Step 1: Write the magnetic force on a moving charge.
\[ F = q v B \sin\theta \]
Here the velocity is perpendicular to \(B\), so \(\theta = 90^\circ\) and \(\sin\theta = 1\):
\[ F = q v B \]
Step 2: Note what is common and what varies.
Speed \(v\) and field \(B\) are the same for all four particles, so the force depends only on the magnitude of charge \(q\).
Step 3: Compare the charges.
Electron: \(|q| = e\); proton: \(q = e\); deuteron: \(q = e\); \(\alpha\) particle: \(q = 2e\).
Step 4: The \(\alpha\) particle carries the largest charge \(2e\), so it experiences the maximum force. Mass is irrelevant to the instantaneous force here.
\[\boxed{\alpha\text{ particle}}\]