w
= k5 ¹ Å 4 ; c" e W _ Ë 8 ý Ò Åy ; c  \ ¥ Ò Å] k ù° Ë Ñ ¹ Åy ¢y ¢5 8 ý P c p7 û ß Ã Å R w
T g ` @+ ä · T a : @® £ · T < 0 å · » Ða : @
â
· ¡ ¤ @ / < Æ § F g s ½ ¨z ´, @ /½ ¨ 702-701
~ ç
¡ ó j u
x 9
ª @ / < Æ § § ª õ & ñ Â Ò, x 9 ª 627-702
) o
+ ä * å
â
· ¡ ¤ @ / < Æ § l / B N < ÆÂ Ò, @ /½ ¨ 702-701
Ð ç ¡¦ · L | ç ¡% ã < ∗
â
· ¡ ¤ @ / < Æ § Ó ü t o < Æõ , @ /½ ¨ 702-701 (2003¸ 4 Z 4 17{ 9 ~ Ã Î6 £ §)
¦^ ? / > \ " f F g ¸ ¸_ y û Z \ ¦ % ò í ß ~ ½ ÓZ O ` ¦ ² ú o # Ä » ¸ % i . # l " f ½ ¨ ô
Ç s y û Z \ H - í 7 H s _ Ø æ[ t õ & ñ ÷ rë ß m ü @Â Ò\ " f Å Ò# Q y n C_ ´ òõ \ ¦ í < Ê ¦ e
. y y _ í ß ê ø Í \ ¦ Ø Ô> ½ + É â Ä º - í 7 H ÷ rë ß m - ¢ ¸ H -Ô ¦í HÓ ü t \ t 6
£
x6 x ½ + É Ã º e ¦ Ò q ty ) a . # l \ " f ½ ¨ô Ç F g ¸ ¸\ " f ' Í P : % ò ~ ½ ÓZ O Ü ¼ Ð ½ ¨ô Ç y û Z H f ] X
s + þ A s 9 þ t Ðà Ô : r / B N" î õ ° ú s \ -t ç ß s { 9 & ñ ô Ç â Ä º\ ô Ç # & h 6 x 0 p x t ë ß , ¿ º P :
~
½
ÓZ O Ü ¼ Ð ½ ¨ô Ç y û Z H 0 A_ â Ä º÷ rë ß m \ -t ç ß s { 9 & ñ t · ú § H â Ä º\ " f ¸ & h 6 x 0 p x
¦ Ò q ty ) a .
PACS numbers: 72
Keywords: F g ¸ ¸ , > , % ò í ß , y û Z
I. " e  ] Ø
þ
j H ¦ ¸_ í ß \ O oü < 8Ô ¦ # Q ì ø Í ¸^ ? /_ [ þ t_
1 l x \ ' aô Ç ½ ¨ 8¹ ¡ ¤ Ö ¸µ 1 ÏK t ¦ e . ì ø Í ¸^ ? /_
r & h Ó ü t o | ¾ Ó[ þ t \ @ /ô Ç s : r É r ª : x > % i < Æ& h ~ ½ ÓZ O Ü
¼ Ð & ñ w n ÷ & H כ s м # & h s . s M : Å Ò ) a @ / © s ÷ &
H כ É r l ¸\ ¦ í < Ê H [ þ t_ Ã º5 Å x & ³ © s ¦ Ã
º5 Å x \ % ò ¾ Ó` ¦ Å Ò H f ä ¼a Ë >B j m 7 £ §(scattering mecha- nism) s . s Qô Ç ½ ¨× æ \ @ /³ ð ÷ & H כ É r + þ A6 £ x² ú s
: r s [1–13]. s כ É r ì ø Í ¸^ \ " f_ y n C_ f ¨ à ºü < ~ ½ Ó Ø
¦1 p x` ¦ í < Ê H r ç ß & h Ü ¼ Ð 1 l x H ô Ç l © \ _ ô
Ç | × ¼a Ë >(perturbation)\ @ /K " f $ í / B N& h Ü ¼ Ð & h 6 x ÷ & ¦ e
. r ç ß & h Ü ¼ Ð 1 l x H l © \ _ K " f Ò q tl H
¸ ¸\ @ /ô Ç + þ A6 £ x² ú s : r É r ª : x > % i < Æ_ ½ Ó0 A\
#
Q t ^ > í ß l Z O ` ¦ í < Ê ¦ e Ü ¼ 9 % ò l Z O ¸ Õ
ª × æ . s l Z O \ " f H % ò ( Vq » ¡ § í ß : pro- jector)\ ¦ # Qb G> × þ H \ " f É r > h+ þ Ad ` ¦
∗
E-mail: [email protected]
°
ú > ) a . : r ½ ¨ É r Y > t _ % ò \ ¦ 6 x # Y >
>
h_ s : r` ¦ ¸Ø ¦ô Ç & h s e . [4,12,14,15] % ò H é ß { 9
% ò , ^ % ò Ð ½ ¨ì r ÷ & ¦, s [ þ t y y É r r
© I _ > r % ò (state-dependent projector), © I 1 l q w n
% ò (state-independent projector)1 p x Ü ¼ Ð ì r À Ó ) a .
