! " # # # $
$ $ $ % " # " &
' #
( # # # #
& ) & %
*
+, -.
/0
*
- *+.*
1
/0 .
2 "
/0 3 * +, -. /0 *
1 /0 . 2 " 4 $ /0
!5 *
6
7
# # 6
! $ $ ; ' & #
% " # " & '
$ ! % " #
$ $ %
" % $ % $ " < *
= ! % #
# # # "
$ $
(
> " $ " !
$ $
-$ " $ % ! $
( $ ?
( ' " % $
# " 6 ' #
% " %
-# & % $
"
$ " >
! $ $ $ % " #
# # # $ 6 % (
( % $ > " &
% $ 1 #
1 &
" % $ > ! $
! " '
# ( ! ( $ #
" $ $ &
! ( $
-" 4 $ $
& " $ $
% # " # !
( ( * ( # $
1 ( & * < =
$ $ 4 " ! ( $
" # & $
! " % % & $
$ ! $ " # & "
$ $
& $ $ ! $ %
( $ # $ ! $
% $
! % $ $ $
$ A + < = < @=
$ $ &
$ $
$ " # & !
$
$ $ "
$$ # ' $
$ ' # &
-% " ! &
; !
% " " $
# > "
" $ " $
$ A # % $
# $ #
% # " < < @== $
$-" # 8 (
# %
" %
+ 0 ! % < @= $
-" # # # $ ! $
( $ & ! '
$ $ # "" " $ $ %
& $ $ $
& "
-$ $ ! " $
$ $
# $ # % " 4
& # )
& % $ " % %
!
# " " " % % ! & %
B
% 4 %
&$ ! # & C ;
# $ ( $ % 4
: #
@ D # $ # E
" % F
! G $ # # 7
max
{ct,kt ,Lt }∞t ∞
t
βtu(c t)
s.t
ct+kt =wt+rtkt+ (1−δ)kt+qtLt+κt
ct, kt 0 0 Lt 1 t
k >0 " %
# ct $ G $ $ tH kt
$ # $ tH Lt $
-# ( $ qtH κt
$-$ " % H wt rt
# " % % $ %
$ $ %
! 4 $ {(qt, wt, rt)}∞t
$ {κt}∞
t " % # " $ 4
-$ $ # #
$
. % % G $ # $
# " $ " C 4
v(k) =
maxh,c[u(c) +βv(h)]
s.t c+h=w+rk+ (1−δ)k+q+κ
c, h 0
< =
! ( " %
−u′(c(k)) +βv′(h(k)) = 0 < =
# h(k) c(k) $ $ $ $
$ $ %
C * % $ ! # ( &$ ( % %
%
v′(k) = (1 +r−δ)u′(c(k)) <:=
" <:= < = # 4
-G $ * 4 ! 4 "
# G " ( $
-$ $
u′(c(k)) =β(1 +r′−δ)u′(c(h(k))) <@=
c(k) +h(k) =w+rk+ (1−δ)k+q+κ < =
# " 7
u(c) = 1
1−γc
−γ <D=
B " # # 4 <@= < = # 7
c(k)−γ =β(1 +r′−δ)c(h(k))−γ <F=
c(k) +h(k) =w+rk+ (1−δ)k+q+κ <I=
! # 7 # &
" # & " % !
" $ &
$ < $ $ =
# " & "
$ % $
&
$-$ * $ %
(
! " %
# "
F (Kf, Nf) =AK
αf
f N
−αf
f
G(Ki, Ni, L) =AB KiψL −
ψ αi
N −αi
i
# 0 < αf < 1 0 < αi < 1 0 < ψ < 1 Kf Ki
$ $ % H Nf Ni
$ % H L
$ ! A $ $ %
B $ %
$ % ! $
" % αf " " %
αiψ " %
1−αi " " % 1−αf #
%
wf rf # " $ $ %
( " % ! $ ( $ %
( " %
πf = (1−τva)AK
αf
f N
−αf
f −(1 +τl)wfNf −(1 +τk)rfKf <J=
# τva & % < 0< τva <1= τk
& % $ % <τk >0= τl &
% % <τl >0=
( T−
va ≡ (1−τva) Tl ≡ (1 +τl) Tk ≡ (1 +τk)
4 <J= #
πf =Nf Tva− Ak
αf
f −Tlwf −Tkrfkf < =
# kf ≡
Kf
Nf
! ( ( G $ ( & ; $
; $ ( $ # " $ 7
rf =
T−
va
Tk
Aαfk
αf−
f < =
wf =
T−
va
Tl
A(1−αf)k
αf
f < =
! ; $ $
(
! $ ( $ % ( " %
πi =AB K
ψ i L
−ψ αiN −αi
i −wiNi−riKi−qL < :=
# q % $ $
( " % # " wi
ri % $ q
! ( ( G $ ( & ; $
; $ ( $ # " 4 7
ri =
ABαiψ kiψl
−ψ i
αi
ki
< @=
q= ABαi(1−ψ) k
ψ i l
−ψ i
αi
li
< =
wi =AB(1−αi) kiψl
−ψ i
αi
< D=
# ki ≡ KNi
i li ≡
L Ni
! % ( $ $
$ (
$ G !
