
ß (H e ) ü < í 7 H _ K x 9 Ðm î ß (H p ), ü < í 7 H _ © ñ
6 x(V ) Ü ¼ Ð s À Ò# Q .
H eq = H e + H p + V
= P
α E α a † α a α + P
q ~ω q b † q b q + V (24) V = P
q
P
α,µ C α,µ (q)a † α a µ (b q + b † −q ) (25)
#
l " f E α H d (6)\ Å Ò# Q _ \ -t s ¦ b † q (b q ) H \ -t ~ω q |q > © I _ í 7 H _ Ò q t$ í ( èY > )
í ß s 9, ω q H à º 7 ' q í 7 H _ y 1 l x à ºs .
í 7 H _ à º 7 ' qü < ì rF G t à º s\ @ /K " f q = (q, s) Ð
&
ñ _ ÷ & ¦ C α,µ ≡< α|C(q)|µ > H ü < í 7 H _ © ñ 6
x í ß C(q)_ ' § > =כ ¹ è\ ¦ · p .
d
(24)ü < (25)\ ¦ 6 x # d (23)` ¦ > í ß 6 £ § õ
° ú .
Γ αβ (¯ ω)(f β − f α ) = P
q
P
γ |C βγ (q)| 2
(1+N
q)f
α(1−f
γ)
~ ¯ ω−E
γα−~ω
q− N
qf
γ(1−f
α)
~ ¯ ω−E
γα−~ω
q+ N
qf
α(1−f
γ)
~ ¯ ω−E
γα+~ω
q− (1+N
q)f
γ(1−f
α)
~ ¯ ω−E
γα+~ω
q+ P
q
P
γ |C αγ (q)| 2
×
(1+N
q)f
γ(1−f
β)
~ ¯ ω−E
βγ−~ω
q− N
qf
β(1−f
γ)
~ ¯ ω−E
βγ−~ω
q+ N
qf
γ(1−f
β)
~ ¯ ω−E
βγ+~ω
q− (1+N
q)f
β(1−f
γ)
~ ¯ ω−E
βγ+~ω
q(26)
#
l " f N q H í 7 H \ @ /ô Ç e ¦ | ½ Óß ¼ ì r í < ÊÃ ºs . d (26) _ Ó ü t o & h _ p H 6 £ § õ ° ú . ' Í ½ Ó É r í
7 H` ¦ f ¨ Ã º " f % 6 £ § © I α\ " f × æ ç ß © I γ Ð s
H כ ` ¦ _ p ô Ç . 7 £ ¤, 1 + N q H í 7 H _ ~ ½ ÓØ ¦` ¦ _ p ¦ f α (1 − f γ ) H α → γ s \ ¦ _ p ô Ç . ' Í ½ Ó_ ì r ¸ H
~ω + E α = E γ + ~ω q s Ù ¼ Ð \ -t Ð > rZ O g Ë :s $ í w n < Ê
`
¦ _ p ô Ç . Qt ½ Ó[ þ t ¸ ° ú É r ~ ½ ÓZ O Ü ¼ Ð K $ 3 ½ + É Ã º e
¦, ¸ H ½ Ó\ H f β − f α H íl © I β\ " f þ j7 á x
© I α Ð s < Ê` ¦ _ p ô Ç . s X O > ¼ # o ô Ç Ó ü t o & h K
$
3 s 0 p x ô Ç õ \ ¦ % 3 ` ¦ Ã º e % 3 ~ s Ä » H # l \ " f 6
x ô Ç í ß H É r s : r[2-8] \ " f ¸{ 9 ) a כ [ þ t õ H Ø
Ô ¦, > í ß õ & ñ \ " f : £ ¤Z > ô Ç l Z O [\ V\ ¦ [ þ t # Q d (22)]\ ¦
6 x % i l M :ë H s .
V. ¤V 4 m
ü < F g$ í í 7 H _ © ñ 6 x s l ¸ ¸\ p u H
% ò
¾ Ó` ¦ ½ ¨^ & h Ü ¼ Ð ¸ l 0 AK 6 £ §` ¦ 6 x # Ã º u
> í ß ` ¦ ô Ç .