© I _ > r % ò \ ¦ & h 6 x½ + É â Ä º (L d J k = const · J z ) ÷ &
#
Q & ñ l © s § 4 ` ¦ â Ä º 7 £ ¤ f ] X s + þ A s 9 þ t Ðà Ô : r /
B
N" î õ ° ú s \ -t ç ß s { 9 & ñ ô Ç â Ä º\ ô Ç # 6 x
½ +
É Ã º e [16–18]. Õ ª Q © I 1 l qw n % ò \ ¦ & h 6 x (L d J k ∗ = 0) ÷ &Ù ¼ Ð 0 A_ â Ä º ÷ rë ß m \ -t ï r 0 A s _ ç ß s { 9 & ñ t · ú § É r â Ä º\ ¸ | Ã Ðf
¦ Å Ò © ÷ & ¦ e [19]. ¢ ¸, © I _ > r % ò \ ¦ & ñ _ H
~
½ ÓZ O É r ª H z ´` ¦ · ú > ÷ &% 3 . [20] : r ½ ¨
É
r s [ þ t_ % ò ~ ½ ÓZ O ` ¦ + " f Y > Y > ì ø Í ¸^ ? /_ s 9 þ t Ð à
Ô : r s \ " f_ f ¨ Ã º ; ¤` ¦ > í ß Ù þ ¡ . Õ ª Q s [ þ t` ¦
½
¨ ¸& h Ü ¼ Ð q § H { 9 \ H èf . Ë y K M ® o . : r 7 Hë H \
"
f H ¿ º> h_ % ò \ ¦ & ñ _ ¦ s [ þ t` ¦ + " f ¸ ¸ J $
"
fü < ; ¤ < ÊÃ º(linewidth function) x 9 s ¢ - aÖ ¦(relaxation
-100-
~
½ ÓZ O ` ¦ è> hô Ç . s ¿ º ~ ½ ÓZ O s # Qb G> Ø Ô 9
#
Q " â Ä º\ Ð | à Ðf > 6 x| ¨ c à º e H t \ @ /K
"
f Ð_ ô Ç . # l \ " f H o Ä ºq _ ~ ½ Ó& ñ d \ " f Ø ¦µ 1 Ï
#
x 9 ¸ í ß \ ¦ ½ ¨ ¦ l _ 1 l x+ þ A_ l © \
@
/ô Ç À Ó_ ¨ î ç H` ¦ ½ ¨ # + þ A H \ " f_ 6 §(Ohm)_
^
> \ ¦ × þ H { 9 ì ø Í& h + þ A6 £ x² ú s : r~ ½ Ód ` ¦ G × þ ô Ç
. s M : H ¸ ¸J $ " fü < Õ ª כ s í < Ê H y û Z
\ Å Ò3 l q # Ð_ l Ð ô Ç . ] j 2 © \ " f H F g
¸ ¸ J $ " fü < ¿ º % ò \ ¦ + " f y û Z \ ¦ + þ Ad o ¦ q
§ô Ç . ] j 3 © \ " f H : r` ¦ ë B H .
II. ° Ë Ñ ¹ Åy ¢y ¢ Ö " eÑ ÷ P c p7 û ß Ã Å 8 ý ] k ùÅ k Ä× D
F
gf ¨ Ã º\ @ /ô Ç + þ A6 £ x² ú s : r \ " f_ ¿ º © I _ > r % ò
~
½ ÓZ O ` ¦ q § l 0 A # | × ¼a Ë >s \ O ` ¦ M :_ > _ K x 9 Ðm î ß ` ¦
H eq = H d + V = X
α
E α a † α a α + V (1)
¦ s כ \ @ /6 £ x H o Ä ºq í ß (Liouville oper- ator)\ ¦
L eq = L d + L v (2)
.
