Given: An electron (mass \(m\), charge \(-e\)) with initial velocity \(\vec{v} = \vec{v_0}\) (where \(v_0 > 0\)) enters a uniform magnetic field \(\vec{B} = B\hat{j}\). The initial de-Broglie wavelength is \(\lambda_0\). Determine its wavelength after time \(t\).
The magnetic field exerts a Lorentz force on the moving electron:
\[ \vec{F} = -e(\vec{v} \times \vec{B}). \]
This force alters the velocity's direction but not its magnitude, as it is perpendicular to \(\vec{v}\). Consequently, the speed remains constant.
The de-Broglie wavelength is defined as:
\[ \lambda = \frac{h}{p} = \frac{h}{mv}. \]
Since \(v\) (velocity magnitude) is invariant, the de-Broglie wavelength also remains constant over time.
Step 1: Formulate the equation of motion:
\[ m \frac{d\vec{v}}{dt} = -e(\vec{v} \times \vec{B}). \]
The magnetic field induces circular motion at an angular frequency (cyclotron frequency):
\[ \omega = \frac{eB}{m}. \]
Step 2: The velocity magnitude \(v_0\) is constant; only its direction changes. Thus, the momentum magnitude \(p = mv_0\) is conserved.
Step 3: The de-Broglie wavelength at time \(t\) is therefore:
\[ \lambda = \frac{h}{mv_0} = \lambda_0. \]
\[ \boxed{\lambda(t) = \lambda_0.} \]
The electron's de-Broglie wavelength remains constant over time.