(x) αβ = [x 0 δ N
α,N
β+ l c
q N
β+1
2 δ N
α,N
β+1
+l c q N
β2 δ N
α,N
β−1 ]δ n
α,n
βδ k
yα,k
yβ(27) (j x ) βα = − mil e~
c
[ q N
α2 δ N
β,N
α−1
− q
N
α+1
2 δ N
β,N
α+1 ]δ n
α,n
βδ k
yβ,k
yα(28)
|C αγ (q)| 2 = |V q | 2 δ k
yα,k
yγ+q
y|A n
α,n
γ(q z , L z )| 2
×K 1 (N α , N γ : t) (29) A n
α,n
γ(q z , L z ) = L 2
z
R L
z0 sin(n α πz/L z )
× exp(iq z z) sin(n γ πz/L z ) (30) K 1 (N α , N β : t) = N N
<!
>
! t ∆N e −t [L ∆N N
<
(t)] (31)
#
l " f (x) αβ =< α|x|β >, j x H é ß { 9 _ À Óx 9 ¸
í ß , t = ~q ⊥ 2 /2eB s ¦ L ∆N N
<(t) H > Ø Ô ' a ½ Ó d
(Associated Laguerre polynomial)s . q z H í 7 H _ Ã
º 7 ' q_ z$ í ì r, N < (N > ) H N α , N β × æ É r à º ( H à º) s
¦ ∆N = N > − N < s . F g$ í í 7 H â Ä º
|V q | 2 = e 2 ~ω l
2V 0
1
(∞) − 1
(0)
q
(q 2 + q 2 d ) 2 (32) s
. # l " f V H > _ Â Òx , (∞)ü < (0) H y y F g Ä » Ö
¦(optical dielectric constant) õ & ñ Ä » Ö ¦(static dielec- tric constant), ~ω l H F g$ í í 7 H _ \ -t , q d H 9 Debye U ´s _ % i à ºs .
&
ñ l © _ [ jl H y © ¦ - í 7 H © ñ 6 x _ [ j l
H ¦ & ñ ¦ / B N" î & h Â Ò H (ω ≈ ω c ) \ " f d
(20) _ z ´Ã ºÂ Òì r` ¦ ½ ¨ 6 £ § õ ° ú .
Re{σ xx (ω)} = − mV e
2~ lim s→0
+P
α,β N
α2
(f
β−f
α)Im{B
βα( ¯ ω)}δ
Nα,Nβ +1δ
nα,nβδ
kαy ,kβy[~¯ ω+~ω
c]
2+[Im{B
βα( ¯ ω)}]
2+ mV e
2~ lim s→0
+P
α,β N
α+1
2
(f
β−f
α)Im{B
βα( ¯ ω)}δ
Nα,Nβ −1δ
nα,nβδ
kαy ,kβy[~¯ ω−~ω
c]
2+[Im{B
βα( ¯ ω)}]
2(33)
#
l " f
lim
s→0
+(f β − f α )Im{B βα (¯ ω)} = X
q
X
γ
|V q | 2 |A n
β,n
γ(q z , L z )| 2 K 1 (N β , N γ ; t)δ k
βy,k
γy+q
z× < [(1 + N q )f (N α , n α ){1 − f (N γ , n γ )} − N q f (N γ , n γ ){1 − f (N α , n α )}]
×(−π)δ{~ω − (N γ − N α )~ω c − (n 2 γ − n 2 α ) 0 − ~ω q }
|[N q f (N α , n α ){1 − f (N γ , n γ )} − (1 + N q )f (N γ , n γ ){1 − f (N α , n α )}]
×(−π)δ{~ω − (N γ − N α )~ω c − (n 2 γ − n 2 α ) 0 + ~ω q } >
+ X
q
X
γ
|V q | 2 |A n
α,n
γ(q z , L z )| 2 K 1 (N α , N γ ; t)δ k
αy,k
γy+q
z× < [(1 + N q )f (N γ , n γ ){1 − f (N β , n β )} − N q f (N β , n β ){1 − f (N γ , n γ )}]
×(−π)δ{~ω − (N β − N γ )~ω c − (n 2 β − n 2 γ ) 0 − ~ω q }
|[N q f (N γ , n γ ){1 − f (N β , n β )} − (1 + N q )f (N β , n β ){1 − f (N γ , n γ )}]
×(−π)δ{~ω − (N β − N γ )~ω c − (n 2 β − n 2 γ ) 0 + ~ω q } > (34)
s
. d (34)\ ¦ d (33)\ @ /{ 9 l ¸ ¸\ ¦ ½ ¨½ + É Ã
º e .