E α H © I |α >\ " f_ é ß { 9 _ \ -t s ¦ a † α (a α ) H © I α\ @ /ô Ç Ò q t$ í ( èY > ) í ß s . s M :_ x 9
¸ í ß \ ¦ ρ eq Ð ¿ ºl Ð ô Ç . # l \ l ü < ° ú
É
r r ç ß _ > r | × ¼a Ë >` ¦ 6 x r v > H q ¨ î + þ As ) a .
© F G H (dipole approximation)\ " f_ | × ¼a Ë >_ K x 9
Ðm î ß É r
H int = e X
l=1,2,3
X
αβ
(x l ) αβ a † α a β E l exp(iωt) + c.c (3)
Ð Ñ ü t à º e . e H _ l | ¾ Ó_ ] X @ /u , x l É r é ß { 9
_ 0 Au ý a³ ð Ð" f x 1 = x, x 2 = y, x 3 = z s ¦, ω H
l © _ y 1 l x à º, c.c H 4 ¤ è/ B NÓ os . e _ _ í ß Y \ @ /K " f Y αβ =< α |Y |β >s . > _ À Ó í
ß J l (l = 1, 2, 3) É r J l = X
λ
l,λ
2J l ∗ = X
λ
1,λ
2(j l ) λ
1λ
2a † λ
1
a λ
2(4)
s
¦ j l É r é ß { 9 _ À Ó í ß s . + þ A H \
"
f_ s > _ À Ó_ l @ /u ( © © ^ ¦¨ î ç H) H 6
§(Ohm)_ + þ Ad Ü ¼ Ð j þ t à º e . 7 £ ¤
< J k >= X
l
σ kl (ω)E l (ω) (5)
. ] j 1+ þ Ad \ " f H
σ kl (ω) = −e X
α,β
(x l ) αβ A αβ k (¯ ω)
= −e X
α,β
(x l ) αβ < (~¯ ω − L eq ) −1 J k > αβ (6)
s
¦ ] j 2+ þ Ad \ " f H
σ kl (ω) = −e X
α,β
X
γ,δ
(x l ) αβ (j k ) γδ A ˜ γδ αβ (¯ ω)
= −e X
α,β
X
γ,δ
(x l ) αβ (j k ) γδ < (~¯ ω − L eq ) −1 a † γ a δ > αβ (7)
Ð H .
#
l \ " f¯ ω ≡ ω − ia(a → 0 † ) s ¦
< X > αβ = T R ρ eq [X, a † α α β ]
(8)
s
¦ T R H ^ à ÔY Us Û ¼(many body trace) s ¦ [A, B] ≡ AB − BAs .
1. < g 1] k ùÅ k Ä
]
j 1 + þ Ad \ " f_ ì r K H 6 £ § õ ° ú .
A αβ k (¯ ω) =< (~¯ ω − L eq ) −1 J k > αβ (9)
s
כ ` ¦ > í ß l 0 A # 6 £ § õ ° ú É r % ò
(projector)P, Q\ ¦ & ñ _ ô Ç .
P k αβ X = < X > αβ
< J k > αβ J k (10)
Q αβ k = 1 − P k αβ (11)
s
% ò í ß \ ¦ d (9)\ í < Ê÷ &# Q e H o Ä ºq
_ ¸ É rA á ¤ \ L eq = L eq (P k αβ + Q αβ k ) ü < ° ú s & h 6 x ¦ (A − B) −1 = A −1 + A −1 B(A − B) −1 \ ¦ + " f ì r K \ ¦
> h 6 £ § õ ° ú s S X © ) a .
1
~¯ ω − L eq
J k = 1
~ ω ¯ − L eq Q αβ k − L eq P k αβ J k
= 1
~ ω ¯ − L eq Q αβ k J k + 1
~ ω ¯ − L eq Q αβ k L eq P k αβ 1
~ ω ¯ − L eq
J k
= 1
~ ω ¯ J k + 1
~ ω ¯ − L eq Q αβ k L eq J k A αβ k (~¯ ω)
< J k > αβ
(12)
s
כ ` ¦ & ñ o 6 £ § õ ° ú s ) a .
