The magnetic force (\( \vec{F}_m \)) experienced by a charged particle with charge (\( q \)) moving with velocity (\( \vec{v} \)) in a magnetic field (\( \vec{B} \)) is given by:
\[ \vec{F}_m = q (\vec{v} \times \vec{B}). \]
Inside a solenoid, the magnetic field (\( \vec{B} \)) is uniform and directed along the axis of the solenoid.
Thus, the magnetic force on the electron is:
\[ \vec{F}_m = 0. \]
Since the magnetic force on the electron is zero, there is no net force acting perpendicular to its motion. As a result:
The electron will not experience a magnetic force (B), and it will continue to move along the axis of the solenoid (C).

Let \( \alpha = \dfrac{-1 + i\sqrt{3}}{2} \) and \( \beta = \dfrac{-1 - i\sqrt{3}}{2} \), where \( i = \sqrt{-1} \). If
\[ (7 - 7\alpha + 9\beta)^{20} + (9 + 7\alpha - 7\beta)^{20} + (-7 + 9\alpha + 7\beta)^{20} + (14 + 7\alpha + 7\beta)^{20} = m^{10}, \] then the value of \( m \) is ___________.