¨o
∂u
∂t
= a
∂
2
u
∂x
2
(x, t) ∈ (−∞; +∞) × (0; 1),
u(·, 1) − ϕ(·) ε,
u(·, 0)
H
s
(R)
E, ϕ(·) ∈ L
2
(R) E > ε > 0
s 0 a > 0
1.
¨o
∂u
∂t
= a
∂
−
s = 0 s = 0 H
s
(R) = H
0
(R) =
L
2
(R)
s s 0
1
v(x, t) ∈ L
2
(R) t ∈ [0; 1+β]
∂v
∂t
= a
∂
2
v
∂x
2
(x, t) ∈ (−∞; +∞) × (0; 1 + β),
αv(x, 0) + v (x, 1 + β) = ϕ(x), x ∈ (−∞; +∞), α > 0, β > 0
(1.3)
−
¨o
1
√
2π
+∞
−∞
e
−ix.ξ
f(x)dx (y ∈ R)
f
f
∨
(ξ) :=
1
√
2π
+∞
−∞
e
ix.ξ
f(x)dx (y ∈ R).
2.2 ( f ∈ L
1
(R) ∩ L
2
(R)
f, f
∨
f
k
−
f
j
=
f
k
− f
j
= f
k
− f
j
{
f
k
}
∞
k=1
L
2
(R)
f
k
D
α
f = (iξ)
α
f α D
α
f ∈ L
2
(R)
f ∗g =
√
2π
fg
f = (
f)
∨
.
2.4 f ∈ H
s
(R) f
f
H
s
(R)
:=
1 − x
y
e
1−x−y
. (2.3)
2.4 x, y z
x + zy (z + 1)x
1/(z+1)
y
z/(z+1)
.
2.5 0 p q < ∞, q = 0 α > 0
αe
−p
α + e
−q
H
p
q
α
p
q
.
p = 0 p = q
0 < p < q < ∞
x = α, z =
p
q
α
1−
p
q
e
−p
.
2.6 u(x, t) ∈ L
2
(R) t ∈ [0; 1]
∂u
∂t
= a
∂
2
u
∂x
2
, (x, t) ∈ (−∞; +∞) × (0; 1). (2.4)
u(·, t) u(·, 1)
t
u(·, 0)
1−t
, t ∈ [0; 1]
u(x, t)
∂u
∂t
2
u(ξ, 1), ξ ∈ R, (2.8)
u(ξ, 1) = e
−aξ
2
u(ξ, 0), ξ ∈ R. (2.9)
u(ξ, t) = e
−atξ
2
u(ξ, 0), (ξ, t) ∈ R ×[0, 1]. (2.10)
|u(ξ, t)|
(1−t)
= e
−at(1−t)ξ
2
|u(ξ, 0)|
(1−t)
, (ξ, t) ∈ R × [0, 1]. (2.11)
|u(ξ, t)| = |u(ξ, 1)|
t
|u(ξ, 0)|
(1−t)
, ξ ∈ R.
t = 0 t = 1
t ∈ (0, 1)
p =
1
t
, q =
1
−∞
|f(ξ)g(ξ)|dξ = f g
1
f
p
g
q
=
+∞
−∞
|f(ξ)|
p
dξ
t
.
+∞
−∞
|g(ξ)|
q
dξ
(1−t)
=
2
(x, t) −
t ∈ [0, 1]
u
1
(·, t) − u
2
(·, t) 2C
1
(t, a, s, β)ε
t
E
1−t
ln
E
ε
−
s
2
(1−t)
(1 + o(1)), ε → 0
+
,
C
1
(t, a, s, β) =
1 + C(a, β, s)a
a(1 + β)
ln
1
α
s/2
E + α
t+β
1+β
−1
ε, ∀t ∈ [0, 1], ∀α ∈ (0, 1).
α =
ε
E
ln
E
ε
s
2
1+β
,
t ∈ [0; 1]
u(·, t) − v
α
(·, t + β) C
2
(1 + o(1)), ε → 0
+
.
s > 0
3.4 ε < ϕ(·) τ > 1 τ ε < ϕ(·)
α
ε
> 0
v
α
ε
(·, 1 + β) − ϕ(·) = τε. (3.1)
u(x, t) v
α
(x, t)
α = α
ε
. t ∈ [0, 1]
u(·, t) − v
α
ε
(·, t + β)
C(τ, a, β, s)ε
t
E
1−t
ln
dv
dt
= −aξ
2
v, 0 < t < 1 + β,
αv(ξ, 0) + v(ξ, 1 + β) = ϕ(ξ), ξ ∈ (−∞; +∞), α > 0, β > 0.