-$ $ # " 7
w=wf =wi
r =rf =ri
B " 4 < = < = < @= < D= # ( # " 7
w
r =
Tk
Tl
1−αf
αf
kf
= 1−αi
αiψ
ki < F=
! $ - - $ $
ki =
Tk
Tl
αi
αf
1−αf
1−αi
ψkf < I=
% " % & (
$
$-$ ! " % " " %
κ =τvaAKαf
f N
−αf
f +τlwNf +τkrKf < J=
# τva τl τk & "
!
"
#
$%
4 G $ 7
c(k) +h(k)−(1−δ)k =AKαf
f N
−αf
f +AB K ψ i L
−ψ αiN −αi
i < =
# Kf Nf $ $ $ $
$ $ $ % (
! " G
4 7
Nf +Ni = 1 < =
Kf +Ki =k < =
L= 1 < :=
# ; k $ $
# " % " " $
6 $ % 4 (
{(ct, kt )}∞t $ % {(Kf t, Nf t)}∞t
( {(Kit, Nit, Lt)}∞t (
4 $ {(rt, wt, qt)}∞t 7
< = {(ct, kt )}∞t % <F= <I= " % $ {(rt, wt, qt)}∞t
" % k H
< ={(Kf t, Nf t)}∞t % < = < = " % $ {(rt, wt, qt)}∞t H
< ={(Kit, Nit, Lt)}∞t % < @= < = < D= " % $ {(rt, wt, qt)}∞t H
< %= 7 < = < = < = < := t
! & ' ( $%
" # (
r = 1
β −(1−δ) < @=
! $
-" % $ %
kf =
Tva−
Tk
Aαf
β
1−(1−δ)β
−αf
< =
ki =ψ
Tk
Tl
αi
αf
1−αf
1−αi
Aαf
T−
va
Tk
β
1−(1−δ)β
−αf
1 # " 4 ; # ( " %
Ni = B
Tl
T−
va
1−αi
1−αf
kψαi
i
kαf
f
−ψ αi
< F=
8 % " %
Nf = 1−Ni
! ( $%
( 4 # $
(& - 4
$ - - kf $ (
$ k "
Niki+ (1−Ni)kf =k < I=
# ki " % < D= Ni " % < F=
"
)
$
! # % " $ $
# & " ! $ δ
% - - $ 0.2 $
0.35 0.95 #
# $ %
$ $ γ + 0 ! % < @=
* "
αf 0.35
αi 0.05
δ 0.04
γ 2.5
! $ ψ ( "" " # $
-$ ! % $
( % $ . % # $
-# &-#34; " " " % $ ψ
% % ψ # $ $ % "
#
% " # % ψ
! $ <A B β= # (
% $ " # $ B
# 4 < I= < = < D= < F= < =
" # % τk= 0.25<# $ & 0.2
$$ $ =: τ
l = 2/3 <# $ & 0.4
$$ = τva = 0.03@ "
# "7 $ - - $ 2.5
0.1 $ " 4 < =
< D= < F= # ( # " 7
Ni =
B Tl
T−
va −αi −αf×
× Tk
Tl
αi
αf −αf
−αiψ Aαf
T−
va
Tk r
−αf ψαi
×
× AαfT
−
va
Tk r
− −αfαf
−ψ αi
< J=
# &$ " # < = < D= < I=
( 4 # ( %
$ A B β ! 4 "
< = < D= < J= < = ! #
% $ ψ
* " + ψ
ψ = 0.1 ψ = 0.3 ψ = 0.5 ψ = 0.7 ψ = 0.9
A F@ F@ F F F
B : F J D
β J@ J@ J@ J@ J@
$ A β $ % #
" % ψ ! : #
:6$$ & C # 4 % # &
& $$
@ + < @= * < =
$ % - - $ % $ ψ
* ( * *, # (
ψ = 0.1 ψ = 0.3 ψ = 0.5 ψ = 0.7 ψ = 0.9
yi/y @ @ @ @ @
χ/y :: :: :: :: ::
# % yi/y χ/y % ψ " 0.1
0.9 ! % # $ % H *
< =
-
.
$
! C ; $ # "
# $ $ β " $
-αi αf 4 B !