A αβ k (¯ ω) = < J k > αβ
~ ω ¯ − Ω αβ − iΓ αβ (¯ ω) (13)
#
l \ " fΩ αβ H s 1 l x < ÊÃ º (lineshift function)s 9, iΓ αβ (ω) H y û Z (damping factor)s . # l \ " f P k αβ J k = J k ü < Q αβ k J k = 0 ` ¦ s 6 x s 1 l x < ÊÃ º Ω αβ H 6 £ § õ ° ú s Å Ò# Q .
Ω αβ ≡ T R {ρ eq [L eq J k , a † α a β ] }/ < J k > αβ (14)
À
» d \ " f L eq 5 Å q \ í < Ê ÷ &# Q e H L d _ © ± ú É r
½ Ó t H # > í ß ¦, L d a † α a β = E αβ a † α a β ` ¦ s 6
x ,
Ω αβ ∼ = −E αβ (15)
) a . # l \ " f E αβ = E α − E β s .
d
(13) \ í < Ê ÷ &# Q e H y û Z H 6 £ § õ ° ú .
iΓ αβ k (¯ ω) < J k > αβ =< L eq Q αβ k (~¯ ω −L eq Q αβ k ) −1 L eq J k > αβ
(16) s
כ ` ¦ > í ß ,
iΓ αβ (ω) < J k > αβ = −E αβ < (~¯ ω − L eq Q αβ k ) −1 L eq J k > αβ +T R {ρ eq [L v a † α a β , (~¯ ω − L eq Q αβ k ) −1 L eq J k ] }
− T R {ρ eq [L eq a † α a β , J k ] } < (~¯ ω − L eq Q αβ k ) −1 L eq J k > αβ / < J k > αβ (17)
s
÷ & 9, L d J k = ~ωJ k = constJ K s ¦, © ñ 6 x s y
© t · ú § É r â Ä º\ [Â Ò2 ¤ A] \ 6 £ § õ ° ú s H
) a .
iΓ αβ k (ω) < J k > αβ ≈ T R {ρ eq [L v a † α a β , (~¯ ω − L d ) −1 L v J k ] } (18)
#
l \ " f
< J k > αβ = (f β − f α )(j k ) βα (19) s
. # l \ " f f α ≡ T R {ρ eq [a † α a α ] } Ð © I α\ @ /ô Ç
_ ` Ø Ôp n | Ã Ì ì r í < ÊÃ ºs . " f d (13) \ d
(15) ü < d (19)\ ¦ V , # Q" f ì r K \ ¦ r & h # Q Ð
6 £ § õ ° ú s ) a .
A αβ (¯ ω) = (j k ) βα (f β − f α )
~¯ ω − E βα − iΓ αβ k (¯ ω) (20)
iΓ αβ k (ω) = T R {ρ eq [L v a † α a β , (~¯ ω −L d ) −1 L v J k ] }/ < J k > αβ
(21) L d ü < L v Å Ò# Qt A αβ (¯ ω) _ ½ ¨^ & h + þ AI \ ¦ ½ ¨
½ +
É Ã º e .
2. < g 2] k ùÅ k Ä
]
j 2 + þ Ad _ ì r K H 6 £ § õ ° ú .
A ˜ γδ αβ (¯ ω) =< (~¯ ω − L eq ) −1 a † γ a δ > αβ (22)
_
ô Ç .