(4.1)
v(ξ, t) = e
−atξ
2
v(ξ, 0), ∀t ∈ [0, 1 + β]. (4.2)
t = 1 + β v(ξ, 1 + β) = e
−a(1+β)ξ
2
v(ξ, 0), ϕ(ξ) = αv(ξ, 0) +
v(ξ, 1 + β) = (α + e
−a(1+β)ξ
2
)v(ξ, 0)
v(ξ, 0) =
ϕ(ξ)
α + e
−a(1+β)ξ
2
. (4.3)
v(ξ, t) =
e
−atξ
2
. (4.6)
|
F | =
F =
e
−atξ
2
α + e
−a(1+β)ξ
2
H
t
1 + β
α
t
1+β
−1
, ∀t ∈ [0, 1 + β]. (4.7)
v(·, t) =
F ϕ
1+β
−1
ϕ
v(·, t) H
t
1 + β
α
t
1+β
−1
ϕ, ∀t ∈ [0, 1 + β]. (4.8)
u(·, t) − v
α
(·, t + β) = u(·, t) − v
α
(·, t + β)
=
e
a(1−t)ξ
2
u(ξ, 1) −
e
2
α + e
−a(1+β)ξ
2
(u(ξ, 1) − ϕ(ξ))
e
a(1−t)ξ
2
−
e
−a(t+β)ξ
2
α + e
−a(1+β)ξ
2
u(ξ, 1)
2
α + e
−a(1+β)ξ
2
u(ξ, 1)
+ sup
ξ∈R
e
−a(t+β)ξ
2
α + e
−a(1+β)ξ
2
u(ξ, 1) − ϕ(ξ)
=
αe
−atξ
2
α + e
−a(1+β)ξ
−a(1+β)ξ
2
(1 + ξ
2
)
s/2
u(ξ, 0)
+ H
t + β
1 + β
α
t+β
1+β
−1
ε
sup
ξ∈R
αe
−atξ
2
(1 + ξ
2
)
t+β
1+β
−1
ε. (4.9)
A = sup
ξ∈R
αe
−atξ
2
(1 + ξ
2
)
−s/2
α + e
−a(1+β)ξ
2
. e
−a(1+β)ξ
2
= αz
0 < z
1
α
αe
−atξ
2
(1 + ξ
2
)
−s/2
a(1 + β)
ln
1
α
s/2
z
t
1+β
(1 + z)
−ln α
−ln(αz) + a(1 + β)
s/2
= α
t
1+β
a(1 + β)
ln
1
α
s/2
z
t
1+β
(1 + z)
1+β
(1 + z)
< 1.
z > 1
0 <
−ln α
−ln α − ln z + a(1 + β)
< 1 +
ln z
a(1 + β)
. (4.10)
0 < a(1 + β) −
ln z
a(1 + β)
ln(αz) = a(1 + β) + ξ
2
ln z. (4.11)
z > 1
z > 1
B =
z
t
1+β
(1 + z)
−ln α
−ln α − ln z + a(1 + β)
s/2
<
a(1 + β)
s/2
= z
−β
1+β
ln(e
a(1+β)
z)
a(1 + β)
s/2
= e
aβ
1
a(1 + β)
s/2
(e
a(1+β)
z)
−β
1+β
ln(e
a(1+β)
z)
z > e
a(1+β)
> 1
g(y) y > 1
g
(y) =
−β
1 + β
y
−β
1+β
−1
(ln y)
s/2
+ y
−β
1+β
s
2
(ln y)
s
2
−1
1
y
= y
−β
1+β
−1
s(1+β)
2eβ
s/2
s > 0
B max
1, e
aβ
= e
aβ
s = 0,
B max
1, e
aβ
s
2aeβ
s/2
s > 0.
A C(a, β, s)α
t
1+β
a(1 + β)
ε
s
2
1+β
u(·, t) − v
α
(·, t + β) ε
t
E
1−t
ln
E
ε
−
s
2
(1−t)
1 + C(a, β, s)a
s
2
ln
E
ε
2
(1 + o(1)) ε → 0
+
lim
→0
+
ln
E
ε
ln
E
ε
−
s
2
ln ln
E
ε
s
2
= 1.
ρ(α) = v
α
(·, 1 + β) − ϕ 0 < ε < ϕ
ρ
=
−
α
α + e
−a(1+β)ξ
2
ϕ(ξ)
=
α
α + e
−a(1+β)ξ
2
ϕ(ξ)
dξ n
δ
|ξ|>n
δ
|ϕ(ξ)|
2
dξ <
δ
2
2
α
0 < α <
δ
√
2ϕ
e
−a(1+β)n
2
δ
ρ
2
(α) =
+∞
−∞
α
α + e
−a(1+β)ξ
|ϕ(ξ)|
2
dξ
|ξ|n
δ
α
α + e
−a(1+β)n
2
δ
2
|ϕ(ξ)|
2
dξ +
|ξ|>n
δ
|ϕ(ξ)|
2
dξ
α
2
e
2a(1+β)n
2
δ
ϕ
2
+
δ
2
2
< δ
2
.
lim
α→0
+
ρ(α) = 0
ρ
2
(α) =
+∞
−∞
α
α + e
−a(1+β)ξ
2
2
|ϕ(ξ)|
2
dξ
2
|ϕ(ξ)|
2
dξ
=
α
α + 1
2
ϕ
2
. (4.14)
ρ(α)
α
α + 1
ϕ ρ(α) ϕ. lim
α→+∞
α
α + 1
ϕ =
ϕ lim
α→+∞
ρ(α) = ϕ.
