Step 1: Understand the symmetry of the circuit.
The circuit contains four equal resistors of value
\[
R_1=\beta R
\]
and a central branch containing
\[
R_2=\gamma R
\]
along with a source \(V_2=\alpha V\).
Using Kirchhoff's laws and symmetry, let the current in the right lower branch be \(I\).
Step 2: Apply Kirchhoff's Voltage Law.
The equivalent analysis of the bridge gives the current through the indicated branch as
\[
I=
\frac{V_2-V_1}{4R_1\left(1+\dfrac{R_1}{R_2}\right)}
\]
Substituting
\[
V_1=V,\qquad V_2=\alpha V,
\]
we get
\[
I=
\frac{\alpha V-V}{4\beta R\left(1+\dfrac{\beta R}{\gamma R}\right)}
\]
\[
=
\frac{(\alpha-1)V}{4\beta R\left(1+\dfrac{\beta}{\gamma}\right)}
\]
Step 3: Simplify the denominator.
\[
1+\frac{\beta}{\gamma}
=
\frac{\beta+\gamma}{\gamma}
\]
Hence,
\[
I=
\frac{(\alpha-1)V}{4\beta R\left(\dfrac{\beta+\gamma}{\gamma}\right)}
\]
\[
=
\frac{(\alpha-1)\gamma}{4\beta(\beta+\gamma)}
\cdot \frac{V}{R}
\]
Step 4: Final conclusion.
Therefore, the current is
\[
\boxed{
\dfrac{(\alpha-1)\gamma}{4\beta(\beta+\gamma)}
\dfrac{V}{R}
}
\]