# $ 7 A B #
4 < J= < = ! " # "
% C ; 0.2 $
-0.04 ! ) '
0.3 C ; $ 0.4
B & 1 <#
$ & 0.5 $$ = ! @ #
% $ % $ A B C ;
% $ ψ
* " + ψ
ψ = 0.1 ψ = 0.3 ψ = 0.5 ψ = 0.7 ψ = 0.9
A @D @D @D @D @D
B : :F :I @ @
! # % 4 yi/y χ/y k/y
% $ ψ
! * / ( * *, # ( / " # * *, # (
ψ = 0.1 ψ = 0.3 ψ = 0.5 ψ = 0.7 ψ = 0.9
yi/y
χ/y :D :D :D :D :D
k/y J : : :
$$ &
? 4 yi/y χ/y $ % ψ "
0.1 0.9 8 $ - - $ % %
$ ψ
* &
' (
)
$
8 # $
# " &$ E &
τl & % τva %
" % % κ . $ # %
% $
ψ 1 % # % τl
τl τl % "
# Ni # # τl
# * &
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
l
0.08 0.1 0.12 0.14 0.16
I
N
ψ=0.1
ψ=0.3
ψ=0.5ψ=0.7
ψ=0.9
. $ # $ " % τl
$ # τl τva )
" % % ! % $
# # &$ 1
-% # % τl $
# $
-% τl % " $
A # %
$ $
$ $ D
# * , #
0.4 0.6 0.8 1 1.2 1.4 1.6 1.8
l 0.95
0.975 1 1.025
1.05 1.075 1.1 1.125
y
ψ=0.1 ψ=0.3
ψ=0.5 ψ=0.7
ψ=0.9
! % $ &
% &
$ " " % % "- $
B
% τl % "
-
.
$
$ &$ C ; !
% 4 B ! %
-" $ ψ " 0.1 0.9 #
# # ψ = 0.1 ! % Ni #
$ % B 1 % # % τl
D $$ & E # "- 4
τl τva )
" % % τl % "
$$ . $ : #
# * &
0.5 1 1.5 2 2.5
l 0.26
0.28 0.3 0.32 0.34
i
N
ψ=0.1
! $ " # . $ @
" % τl E
B $
#
# * , #
0.5 1 1.5 2 2.5
l
0.4 0.42 0.44 0.46 0.48
y
ψ=0.1
! # B C ;
-" ! $ "
# "
!
*
(
!
)
$
$ % # % ' &$ #
& τl # &
% τva # ) " % % κ
# $ &$
$ # # $ #
$ " "
# ; 4 &$
$ ! ' # # $
" C " #
% ' $ &$
E τl τva % " %
% κ $ k . $ # #
% $
$ % ψ = 0.9 # %
&$ % % $ τl = 2/3
# τl τva )
" % % κ $ k
# ! * &
0 . 4 0 . 4 5 0 . 5 0 . 5 5 0 . 6 0 . 6 5 0 . 7 l
0 . 0 2 5 0 . 0 5 0 . 0 7 5 0 . 1 0 . 1 2 5 0 . 1 5 0 . 1 7 5 0 . 2
I
N
ψ =0 . 1 ψ =0 . 3
ψ =0 . 5
ψ =0 . 7
. $ D # # $$ $ #
$ (& # % $ #
# 0 * , #
0 . 4 0 . 4 5 0 . 5 0 . 5 5 0 . 6 0 . 6 5 0 . 7
l
0 . 9 8 0 . 9 9 1 1 . 0 1 1 . 0 2 1 . 0 3 1 . 0 4
y
ψ =0 . 1
ψ =0 . 3
ψ =0 . 5
ψ =0 . 7
# ( ' B !
$ # # $$
"
!
-
.
