In the theory of partial differential equations, a partial differential operator
P
{\displaystyle P}
defined on an open subset
-
U
⊂
R
n
{\displaystyle U\subset {\mathbb {R} }^{n}}
is called hypoelliptic if for every distribution
u
{\displaystyle u}
defined on an open subset
V
⊂
U
{\displaystyle V\subset U}
such that
P
u
{\displaystyle Pu}
is
C
∞
{\displaystyle C^{\infty }}
(smooth),
u
{\displaystyle u}
must also be
C
∞
{\displaystyle C^{\infty }}
.
If this assertion holds with
C
∞
{\displaystyle C^{\infty }}
replaced by real-analytic, then
P
{\displaystyle P}
is said to be analytically hypoelliptic.
Every elliptic operator with
C
∞
{\displaystyle C^{\infty }}
coefficients is hypoelliptic. In particular, the Laplacian is an example of a hypoelliptic operator (the Laplacian is also analytically hypoelliptic). In addition, the operator for the heat equation (
P
(
u
)
=
u
t
−
k
Δ
u
{\displaystyle P(u)=u_{t}-k\,\Delta u\,}
)
-
P
=
∂
t
−
k
Δ
x
{\displaystyle P=\partial _{t}-k\,\Delta _{x}\,}
(where
k
>
0
{\displaystyle k>0}
) is hypoelliptic but not elliptic. However, the operator for the wave equation (
P
(
u
)
=
u
t
t
−
c
2
Δ
u
{\displaystyle P(u)=u_{tt}-c^{2}\,\Delta u\,}
)
-
P
=
∂
t
2
−
c
2
Δ
x
{\displaystyle P=\partial _{t}^{2}-c^{2}\,\Delta _{x}\,}
(where
c
≠
0
{\displaystyle c\neq 0}
) is not hypoelliptic.
References
- Shimakura, Norio (1992). Partial differential operators of elliptic type: translated by Norio Shimakura. American Mathematical Society, Providence, R.I. ISBN 0-8218-4556-X.
- Egorov, Yu. V.; Schulze, Bert-Wolfgang (1997). Pseudo-differential operators, singularities, applications. Birkhäuser. ISBN 3-7643-5484-4.
- Vladimirov, V. S. (2002). Methods of the theory of generalized functions. Taylor & Francis. ISBN 0-415-27356-0.
- Folland, G. B. (2009). Fourier Analysis and its applications. AMS. ISBN 978-0-8218-4790-9.
This article incorporates material from Hypoelliptic on PlanetMath, which is licensed under the Creative Commons Attribution/Share-Alike License.