P ˜ γδ αβ X = < X > αβ
< a † γ a δ > αβ
a † γ a δ (23)
Q ˜ αβ γδ = 1 − ˜ P γδ αβ (24)
s
. s כ ` ¦ + þ Ad 1\ " fü < ° ú É r ~ ½ ÓZ O Ü ¼ Ð S X ©
1
~ ω ¯ − L eq
a † γ a δ = 1
~ ω ¯ − L eq Q ˜ αβ γδ − L eq P ˜ γδ αβ a † γ a δ
= 1
~ ω ¯ − L eq Q ˜ αβ γδ a † γ a δ + 1
~ ω ¯ − L eq Q ˜ αβ γδ L eq P ˜ γδ αβ 1
~¯ ω − L eq
a † γ a δ
= 1
~¯ ω a † γ a δ + 1
~¯ ω L eq Q ˜ αβ γδ 1
~ ω ¯ − L eq Q ˜ αβ γδ a † γ a δ + 1
~ ω ¯ − L eq Q ˜ αβ γδ L eq P ˜ γδ αβ 1
~ ω ¯ − L eq
a † γ a δ
= 1
~ ω ¯ a † γ a δ + 1
~ ω ¯ − L eq Q ˜ αβ γδ L eq
< (~¯ ω − L eq ) −1 a † γ a δ > αβ
< a † γ a δ > α β a † γ a δ
(25)
) a . # l \ " f
(~¯ ω) −1 L eq Q ˜ αβ γδ (~¯ ω − L eq Q ˜ αβ γδ ) −1 a † γ a δ = (~¯ ω) −1 (~¯ ω − L eq Q ˜ αβ γδ ) −1 L eq Q ˜ αβ γδ a † γ a δ (26) ü
< ° ú s " f Ð § ¨ 8 > í ß s 0 p x . s כ ` ¦ > í ß
Q ˜ αβ γδ a † γ a δ = (1 − ˜ P γδ αβ )a † γ a δ = a † γ a δ − ˜ P γδ αβ a † γ a δ = a † γ a δ − < a † γ a δ > αβ
< a † γ a δ > αβ
a † γ a δ = 0 (27)
s
Ù ¼ Ð,
(~¯ ω) −1 L eq Q ˜ αβ γδ (~¯ ω − L eq Q ˜ αβ γδ ) −1 a † γ a δ = 0 (28) s
) a . À » d ` ¦ ¦ 9 # d (22)\ ¦ r & h # Q Ð ,
A ˜ γδ αβ (¯ ω) = < a † γ a δ > αβ
~ ω ¯ − ~¯ ω ˜ B αβ (¯ ω)/ < a † γ a δ > αβ
(29) s
) a . # l \ " f
B ˜ αβ (¯ ω) =
* 1
~ ω ¯ − L eq Q ˜ αβ γδ L eq a † γ a δ +
αβ
(30)
s
. d (29)\ ¦ 7 á § 8 © [ jy > í ß ,
< a † γ a δ > αβ = T R {ρ eq [a † γ a δ , a † α a β ] }
= T R {ρ eq [ a † γ a β δ δα − a † α a δ δ γβ ] }
= (f γ − f α )δ γβ δ δα (31)
s
÷ & ¦, ˜ B αβ (¯ ω) H 6 £ § õ ° ú s S X © 0 p x .
B ˜ αβ (¯ ω) =
* 1
~¯ ω − L eq Q ˜ αβ γδ L eq a † γ a δ +
αβ
= 1
~ ω ¯ < L eq a † γ a δ > αβ + 1
~¯ ω < L eq Q ˜ αβ γδ 1
~ ω ¯ − L eq Q ˜ αβ γδ L eq a † γ a δ > αβ (32)
< L v a † γ a δ > αβ H b q ¢ ¸ H b † −q × æ ô Ç > h\ @ /ô Ç © ©
^
¦ ¨ î ç H s ÷ &Ù ¼ Ð Õ ª ° ú כ É r % ò s ÷ & 9, [Â Ò2 ¤ B] \ ¦ Ã Ð ¦
#
> í ß ,
B ˜ αβ (¯ ω) = 1
~ ω ¯ E βα (f β − f α ) + 1
~ ω ¯ < L eq Q ˜ αβ γδ 1
~ ω ¯ − L eq Q ˜ αβ γδ L d a † β a α > αβ (33) s
. s d _ z ´ » ½ Ó` ¦ > í ß l 0 A # L v _ ] jY L ½ Ó t ë ß H ¦, L d J k ∗ = 0 s ÷ & 9, T R {ρ eq [L eq Q ˜ αβ γδ X, a † α a β ] } = T R {ρ eq [L v a † α a β , X] }δ γβ δ δα \ ¦ s 6 x ,
< L eq Q ˜ αβ γδ 1
~ ω ¯ − L eq Q ˜ αβ γδ L d a † β a α > αβ = E βα T R {ρ eq [L eq Q ˜ αβ γδ (~¯ ω − L eq Q ˜ αβ γδ ) −1 a † β a α , a † α a β ] }
∼ = T R {ρ eq [L v a † α a β , (~¯ ω − L d ) −1 L v a † β a α ] }δ γβ δ δα (34)
) a . À » d ` ¦ ¦ 9 # Ä ºo · ú ¦ H ì r K
\
¦ r & h # Q Ð
A ˜ γδ αβ (¯ ω) = (f β − f α )
~ ω ¯ − E βα − Γ αβ γδ (¯ ω) (35)
) a . # l \ " f y û Z Γ αβ γδ (¯ ω) H
Γ αβ γδ ∼ = T R {ρ eq [L v a † α a β , (~¯ ω − L d ) −1 L v a † β a α ] }δ γβ δ δα (36) s
. # l \ " f ¸ L d ü < L v & ñ K t ˜ A γδ αβ (¯ ω)_ ½ ¨
^
& h + þ AI \ ¦ ½ ¨½ + É Ã º e . ¿ º + þ Ad _ q § H 6 £ § õ
° ú .