$
# C ;
$ # ψ = 0.5 1 $
% &$ % . $ F # %
τl τva )
" % % κ $ k (
$ % B
# 1 * &
0.4 0.5 0.6 0.7 0.8 0.9 1 1.1
l
0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4
i
N
ψ=0.5
. $ I # # $$ $
% $ # # %
# 2 * , #
0.4 0.5 0.6 0.7 0.8 0.9 1 1.1
l
0.4 0.42 0.44 0.46 0.48
y
ψ=0.5
# ( $$ % "
! B C ;
0
3
0
# # % $ $ &$
$ '
"-- $ τl
τva ) " % % κ $ k
" # % ) $$ #
$ " ! #
! F
! # " %
W =
∞
t
βtu(ct)
! $ τl W " %
dW dτl ∗
=
∞
t
βtu´(c∗) dct
dτl ∗
=u´(c∗) ∞
t
βt dct
dτl ∗
! 4 4 " %
ct+kt −(1−δ)kt=yt
u´(ct) =β(1 +rt −δ)u´(ct )
#
yt=Ak
αf
f,t(1−Ni,t) +ABk αiψ
i,t N
−αi −ψ
i,t
ki,t =
1 +τk
1 +τl
αi
αf
1−αf
1−αi
ψkf,t
Ni,t= B
1 +τl
1−τva
1−αi
1−αf
kψαi
i,t k
−αf
f,t
−ψ αi
rt =
1−τva
1 +τk
Aαfk
αf−
f,t
Ni,tki,t+ (1−Ni,t)kf,t =k
% # ki Ni τva τl kf
! 4 4 Ni,tki,t+ (1−Ni,t)kf,t = k (
$ kf k ! # % # y r
k % #
ct+kt −(1−δ)kt=yt(kt, τl)
u´(ct) =β[1 +rt (kt , τl)−δ]u´(ct ) <: =
% # $ τl
dct
dτl ∗+
dkt
dτl ∗ =
∂yt
∂kt ∗+ 1−δ
dkt
dτl ∗+
∂yt
∂τl ∗
dct
dτl ∗−
dct
dτl ∗ = β
u c∗ u c∗
∂rt
∂kt ∗
dkt
dτl ∗+β
u|c∗ u c∗
∂rt
∂τl ∗
<: =
( # "
Cτl(s)≡ ∞
t
st dct
dτl ∗
Kτl(s)≡ ∞
t
st dkt dτl ∗
<::=
# 0< s <1 ?
∞
t
st dct
dτl ∗
= 1
s Cτl(s)−
dc dτl ∗
<:@=
∞
t
st dkt
dτl ∗
= 1
sKτl(s) <: =
dk
dτl ∗ = 0
# $ 4 <: = st # 0 < s <
1 ; ( # # "
4 7
∂yt
∂kt ∗+ 1−δ− s −1
−βu cu c∗∗
∂rt
∂kt ∗ s 1− s
Kτl(s)
Cτl(s)
= − −s ∂yt
∂τl ∗
lhs <:D=
#
lhs= 1
1−sβ u´(c∗)
u´´(c∗)
∂rt
∂τl ∗
− 1
s dc dτl ∗
% Kτl(s) Cτl(s)
Kτl(s) =
1 ∆
1 1−sβ
u´(c∗)
u´´(c∗)
∂rt
∂τl ∗
− 1
s dc dτl ∗
− ∂yt
∂τl ∗
<:F=
Cτl(s) =
1 ∆ ∂yt
∂kt ∗+ 1−δ− s ×
× −sβu cu c∗∗
∂rt
∂τl ∗− s
dc dτl ∗ +
− −s ∂yt
∂τl ∗β
u c∗ u c∗
∂rt
∂kt ∗ s <:I= #
∆≡ ∂yt
∂kt ∗
+ 1−δ− 1
s 1−
1
s − β
u´(c∗)
u´´(c∗)
∂rt
∂kt ∗
1
s
& " % % & & > 1
1 4 # %
&dc dτl
|∗ = β
u´(c∗)
u´´(c∗)
∂rt
∂kt ∗
&Kτl &
− −(1−&)C
τl &
− + &
&−1β
u´(c∗)
u´´(c∗)
∂rt
∂τl ∗
0< &− <1 ! % & # " 4
∂yt
∂kt ∗
+ 1−δ−& (1−&) = βu´(c
∗)
u´´(c∗)
∂rt
∂kt ∗
&
$ " % 4 Kτl(&
− ) "
( 4 # (
(1−&) Cτl &
− − &
&−1
∂yt
∂τl ∗
= βu´(c
∗)
u´´(c∗)
∂rt
∂kt ∗
&Kτl & −
# &$ ) $ $
$ (
dc dτl
|∗ =
1
&−1 β
u´(c∗)
u´´(c∗)
∂rt
∂τl ∗
+ ∂yt
∂τl ∗
# $ τl #
dW dτl ∗
=u´(c∗)Cτl(β) <:J=
( dW
dτl ∗ # $ # " % % 7
∂rt
∂τl ∗
∂rt
∂kt ∗
∂yt
∂τl ∗
∂yt
∂kt ∗ $ $
$ ! 4 4 #
ki(τl, τva, kf) =
1 +τk
1 +τl
αi
αf
1−αf
1−αi
ψkf
Ni(τl, τva, kf) = B
1 +τl
1−τva
1−αi
1−αf
[ki(τl, τva, kf)]ψαik
−αf
f
−ψ αi
Ni(τl, τva, kf)ki(τl, τva, kf) + [1−Ni(τl, τva, kf)]kf =k
! 4 ( kf $ τl, τva k
kf =kf(τl, τva, k) "
C $ 1 ! # (
∂kf
∂τl ∗
=−
∂Ni
∂τl (ki−kf) +Ni
∂ki
∂τl
∂Ni
∂kf (ki−kf) + 1−Ni 1−
∂ki
