The condition for constructive interference (bright fringes) in a double-slit experiment is given by the formula:
\[
y_m = \frac{m \lambda D}{d}
\]
where:
- \( m \) is the fringe order (1, 2, 3,...),
- \( \lambda \) is the wavelength of light,
- \( D \) is the distance between the slits and the screen,
- \( d \) is the distance between the slits.
For the two wavelengths to produce coinciding fringes, their fringe positions should be equal. Hence, we set the condition for the bright fringe coincidence of both wavelengths \( \lambda_1 = 600 \ \text{nm} \) and \( \lambda_2 = 400 \ \text{nm} \).
The fringe positions for each wavelength at the same order \( m \) are given by:
\[
y_m = \frac{m \lambda_1 D}{d} = \frac{m \lambda_2 D}{d}
\]
The first coinciding fringe occurs when \( m_1 \lambda_1 = m_2 \lambda_2 \), i.e., the smallest common multiple of the wavelengths, which happens when \( m_1 = 2 \) and \( m_2 = 3 \).
Now, using \( d = 1.5 \times 10^{-3} \ \text{m} \) and \( D = 1.5 \ \text{m} \), we substitute these values into the equation for \( m_1 = 2 \) and \( m_2 = 3 \):
\[
y = \frac{(2) \cdot 600 \times 10^{-9} \cdot 1.5}{1.5 \times 10^{-3}} = 0.36 \ \text{m}
\]
Thus, the minimum distance from the central maximum where the bright fringes coincide is approximately \( 0.36 \ \text{m} \).
Final Answer: The minimum distance is approximately \( \boxed{0.36 \ \text{m}} \).