  In recent times, Bogoliubov Fermi surfaces (BFSs) in superconductors (SCs)
have drawn significant attention due to a substantial population of Bogoliubov
quasiparticles (BQPs) together with Cooper pairs (CPs) in them. The BQPs as
zero energy excitations give rise to captivating and intricate charge dynamics
within the BFSs. In this theoretical study, we propose to reveal the unique
signatures of the topologically protected BFSs in bulk $d$-wave SCs using
normal metal/time-reversal symmetry (TRS) broken $d$-wave SC hybrid setup, in
terms of the differential conductance and Fano factor (FF). Orientation of
crystal $a$ axis with respect to junction normal, quantified by the parameter
$\alpha$, is crucial for transport properties in these hybrid devices. For
$\alpha=0$, an enhancement in zero-bias conductance (ZBC) can be identified as
a key signature of BFSs. However, for $\alpha\ne0$, this feature does not
replicate due to the presence of the localized Andreev bound state (ABS) at the
interface. The interplay of ABS and BFSs gives rise to an anomalous behavior in
ZBC compared to the $\alpha=0$ case. This behavior remains qualitatively
similar even at finite temperatures. Finally, we explain this anomalous
behavior by analyzing the effective charge of the carriers in terms of the FF.
The simplicity of our setup based on $d$-wave SC makes our proposal persuasive.