∂kf ∗
<@ =
∂kf
∂τva ∗
=−
∂Ni
∂τva(ki−kf) +Ni
∂ki
∂τva
∂Ni
∂kf (ki−kf) + 1−Ni 1−
∂ki
∂kf ∗
<@ =
∂kf
∂k ∗ =
1
∂Ni
∂kf (ki−kf) + 1−Ni 1−
∂ki
∂kf ∗
<@ =
# kf " % < =
! " % " #
κ = [1−Ni(τl, τva, kf)]Akαf
f τva+τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf
# kf = kf(τl, τva, k) $ #
-τl τva ) " % % κ
! % 4 ( τva $
τl k τva = τva(τl, k)
" (
H(τl, τva, k) ≡ [1−Ni(τl, τva, kf)]k αf
f A×
× τva+τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf −κ
# kf =kf(τl, τva, k) $ $ % % 7
∂H ∂τl
= −Akαf
f τva+τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf ×
× ∂Ni
∂τl
+ ∂Ni
∂kf
∂kf
∂τl
+
+ (1−Ni)Aαfk αf−
f τva+τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf ×
×∂kf
∂τl
+ (1−Ni)Ak αf
f
(1−τva)
(1 +τl)
∂H
∂τva
= −Akαf
f τva +τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf ×
× ∂Ni
∂τva
+ ∂Ni
∂kf
∂kf
∂τva
+
+ (1−Ni)Aαfk αf−
f τva+τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf ×
×∂kf
∂τva
+Akαf
f (1−Ni)×
× 1−τl
1−αf
1 +τl
−τk
αf
1 +τk
∂H
∂k = τva+τl
1−τva
1 +τl
(1−αf) +τk
1−τva
1 +τk
αf Ak
αf
f
∂kf
∂k (1−Ni)αfk
−
f −
∂Ni
∂kf
C $ 1 ! # (
∂τva
∂τl ∗
=−
∂H ∂τl ∗
∂H ∂τva ∗
<@:=
∂τva
∂k ∗ =−
∂H ∂k ∗
∂H ∂τva ∗
<@@=
# kf " % < =
# $ % % ∂r
∂k ∗
∂r ∂τl ∗
∂yt
∂τl ∗
∂y ∂k ∗
1 4 4 < = # (
∂r
∂k ∗ = −
1 1 +τk
∂τva
∂k Aαfk
αf−
f
∗
+
− 1−τva
1 +τk
Aαf(1−αf)k
αf−
f ∂kf ∂k + ∂kf ∂τva ∂τva
∂k ∗ <@ =
∂r ∂τl ∗
= − 1
1 +τk
∂τva
∂τl
Aαfk
αf−
f
∗
+
− 1−τva
1 +τk
Aαf (1−αf)k
αf−
f
∂kf
∂τl
+ ∂kf
∂τva
∂τva
∂τl ∗
<@D=
# kf " % < =
! $ dydk ∗ ∂τ∂y
l ∗ $ " %
y(τl, τva, k) = Ak αf
f [1−Ni(τl, τva, kf)] +
+AB[ki(τl, τva, kf)] αiψ[N
i(τl, τva, kf)] − αi −ψ
# kf = kf (τl, τva, k) $ ( % !
% % y # $ k τl % " %
∂y
∂k ∗ = Aαfk
αf−
f (1−Ni)
∂kf
∂k +
∂kf
∂τva
∂τva
∂k ∗+
−Akαf
f ∂Ni ∂τva ∂τva ∂k + ∂Ni ∂kf ∂kf ∂k + ∂kf ∂τva ∂τva
∂k ∗+
+ABαiψk αiψ−
i N
−αi −ψ
i ×
× ∂ki
∂τva ∂τva ∂k + ∂ki ∂kf ∂kf ∂k + ∂kf ∂τva ∂τva
∂k ∗+
+AB[1−αi(1−ψ)]kiαiψN
−αi −ψ
i ×
× ∂Ni
∂τva ∂τva ∂k + ∂Ni ∂kf ∂kf ∂k + ∂kf ∂τva ∂τva
∂k ∗ <@F=
∂y ∂τl ∗
= Aαfk αf−
f (1−Ni)
∂kf
∂τl
+ ∂kf
∂τva
∂τva
∂τl ∗
+
−Akαf
f
∂Ni
∂τl
+ ∂Ni
∂τva
∂τva
∂τl
+∂Ni
∂kf
∂kf
∂τl
+ ∂kf
∂τva
∂τva
∂τl ∗
+ +ABαiψkαiiψ− N
−αi −ψ
i ×
× ∂ki
∂τl
+ ∂ki
∂τva
∂τva
∂τl
+ ∂ki
∂kf
∂kf
∂τl
+ ∂kf
∂τva
∂τva
∂τl ∗
+ +AB[1−αi(1−ψ)]kiαiψN
−αi −ψ
i ×
× ∂Ni
∂τl
+ ∂Ni
∂τva
∂τva
∂τl
+∂Ni
∂kf
∂kf
∂τl
+ ∂kf
∂τva
∂τva
∂τl ∗
<@I=
# kf " % < =
0
4
(
# $ % dW
dτl ∗ ' $ (τl, τva)
! $ # 7 # τl% )
τva " % % ? $
(τl, τva) ( ' ! "
" % %
0 ) $
. $ J # % dW
dτl ∗ ' $ (τl, τva)# ψ = 0.1
I
! # # τl !
