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Light-front computational methods : ウィキペディア英語版
Light-front computational methods

The light front quantization


of quantum field theories
provides a useful alternative to ordinary equal-time
quantization. In
particular, it can lead to a relativistic description of bound systems
in terms of quantum-mechanical wave functions. The quantization is
based on the choice of light-front coordinates,
where
x^+\equiv ct+z plays the role of time and the corresponding spatial
coordinate is x^-\equiv ct-z. Here, t is the ordinary time, z
is one Cartesian coordinate,
and c is the speed of light. The other
two Cartesian coordinates, x and y, are untouched and often called
transverse or perpendicular, denoted by symbols of the type
\vec x_\perp = (x,y). The choice of the
frame of reference where the time
t and z-axis are defined can be left unspecified in an exactly
soluble relativistic theory, but in practical calculations some choices may be more suitable than others.
The solution of the LFQCD Hamiltonian eigenvalue
equation will utilize the available mathematical
methods of quantum mechanics and contribute to the
development of advanced computing techniques for
large quantum systems, including nuclei. For
example, in the discretized light-cone quantization method
(DLCQ),





periodic conditions are introduced such that momenta are
discretized and the size of the Fock space is
limited without destroying Lorentz invariance.
Solving a quantum field theory is then reduced to
diagonalizing a large sparse Hermitian matrix. The
DLCQ method has been successfully used to obtain
the complete spectrum and light-front wave functions in numerous model
quantum field theories such as QCD with one or two
space dimensions for any number of flavors and
quark masses. An extension of this method to
supersymmetric theories,
SDLCQ,

takes advantage of the
fact that the light-front Hamiltonian can be factorized as
a product of raising and lowering ladder operators.
SDLCQ has provided new insights into a
number of supersymmetric theories including direct numerical
evidence
for a supergravity/super-Yang—Mills duality conjectured
by Maldacena.
It is convenient to work in a Fock basis
\\rangle\} where the light-front
momenta \mathcal^+ and \vec\mathcal_\perp are diagonal.
The state |\underline\rangle is given by an expansion

|\underline\rangle=\sum_n\int ()_n\,()_n\,
\psi_n(x,\vec_\perp)|n:xP^+,x\vec_\perp+\vec_\perp\rangle\,,

with

()_n=4\pi\delta(1-\sum_^nx_i)

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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