V2O5 is a promising
candidate in varied fields
and has proven to favor polaron formation. Polarons are slow-moving
with extra mass, thus affecting conductivity. Charge transport/conductivity
is one of the key factors deciding device utility and is compromised
due to the slow motion of polarons. To solve this, incorporating graphene
into V2O5 is widely practiced. V2O5 exhibiting small polaron hopping is a fact, and variable
range hopping of highly mobile electrons is observed in graphene at
low temperatures. The inclusion of graphene into V2O5 shows conductivity enhancement and hence has been widely
studied for varied applications. The reason for conductivity enhancement
is considered to be the presence of delocalized electrons in graphene,
which makes the sample electron-rich and increases conductivity. But
the actual mechanism of conductivity enhancement is unclear. This
led us to explore the electrical properties of graphene-wrapped V2O5. To our surprise, the inclusion of graphene
completely changes the dynamics of charge carriers. Polarons in composite
chose variable range hopping over Arrhenius-type small polaron hopping
in the temperature range of 143–263 K. ac conductivity σ′(ω)
data of V2O5 and reduced graphene oxide (RGO)-wrapped
V2O5 are analyzed using the Cole–Cole-type
combined conduction and dielectric model. σdc of
polarons shows T
–1 dependence for
V2O5 and T
–1/2 dependence for RGO-wrapped V2O5 (VRGO). In
general, at low temperatures (T < 100 K), such
behavior is interpreted to be Efros–Shklovskii (ES) VRH, but
the temperature range (143–263 K) that we have covered cannot
justify ES-VRH. A detailed overview of the carrier environment is
carried out using tools such as XRD and temperature-dependent Raman
along with conductivity measurements to account for the T
–1/2 dependence of polarons. The results of various
measurements point toward the origin of Mott gap in V2O5 after incorporating graphene into it, thus controlling the
surprising behavior of polarons.