GaAs â Ä º F g$ í í 7 H s l ¸ ¸\ p u H % ò ¾ Ó
`
¦ Ã ºu & h Ü ¼ Ð ¸ l 6 £ § _ Ó ü t o © Ã º[ þ t` ¦ ¦ 9ô Ç
[12, 13].
m = 0.067m 0 , m h = 0.51m 0 , E g = 1.424eV,
Fig. 1. Well width depedence of optical conductivity half-width due to electron-LO phonon scattering in pure GaAs for several photon energies.
(0) = 12.53, (∞) = 10.9, ω l = 2π × 8.76 × 10 12 Hz
#
l " f m 0 H Ä » _ | 9 | ¾ Ó, m h H ½ ¨" í (hole)_ | 9
|
¾ Ó, E g H \ -t ç ß s ¦ 2 " é ¶ x 9 ¸ H n 2D = 2 × 10 12 cm −2 Ü ¼ Ð ¿ ºl Ð ô Ç .
Fig. 1 É r F g ¸ ¸ y Ä ºÓ ü t _ ¿ ºa \ # Qb G>
H t \ ¦ F g _ \ -t \ @ /K Ð# Å Ò H Õ ªa Ë >s .
γ H F g ¸ ¸ Re{σ xx (ω)} _ ì ø Í; ¤ u 7 £ ¤, 2γ H þ j@ /u _
Fig. 2. Temperature dependence of optical conductivty
half-width due to electron-LO phonon scattering in pure
GaAs for several photon energies.
] X
ì ø Ís ÷ & H ç ß ` ¦ _ p ô Ç . " f í ß ê ø Í´ òõ 9 þ t à º 2
¤ γ ß ¼> è ß . > í ß õ \ _ ¿ ºa 7 £ x
½
+ ÉÃ º2 ¤ ì ø Í; ¤ u y è H כ Ü ¼ Ð z ¤ . Fig. 2 H ì ø Í
;
¤ u _ : r ¸_ > r$ í ` ¦ Ð# ï r . : r ¸ 7 £ x ° ú Ã º2 ¤ í 7 H _
ì r í < ÊÃ º 7 £ x Ù ¼ Ð í 7 H \ _ ô Ç í ß ê ø Í´ òõ 7 £ x
ô Ç . " f ì ø Í; ¤ u H 7 £ x ô Ç .
VI. + s Ç Â ] Ø
© I 1 l qw n % ò í ß \ ¦ 6 x # í 7 H õ © ñ 6 x
H ï r s " é ¶ > _ F g ¸ ¸\ ¦ > í ß Ù þ ¡ . ü < í
7 H _ © ñ 6 x _ [ jl ¦ & ñ # © ñ 6 x _ ]
jY L ½ Ó t ë ß ¦ 9ô Ç õ H Ó ü t o & h Ü ¼ Ð K $ 3 l ¼ # o
< Ê` ¦ · ú Ã º e % 3 . : r ¸ 7 £ x ì ø Í; ¤ u 7 £ x
H X < Õ ª s Ä » H í 7 H _ ì r í < ÊÃ º 7 £ x í 7 H \ _ ô
Ç í ß ê ø Í´ òõ & t l M :ë H s . Õ ª X < y Ä ºÓ ü t _ ¿ º a
7 £ x ì ø Í; ¤ u y è H כ Ü ¼ Ð z ¤ H X < s
\
@ /ô Ç © [ jô Ç : r É r III-V 7 á ¤ _ É r Ó ü t| 9 \ @ /ô Ç s
: r& h ] X H õ < Êa z ´+ « > õ e # Q 0 p x ½ + É כ Ü ¼ Ð
«
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Effect of Optical Phonon Scattering on the Optical Conductivity in a Quasi-Two-Dimensional Electron System
Nam Lyong Kang ∗
Faculty of Liberal Arts, Miryang National University, Miryang 627-702 (Received 30 September 2005, in final form 2 January 2006)
Utilizing the quantum statistical operator algebra technique, we derive the intraband linewidth function in the optical conductivity for a system of electrons interacting with longitudinal optical phonons in a quantum well. The electron and the phonon distribution functions are included in the conductivity, so we can explain the phonon emission and absorption in an organized way for all electron transition processes. The numerical result shows that the width decreases with the well width and increases with the temperture.
PACS numbers: 72.20.-i, 72.10.Di
Keywords: Conductivity, Scattering by phonons
∗