  In this work, we compute the hard thermal loop pressure of quark-gluon plasma
within strong magnetic field approximation at one-loop order. Magnetic field
breaks the rotational symmetry of the system. As a result, the pressure of QGP
becomes anisotropic and one finds two different pressures along the
longitudinal (along the magnetic field direction) and transverse direction.
Similarly, the second-order quark number susceptibility, which represents the
fluctuation of the net quark number density, also becomes anisotropic. We
compute the second order QNS of deconfined QCD matter in strong field
approximation considering same chemical potential for two quark flavors.
