Step 1: Use magnetic force on a current carrying wire.
\[
F = I l B \sin\theta
\]
where \(\theta\) is the angle between length of conductor and magnetic field.
Step 2: Force on arm \(XY\).
Since magnetic field is along \(XY\),
\[
\theta = 0^\circ
\]
\[
F_{XY} = I l B \sin 0^\circ = 0
\]
Step 3: Force on arm \(YZ\).
Arm \(YZ\) is perpendicular to \(XY\), so it is perpendicular to magnetic field.
\[
F_{YZ} = IB(YZ)\sin 90^\circ
\]
Given,
\[
F_{YZ} = \sqrt{2}F
\]
Step 4: Use net force condition on closed loop.
In a uniform magnetic field, the net magnetic force on a closed current loop is zero.
\[
F_{XY} + F_{YZ} + F_{XZ} = 0
\]
Step 5: Substitute known force.
\[
0 + \sqrt{2}F + F_{XZ} = 0
\]
Step 6: Solve for force on \(XZ\).
\[
F_{XZ} = -\sqrt{2}F
\]
Step 7: Final answer.
\[
\boxed{-\sqrt{2}F}
\]