0 < α
1
< α
2
ρ(α
1
+n
0
−n
0
|ϕ(ξ)|
2
dξ > 0. (4.16)
ρ(α
1
) < ρ(α
2
)
α
0
ρ α
0
α
0
> 0 ϕ > 0 ρ
2
(α
0
) > 0
ρ(α
0
) > 0 ρ(α
0
) α
ρ(α
−
α
0
α
0
+ e
−a(1+β)ξ
2
2
|ϕ(ξ)|
2
dξ. (4.17)
α
α + e
−a(1+β)ξ
2
0
+ e
−a(1+β)ξ
2
α
α + e
−a(1+β)ξ
2
+
α
0
α
0
+ e
−a(1+β)ξ
2
2
(α + e
−a(1+β)ξ
2
)(α
0
+ e
−a(1+β)ξ
2
)
2
|α − α
0
|
αα
0
, ∀n ∈ N
∗
. (4.18)
ρ(α
0
)|ρ(α) − ρ(α
0
)| 2
|α − α
0
.
lim
α→α
0
2
|α − α
0
|
αα
0
ρ(α
0
)
ϕ
2
= 0 lim
α→α
0
|ρ(α) −
ρ(α
0
)| = 0 lim
α→α
0
ρ(α) = ρ(α
0
) ρ α
0
ρ α
ε
e
aξ
2
u(ξ, 1) −
e
−aβξ
2
α
ε
+ e
−a(1+β)ξ
2
ϕ(ξ)
=
e
aξ
2
u(ξ, 1) −
e
aξ
2
−
e
−aβξ
2
α
ε
+ e
−a(1+β)ξ
2
u(ξ, 1)
+
e
−aβξ
2
α
ε
+ sup
ξ∈R
e
−aβξ
2
α
ε
+ e
−a(1+β)ξ
2
u(ξ, 1) − ϕ(ξ)
=
α
ε
α
ε
+ e
−a(1+β)ξ
2
u(ξ, 0)
+ sup
s/2
u(ξ, 0)
+ H
β
1 + β
α
−1
1+β
ε
ε
sup
ξ∈R
α
ε
(1 + ξ
2
)
−s/2
α
ε
+ e
−a(1+β)ξ
2
ε. (4.21)
A t = 0
sup
ξ∈R
α
ε
(1 + ξ
2
)
−s/2
α
ε
+ e
−a(1+β)ξ
2
C
2
(a, β, s)
a(1 + β)
ln
1
α
ε
s/2
(4.22)
C
2
(a, β, s) =
ε
ε (4.24)
α
α
ε
+ e
−a(1+β)ξ
2
u(ξ, 1)
− ( ϕ − v
α
ε
(ξ, 1 + β))
=
−a(1+β)ξ
2
u(ξ, 1)
−
1
α
ε
+ e
−a(1+β)ξ
2
ϕ
=
α
ε
α
ε
+ e
−a(1+β)ξ
2
(u(ξ, 1) − ϕ)
+
α
ε
α
ε
+ e
−a(1+β)ξ
2
u(ξ, 1)
− ( ϕ − v
α
ε
(ξ, 1 + β))
. (4.25)
z(·, 0) C
2
(a, β, s)
a(1 + β)
ln
1
α
ε
s/2
E + α
−1
1+β
ε
1
τ −1
α
ε
α
ε
+ e
−a(1+β)ξ
e
−aξ
2
α
ε
+ e
−a(1+β)ξ
2
u(ξ, 0)
C
2
(a, β, s)
a(1 + β)
ln
1
α
ε
s/2
E + α
−1
1+β
ε
1
s/2
E
(τε)
2
= v
α
ε
(·, 1 + β) − ϕ
2
= v
α
ε
(·, 1 + β) − ϕ
2
=
α
ε
α
ε
+ e
−a(1+β)ξ
2
ϕ
+ 1
ϕ
ε
α
ε
ϕ − τε
τ
(4.26)
a(1 + β)
ln
1
α
ε
=
a(1 + β)
ln
E
ε
ε
α
ε
1
E
a(1 + β)
ln
ε
ln
E
ε
ϕ − τε
τ
1
E
= 1. (4.28)
ε → 0
+
z(·, 0)
C
2
(a, β, s) +
1
τ −1
C(a, β, s)
a(1 + β)
ln
E
ε
s/2
E(1 + o(1)). (4.29)
C(a, β, s)
1−t
.
C(τ, a, β, s) = sup
t∈[0,1]
C
3
(τ, t, a, β, s) < +∞
[1] K. A. Ames and B. Straughan, Aca-
demic Press, San Diego, 1997.
[2] Dinh Nho Hao,
, Journal of Mathematical Analysis and Applications, (1996),
873-909.
[3] Dinh Nho H`ao, Nguyen Van Duc and D. Lesnic,
, Inverse problems, 25 (2009),055002,
27pp.
[4] , ,
¨o
∂u
∂t
= a
∂
2
u