(1)

(2)

+

t

(3)

t

(4)

d

d

d

ρ

ρ

t

ε

ε

ε

ε

ε

ε

t

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

ε

(5)

ε

ε

ε

ε

ε

ε

ε

ε

ρ

ε

ε

ρ

ε

t∈

ε

L2

ε

nε

nε

nε

(6)

nε

{ρ≥ε2}

n+1ε

{ρ<ε2}

A

n+1ε

nε

n

nε

n+1ε

n+1ε

n+1ε

εn

εn

n+1ε

n+1ε

n+1ε

εn

εn

εn

εn

εn

n

k=1

k

n

k=1

k

εn

ρ ε2

n

ρ ε2

n

n+1

n+1ε

εn

n

k=1

k−

n

(7)

nε

nε

{ρ≥ε2}

nε

{ρ<ε2}

nε

n+1ε

εn

εn

n

n−

k=1

k

εn

ε

ε

nε

n

ε

ε

nε

n

ε

ε

nε

nε

nε

nε

nε

nε

nε

nε

′′

nε

nε

nε

nε

{ρ≥ε2}

n−

n−

k=0

k

{ρ<ε2}

nε

nε

|z2|2

|z1|2

nε

|z2|2

|z1|2

n−

n

k=0

|z2|2

|z1|2

k

(8)

n−

k=0

nε

nε

nε

nε

nε

nε

nε

nε

nε

nε

nε

nε

nε

{ρ≥ε2}

n−

n

k=0

k

{ρ<ε2}

{ρ≥ε2}

n−

n

{ρ<ε2}

{ρ<ε2}

n−

nε

nε

{ρ≥ε2}

n−

n−

k=0

k

{ρ<ε2}

(9)

nε

′′

{ρ≥ε2}

n−

n

k=0

k

{ρ<ε2}

nε

nε

′′

n

k=0

nε

n

n

k=1

k

n−

k=1

n

k=2

nε

nε

ε

ε

nε

nε

ε

ε

nε

nε

nε

nε

nε

nε

t

δEnε

δu

t

ε

ε

ε

nε

ε

ε

nε

(10)

d

α

α

d

α

d

L2α

α

L2

Rd

d

ε

(11)

ε

L

1

H1

ε

ε

L

2

H2

d

α

(12)

ε

d

α

ε

L

1

H1

ε

L

2α

H1

L2α

d

ε

d

ε

L

2

H2

L2α

d

ε

d

ε

ε

ε

(13)

′′

ε

ε

L2

L2

j

t

j

ε

j

ε

nε

ε

ε

nε

ε

ε

j

ε

j

ε

j

ε

L2

j

ε

L2

nε

(14)

n

′′

j

t

t

ε

L2

t

ε

L2

|λ||t|

t

ε|t=0

nε

nε

δ/2

t

ε

L2

H2

L2−2δδ

H1

L2−2δ

L2

δ/(2

ε

d

α

ε

L2α

Rd

ε

ε

ε

L2

Rd

ε

L2

Rd

α

ε

L2

d

ε

L2

d

(15)

Rd

L2

d

dδ/α

α

dδ/αL2

d

2

2

1

{|

ε|

}

2

|

ε|

2

|

ε|

2

|

ε|

2

|

ε|2

2

|

ε|

2

|

ε|2

2

1

2

|

ε|2

2

1

2

1

(16)

2

2

Rd

4+d4

1

Rd

4+d2

22

2

Rd

1

2

1

2

2

1

2

22

2

4−d4+d

2d 4+d

22

α

|

0

x

|

|

0

x

|

2

|

0

x

|2

2

|

0

x

|2

2

α

α

(17)

2

2

α

α

(18)

nε

|

0|2

s

s

2

2

1

1

2

2

nε

|

0|

2

nε

|

|

2

nε

|

|

2

nε

|

|

2

nε

|

|2

nε

|

|2

2

2

2

2

1

1

1

1

2

(19)

2

1

2

2

2

2

2

2

2

2

1

1

1

1

1

1

1

(20)

1

0

k

kH1

2

1

1

2

1

2

2

1

1

nε

|

|2

2

2

nε

|

|2

1

1

2

2

1

2

2

1

1

1

0

1

2

2

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