( $ (τl, τva)
. $ J - 6 7 B * <ψ .=
0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 l
-160 -140 -120 -100 -80 -60
W
d
d
l
6$$ & * # # ψ = 0.9 % % dW
dτl ∗
$ % " τl # ! % ψ = 0.9
$ % " $ "
$ 1 %
ψ # ( " % % dW
dτl ∗ $ (τl, τva)
$ & &
I 6$$ & * # # % ψ
% $ " " % % #
0 - . $
. $ # % dWdτ
l ∗ ' $ (τl, τva)# ψ = 0.1
! # # τl !
( $ (τl, τva)
. $ - 6 7 C ; * <ψ . =
0.8 0.9 1 1.1 1.2 1.3 1.4 l
-370 -360 -350 -340
W
d
d
l
! # % B
C ; 7 &
% & %
$ " % %
1
"
" # % $ &$ " τl
) "τva " % %
$ " % $ ψ
% " % τl C
# % τl # %
# $ (& # % #
$ # ! B
C ;
6 " # % $$ " 4
-# # # # τl ! $ $
& &
% " % %
#
2
-
'
#
C + + 9 K - " E $ 6
-L *+.*-1.2 @
* 1 K # * 7 ;
E E 4 L 2 MMM2
: 1 * N O
-+ K " " . " A 7 B > 6
%-DJ E L FD $ " @ J-@J:
@ A . + * # K #L
% J ? @ $ " - F
N K6 % - E $ +
-1 " L JI
D N K! E 1 ! & +
-1 " L J JIF
F + * # K 6 !
* $ PL %
I ? @
I + 0 E ! % $ K -C 8$
! & E $ % $ " * L
B % " @
J " KC E $ 6 6"" "
! 1 + % L ! % @ ?
1 @
6$$
& 6 - !
6 #
8$
# " # $ % " % τva = τl = τk = 0% " &Yi >0'(
! ( (
% # " ; $ 7
min
Ki,Ni
{rKi+wNi+q}
s.t Yi =ABK
ψαi
i N
−αi
i
! " " $ " %
L(Ki, Ni, λ) =rKi+wNi+q−λ ABKiψαiN
−αi
i −Yi
( " %
∂L
∂Ki
= r−λψαiABK ψαi−
i N
−αi
i = 0
∂L ∂Ni
= w−λ(1−αi)ABKiψαiN
−αi
i = 0
∂L
∂λ = − ABK
ψαi
i N
−αi
i −Yi = 0
#
Ki
Ni
= w
r ψαi
(1−αi)
" %
Ni(w, r, Yi) =
w r
ψαi
(1−αi)
− −αiψαi−ψ
(AB)− −αi −ψ Y −αi −ψ
i
Ki(w, r, Yi) =
w r
ψαi
(1−αi)
−αi −αi −ψ
(AB)− −αi −ψ Y −αi −ψ
i
! # " 7
ci(w, r, Yi) = w
−αi −αi −ψ r
ψαi
−αi −ψ ×
× ψαi
1−αi
− −αiψαi−ψ
+ ψαi 1−αi
−αi −αi −ψ
×
×(AB)− −αi −ψ Y −αi −ψ
i +q
(
ai ≡w
−αi −αi −ψ r
ψαi
−αi −ψ
ψαi −αi
− −αiψαi−ψ
+ + ψαi
−αi
−αi −αi −ψ
(AB)− −αi −ψ
! #
ci(w, r, Yi) =aiY
−αi −ψ
i +q <@J=
# " " %
cmgi(Yi)≡
∂ci(w, r, Yi)
∂Yi
= 1
1−αi(1−ψ)
aiY
αi −ψ
−αi −ψ
i < =
( (
min
Ki,Ni
{rKf +wNf}
s.a Yf =AK
αf
f N
−αf
f
! " " ; $ " %
L(Ki, Ni, λ) =rKf +wNf −λ AK
αf
f N
−αf
f −Yf
! ( " %
∂L
∂Kf
= r−λαfAK αf−
f N
−αf
f = 0
∂L
∂Nf
= w−λ(1−αf)AK αf
f N
−αf
f = 0
∂L
∂λ = − AK
αf
f N
−αf
f −Yf = 0
#
Kf
Nf
= w
r αf
(1−αf)
" %
Nf(w, r, Yf) =A−
w r
−αf αf
1−αf
−αf
Yf
Kf(w, r, Yf) = A−
w r
−αf αf
1−αf
−αf
Yf
! # " 7
cf(w, r, Yf) =A− w −αfrαf
αf
1−αf
−αf
+ αf 1−αf
−αf