3. R w
" f ] j 1 + þ Ad _ ¸ ¸ J $ " f H σ kl (ω) = −e X
α,β
(x l ) αβ (jk) βα f β − f α
~ ω ¯ − E βα − i~Γ αβ
= −e X
α,β
(x l ) αβ (jk) βα
f β − f α
~ ω ¯ − E βα − < [L v a † α a β , (~¯ ω − L d ) −1 L v J k > 0 /< J k > αβ
(37)
÷ & ¦, ] j 2 + þ Ad _ ¸ ¸ J $ " f H σ kl (ω) = −e X
α,β
(x l ) αβ (j k ) βα f β − f α
~ ω ¯ − E βα − i~Γ αβ
= −e X
α,β
(x l ) αβ (j k ) βα f β − f α
~¯ ω − E βα − < [L v a † α a β , (~¯ ω − L d ) −1 L v a † β a α > 0 / < a † γ a β > αβ
(38)
s
.
< x > 0 H X _ ¨ î + þ A © © ^ ¦ ¨ î ç H s . ë ß L v \ @ /6 £ x H í ß ê ø Í ( J $ [ > V \ @ /K " f
< [L v a † α a β , (~¯ ω − L d ) −1 L v J k ] > 0 < a † γ a β > αβ = < [L v a † α a β , (~¯ ω − L d ) −1 L v a † α a β ] > 0 < J k > αβ (39)
Ð ì r K | ¨ c à º e Ü ¼ ¿ º + þ Ad É r ° ú . \ V\ ¦ [ þ t # Q - í 7 H > \ " f H { 9 ì ø Í& h Ü ¼ Ð V = X
q
X
α,µ
C α,µ (q)a † α a µ (b q + b † −q ) (40)
1 l
x| ¾ Ós ~q, −~q í 7 H_ èY > , Ò q t$ í í ß s .) J k H d
(4) Ð Å Ò# Qt Ù ¼ Ð ~ 1 > d (39) Ð Ã ºì r K ÷ &t · ú § H
. [ d (39) _ L v \ Å Ò3 l q ~ 1 > · ú Ã º e .] " f
¿
º + þ Ad É r Ø Ô .
ì
ø Í ¸^ \ & ñ l © ` ¦ r v [ þ t É r { ? / s ü
< { ç ß s \ ¦ { 9 Ü ¼ . & ñ l © ` ¦ Ù þ ¡` ¦ â Ä º { 9 # Q
H \ -t ç ß s { 9 & ñ ô Ç â Ä º\ ô Ç # H ] j 1+ þ Ad s 8
À Òl ~ 1 ¦ · ú 94 R e [21–23]. Õ ª Q \ -t ç ß
s { 9 & ñ ô Ç f ] X s + þ A s 9 þ t Ðà Ô : r / B N" î õ ° ú s { 9
&
ñ t · ú § É r â Ä º\ " f H ] j 2+ þ Ad s 8 | Ã Ðf . ] j 2+ þ Ad É r L d J k ∗ = 0 s ÷ &Ù ¼ Ð { 9 ì ø Í& h Ü ¼ Ð & h 6 x 0 p x
.
