  Anisotropic Special Relativity (ASR) is the relativistic theory of nature
with a preferred direction in space-time. By relaxing the full-isotropy
constraint on space-time to the preference of one direction, we get a
perturbative modification of the Minkowski metric as
$\mathscr{g}_{\mu\nu}=\eta_{\mu\nu}-b\epsilon_{\mu\nu}$ leading to an extension
to the geometrical objects such as line element. The symmetry group of ASR is
obtained to have six generators satisfying the full Lorentz group algebra.
However, the generators are deformed using the perturbation parameter $b$. So,
ASR retains the same representations of Special Relativity (SR) but allows for
Lorentz-invariant violation at the same time. A procedure to make an
anisotropic quantum field theory is provided wherein the Lorentz-invariant
Lagrangians are replaced with their ASR version in which the inner product of
any pair of covariant/contravariant indices is mediated by the anisotropic
metric $\mathscr{g}_{\mu\nu}$.