Yf
( af ≡A− w −αfrαf αf −αf
−αf
+ αf −αf
−αf
-( #
cf(w, r, Yf) =afYf < =
A ( <$ % = " 7 cmgf(Yf)≡
∂cf(w,r,Yf)
∂Yf =af >0 # % Yi cmgi(Yi)<
af Yi ∈(0, Yi) cmgi(Yi) "
(0,∞) limYi→ cmgi(Yi) = 0 ! $ ( $
6$$
& C - *4 %
C #
! &
1
! &
$$
1
# 4 % # & $
& $$ $ <
$ % $$ = E
# # $ # &
$ % $$
! G $ # # " # 7
max
{(ct,ki,t ,kf,t ,ni,t,nf,t,Lt)}
∞
t ∞
t
βtu(ct)
s.t
ct+ki,t +kf,t = (1−τls)wf,tnf,t+wi,tni,t+
(1−τs
k)rf,tkf,t+ri,tki,t+ (1−δ) (ki,t+kf,t) +qtLt+κt
ki,t+kf,t=kt
ni,t+nf,t = 1
ct, ki,t , kf,t , ni,t, nf,t 0 0 Lt 1 t
k >0 " %
! C 4 $
v(k) =
maxc,h,nf,kf logc+βv(h)
s.t
c+h= (1−τs
l)wfnf +wi(1−nf) +
(1−τs
k)rfkf +ri(k−kf) + (1−δ)k+q+χ
c 0, h 0,0 kf k, 0 nf 1
! ( * % $ " %
1
c(k) =βv
′(g(k))
1
c(k)[(1−τ
s
k)rf −ri] = 0
1
c(k)[(1−τ
s
l)wf −wi] = 0
v′(k) = 1
c(k)[(1−δ) +ri]
! * 4
1
c(k) =β
1
c(g(k))[(1−δ) +r
′
i]
(1−τs
k)rf = ri (1−τsl)wf = wi (
" $ $
1 $ ( & ; $ $ % (
#
wf =A(1−αf)K
αf
f N
−αf
f
rf =AαfK
αf−
f N
−αf
f
1 $ ( & ; $ $ % (
#
wi =AB(1−αi) KiψL −
ψ αi
N−αi
i
ri =ABαiψ KiψL
−ψ αiN −αi
i K
−
i
q =ABαi(1−ψ) KiψL −
ψ αi
N −αi
ii L−
4 # % # " 7
AB(1−αi) K
ψ i L −ψ
αi
N−αi
i = (1−τsl)A(1−αf)K αf
f N
−αf
f
ABαiψ KiψL −
ψ αiN −αi
i Ki− = (1−τ s
k)AαfK αf−
f N
−αf
f
! $ % # " #
$ - - 7
1−αi
αiψ
Ki
Ni
= 1−τ
s l
1−τs k
1−αf
αf
Kf
Nf
< =
# 1− τs
k = τk 1 −τ
s
l = τl # 4
< I= ! 4 % # &
& $$
6$$
& E -
"
6
% # $ - - "
τva τl A # ( kf : (0,1)×(0,∞)→R
kf (τva, τl) = A
1−τva
1 +τk
αf
β
1−(1−δ)β
−αf
ki : (0,1)×(0,∞)→R
ki(τva, τl) =
1 +τk
1 +τl
αi
αf
1−αf
1−αi
ψ 1−τva
1 +τk
Aαf
β
1−(1−δ)β
−αf
r= β −(1−δ) ! # % # "
∂kf
∂τl
= 0
∂kf
∂τva
=− αf
1−αf
1 1 +τk
1
rAk
αf
f <0
∂ki
∂τl
=− 1
1 +τl
ki <0
∂ki
∂τva
=−ki
kf
αf
1−αf
1 1 +τk
1
rAk
αf
f <0
(τva, τl)∈(0,1)×(0,∞) ( Ni
τva τl Ni : (0,1)×(0,∞)→R " %
Ni(τva, τl) =
1 +τl
1−τva
B1−αi
1−αf
kψαi
i k
−αf
f
−ψ αi
# kf = kf(τva, τl) ki = ki(τva, τl) ( $
% % Ni
∂Ni
∂τva = −ψ αi B
τl −τva
−αi −αfk
ψαi
i k
−αf
f
−ψ αi ×
× −τva +ψαik
−
i ∂ki
∂τva+
−αfk−f
∂kf
∂τva
−ψ αi
τl −τvaB
−αi −αfk
ψαi
i k
−αf
f
−ψ αi
$ %
# - "
% % ∂Ni
∂τva ? # # # " # 7
−τva +ψαik −
i ∂ki
∂τva −αfk −
f ∂kf
∂τva = −τva +
αf −αf τk
A rk
αf−
f (αf −ψαi)
αf −ψαi > 0 % % ∂τ∂Ni
va $ % ?