III. + s Ç Â ] Ø
#
l \ " f Ä ºo H ¿ ºt % ò í ß ~ ½ ÓZ O ` ¦ s 6 x
#
y y + þ A l ¸ ¸\ ¦ ½ ¨ % i . y y _ ¸ ¸ H L v _ ] jY L ½ Ó t H # ½ ¨ % i . s כ É r e _ _ x 9
¸ í ß _ - í 7 H © ñ 6 x K x 9 Ðm î ß É r © ñ
6 x s ô Ç > _ F g ¸ ¸_ : £ ¤f ç \ H ß ¼> % ò ¾ Ó` ¦ p u
t 3 l w l M :ë H s . y û Z ½ Ó\ e H F g ¸ ¸ J $
" f\ H ü < í 7 H s _ Ø æ[ t õ & ñ ÷ rë ß m ü @ Â
Ò\ " f Å Ò# Q y n C_ Å Ò Ã º_ / B N ³ ´ òõ ì ø Í% ò ÷ &# Q e
. ¿ º + þ Ad \ e # Q" f L v & ñ K t y û Z \ ¦ ½ ¨
¦ " f F g ¸ ¸ J $ " f\ ¦ ½ ¨½ + É Ã º e . Õ ª Q # QÖ ¼ A
á
¤ s 8 Ä »6 x > æ ¼# t H t \ @ /ô Ç 7 H_ H L v _ + þ AI
\
\ ¦ כ Ü ¼ Ð l @ /ô Ç . s \ @ /ô Ç © [ jô Ç ¸
H · ú ¡Ü ¼ Ð Ã º' ½ + É ½ ¨ õ ] js .
P c
p 8 ý ò k >
: r ½ ¨ H < Ʋ D G ½ + ÉÕ ü t < É ª F é ß ½ ¨t " é ¶ (KRF-2002- 015-DP0122) _ t " é ¶ Ü ¼ Ð s À Ò# Q & Ü ¼ 9 s \ y × ¼w n m
.
Y c
p w à U Ø ô
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APPENDIX A
T R ρ eq [L eq A, a † α a β ],
= T R {ρ eq [H eq A − AH eq , a † α a β ] }
= T R {ρ eq ((H eq Aa † α a β − AH eq a † α a β ) }
− T R {ρ eq (a † α a β H eq A − a † α a β AH eq ) } (A1) [H eq , ρ eq ] = 0 s ¦ T R {ABC} = T R {BCA} ` ¦ & h 6 x
,
T R ρ eq [L eq A, a † α a β ],
= T R {ρ eq ((Aa † α a β H eq − AH eq a † α a β ) }
− T R {ρ eq (a † α a β H eq A − H eq a † α a β A) } (A2)
÷ & 9, þ j7 á x& h Ü ¼ Ð 6 £ § õ ° ú É r õ \ ¦ % 3 H .
T R {ρ eq [L eq A, a † α a β ] } = T R {ρ eq [L eq a † α a β , A] } (A3)
APPENDIX B
< L eq a † γ a δ > αβ = < L d a † γ a δ > αβ + < L v a † γ a δ > αβ
= < L e a † γ a δ > αβ + < L p a † γ a δ > αβ
+ < L v a † γ a δ > αβ (B1)
< L d a † γ a δ > αβ = T R ρ eq [ (L e + L p )a † γ a δ , a † α a β ]
= T R ρ eq [ L e a † γ a δ , a † α a β ]
= E γδ T R ρ eq [ a † γ a δ , a † α a β ]
= E γδ (f γ − f α )δ γβ δ αδ (B2)
< L p a † γ a δ > αβ = 0 (B3)
< L v a † γ a δ > αβ = 0 (B4)
Comparison of Damping Factors in the Optical Conductivity of Many-electron System in Solids by Using Two Projection Techniques
Hyun Jung Lee, Yun Ju Lee, Jai Hoon Lee and So Youn Kim Optical Transition Laboratory, Kyungpook National University, Daegu 702-701
Nam Lyong Kang
Faculty of Liberal Arts, Miryang National University, Miryang 627-702
Jung Young Sug
Faculty of Electronic and Electrical Engineering, Kyungpook National University, Daegu 702-701
Sang Gyu Jo and Sang Don Choi ∗
Department of Physics, Kyungpook National University, Daegu 702-701 (Received 17 April 2003)
Two different projection techniques are applied to derive the damping factors contained in the optical conductivity tensors of a many-electron system in solids. The damping terms contain the effect of the external radiation, as well as the electron phonon interaction. The two results turn out to be different form each other in general. The first form is well known to be applicable to cyclotron transitions in systems with constant energy separations. The second one seems to be more suitable for transitions with irregular energy separations.
PACS numbers: 72
Keywords: Optical conductivity, Many-electron system, Projection technique, Damping term
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