The radius of the circular path of a charged particle moving in a uniform magnetic field is given by the formula:
\[
r = \frac{mv}{qB}
\]
where:
- \( r \) is the radius of the circular path,
- \( m \) is the mass of the particle,
- \( v \) is the velocity of the particle,
- \( q \) is the charge of the particle,
- \( B \) is the magnetic field strength.
For a proton, the kinetic energy \( K_e \) is related to its velocity by:
\[
K_e = \frac{1}{2} m v^2
\]
For a deuteron, the mass \( m_d \) is twice the mass of the proton \( m_p \), i.e., \( m_d = 2 m_p \), and the charge \( q_d \) is twice the charge of the proton, i.e., \( q_d = 2 q_p \).
Since both particles are moving in the same circular path, we can equate their radii:
\[
r_p = r_d
\]
Thus:
\[
\frac{m_p v_p}{q_p B} = \frac{m_d v_d}{q_d B}
\]
Simplifying, we get:
\[
\frac{m_p v_p}{q_p} = \frac{2 m_p v_d}{2 q_p}
\]
\[
v_p = v_d
\]
Therefore, the velocities of the proton and deuteron are the same. Now, using the relation between kinetic energy and velocity for both particles:
\[
K_e = \frac{1}{2} m v^2
\]
For the proton, we know the kinetic energy is 2 MeV:
\[
2 \, {MeV} = \frac{1}{2} m_p v_p^2
\]
For the deuteron, the kinetic energy \( K_d \) is:
\[
K_d = \frac{1}{2} m_d v_d^2 = \frac{1}{2} (2 m_p) v_p^2 = 2 \times \frac{1}{2} m_p v_p^2 = 2 \times 2 \, {MeV} = 1 \, {MeV}
\]
Thus, the correct answer is option (B), 1 MeV.