$ $
$ %
∂Ni
∂τl = −ψ αi B
τl −τva
−αi −αfk
ψαi
i k
−αf
f
−αi −ψ
−ψ αi ×
×B −τ
va −αi −αf k
ψαi
i k
−αf
f 1 +ψαi(1 +τl)k
−
i ∂k∂τil
#
1 +ψαi(1 +τl)ki−
∂ki
∂τl
= 1−ψαi
0 < ψαi < 1 # ∂N∂τi
l > 0 ! Ni
" τva τl 8 % Nf : (0,1)×(0,∞) → R
(
Nf(τva, τl) = 1−Ni(τva, τl)
" τva τl
6 # % # $
τva τl ( Kf : (0,1)×(0,∞) → R Ki :
(0,1)×(0,∞)→R
Kf(τva, τl) =Nf(τva, τl)kf (τva, τl)
Ki(τva, τl) =Ni(τva, τl)ki(τva, τl)
$ % ! $ % % " %
∂Kf
∂τl
=kf
∂Nf
∂τl
<0
∂Kf
∂τva
=Nf
∂kf
∂τva
+kf
∂Nf
∂τva
<0
∂Ki
∂τl
=Ni
∂ki
∂τl
+ki
∂Ni
∂τl
∂Ki
∂τva
=Ni
∂ki
∂τva
+ki
∂Ni
∂τva
? " % % ∂Ki
∂τl
∂Ki
∂τva "
6$$
&
- !
8 $
C ;
*
0.4B *
Kus "" " $ B E
" $ $
hus % " " B ! $ " %
Yus = [Aexp (φhus)Lus] − α
Kusα
# A ' % Lus # (
yus ≡
Yus
Lus
%
ybrexp (φhbr)
yusexp (φhus)
= 0.2
exp [φ(hus−hbr)] 2 # ( ybr/yus
0.4
6$$
& * -
ψ = 0.3 ψ = 0.5 ψ = 0.7ψ = 0.9 ψ = 0.95
# % dW
dτl ∗ % $ ψ
. $ : @ B . $ D F I
J C ;
. $ - 6 7 B * <ψ . =
0.6 0.7 0.8 0.9 1 1.1 1.2 1.3
l -80
-70 -60 -50 -40
W
d
d
l
. $ - 6 7 B * <ψ . =
0.6 0.7 0.8 0.9 1 1.1 1.2 1.3
l -60
-55 -50 -45 -40
W
d
d
l
. $ : - 6 7 B * <ψ . =
0.6 0.7 0.8 0.9 1 1.1 1.2 1.3
l -54
-52 -50 -48 -46 -44 -42 -40
W
d
d
l
. $ @ - 6 7 B * <ψ . =
0.6 0.7 0.8 0.9 1 1.1 1.2 1.3
l 0
25 50 75 100 125 150
W
d
d
l
. $ - 6 7 B * <ψ . =
0.6 0.7 0.8 0.9 1 1.1
l -10
-7.5 -5 -2.5 0 2.5 5
W
d
d
l
. $ D - 6 7 C ; * <ψ . =
0.8 0.9 1 1.1 1.2 1.3 1.4
l -390
-385 -380 -375
W
d
d
l
. $ F - 6 7 C ; * <ψ . =
0.8 0.9 1 1.1 1.2 1.3 1.4
l -4000
-3000 -2000 -1000 0
W
d
d
l
. $ I - 6 7 C ; * <ψ . =
0.8 0.9 1 1.1 1.2 1.3 1.4
l -120
-110 -100 -90 -80 -70
W
d
d
l
. $ J - 6 7 C ; * <ψ . =
0.8 0.9 1 1.1 1.2 1.3 1.4
l -200
-190 -180 -170 -160 -150 -140
W
d
d
l
. $ - 6 7 C ; * <ψ . =
0.6 0.7 0.8 0.9 1 1.1
l -230
-220 -210 -200 -190 -180
W
d
d
l