Derrick's theorem
Derrick's theorem is an argument due to a physicist G.H. Derrick which shows that stationary localized solutions to a nonlinear wave equation or nonlinear Klein–Gordon equation in spatial dimensions three and higher are unstable.
Original argument
Derrick's paper,[1] which was considered an obstacle to interpreting soliton-like solutions as particles, contained the following physical argument about non-existence of stable localized stationary solutions to the nonlinear wave equation
,
now known under the name of Derrick's Theorem.
(Above, is a differentiable function with
.)
The energy of the time-independent solution
is given by
A necessary condition for the solution to be stable
is .
Suppose
is a localized solution of
.
Define
where
is an arbitrary constant, and write
,
.
Then
Whence
,
and since
,
That is, for a variation corresponding to
a uniform stretching of the particle.
Hence the solution
is unstable.
The above argument also works for ,
.
Pohozaev's identity
More generally,[2]
let be continuous, with
.
Denote
.
Let
be a solution to the equation
,
in the sense of distributions.
Then satisfies the relation
known as Pohozaev's identity.[3] It result is similar to the Virial theorem.
Interpretation in the Hamiltonian form
We may write the equation
in the Hamiltonian form
,
,
where
are functions of
,
the Hamilton function is given by
and ,
are the
variational derivatives of
.
Then the stationary solution
has the energy
and
satisfies the equation
with
denoting a variational derivative
of the functional
.
Although the solution
is a critical point of
(since
),
Derrick's argument shows that
at
,
hence
is not a point of the local minimum of the energy functional
.
Therefore, physically, the solution
is expected to be unstable.
Stability of localized time-periodic solutions
Derrick describes some possible ways out of this difficulty, including the conjecture that Elementary particles might correspond to stable, localized solutions which are periodic in time, rather than time-independent.
Indeed, it was later shown[4] that a time-periodic solitary wave with frequency
may be orbitally stable if the Vakhitov–Kolokolov stability criterion is satisfied.
See also
References
- ↑ G.H. Derrick (1964). "Comments on nonlinear wave equations as models for elementary particles". J. Mathematical Phys. 5: 1252–1254. Bibcode:1964JMP.....5.1252D. doi:10.1063/1.1704233.
- ↑ Berestycki, H. and Lions, P.-L. (1983). "Nonlinear scalar field equations, I. Existence of a ground state". Arch. Rational Mech. Anal. 82: 313–345. Bibcode:1983ArRMA..82..313B. doi:10.1007/BF00250555.
- ↑ Pohozaev, S.I. (1965). "On the eigenfunctions of the equation
". Dokl. Akad. Nauk SSSR 165: 36–39.
- ↑ Вахитов, Н. Г. and Колоколов, А. А. (1973). "Стационарные решения волнового уравнения в среде с насыщением нелинейности". Известия высших учебных заведений. Радиофизика 16: 1020–1028. N.G. Vakhitov and A.A. Kolokolov (1973). "Stationary solutions of the wave equation in the medium with nonlinearity saturation". Radiophys. Quantum Electron. 16: 783–789. Bibcode:1973R&QE...16..783V. doi:10.1007/BF01031343.