Throughout this article, we use the following notation and conventions. For a complex vector
, we
denote by
its transposed, complex conjugate, such that
is the standard scalar product
for two vectors
. The corresponding norm is defined by
. The norm of a complex,
matrix
is
The transposed, complex conjugate of
is denoted by
, such that
for all
and
. For two Hermitian
matrices
and
, the
inequality
means
for all
. The identity matrix is denoted by
.
The spectrum of a complex,
matrix
is the set of all eigenvalues of
,
which is real for Hermitian matrices. The spectral radius of
is defined as
Then, the matrix norm
of a complex
matrix
can also be computed as
.
Next, we denote by
the class of measurable functions
on the open subset
of
, which are square-integrable. Two functions
, which differ from each
other only by a set of measure zero, are identified. The scalar product on
is defined
as

and the corresponding norm is
. According to the Cauchy–Schwarz inequality we
have
The Fourier transform of a function
, belonging to the class
of infinitely-differentiable
functions with compact support, is defined as
According to Parseval’s identities,
for all
, and the map
,
can be extended to a linear, unitary map
called the Fourier–Plancharel
operator; see, for example, [346
]. Its inverse is given by
for
and
.
For a differentiable function
, we denote by
,
,
,
its partial derivatives with respect
to
,
,
,
.
Indices labeling gridpoints and number of basis functions range from
to
. Superscripts and
subscripts are used to denote the numerical solution at some discrete timestep and gridpoint, as
in
|
Living Rev. Relativity 15, (2012), 9
http://www.livingreviews.org/lrr-2012-9 |
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