- A$\lambda_d / \lambda$
- B$\lambda_{\mathrm{d}}^2 / \lambda$
- C$\lambda_d^3 / \lambda$
- ✓$\lambda_{\mathrm{d}}^3 / \lambda^2$
$\frac{\mathrm{h}^2}{2 \mathrm{~m} \cdot \lambda_{\mathrm{D}}^2}=\frac{\mathrm{hc}}{\lambda}-\phi_0$
$-\frac{\mathrm{h}^2}{\mathrm{~m}} \frac{1}{\lambda_{\mathrm{D}}^3} \mathrm{~d} \lambda_{\mathrm{D}}=\frac{\mathrm{hc}}{\lambda^2} \mathrm{~d} \lambda$
$\frac{\Delta \lambda_{\mathrm{D}}}{\Delta \lambda} \propto \frac{\lambda_{\mathrm{D}}^3}{\lambda^2}.$
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($A$) Straight bright and dark bands parallel to the $x$-axis
($B$) The region very close to the point $O$ will be dark
($C$) Hyperbolic bright and dark bands with foci symmetrically placed about $\mathrm{O}$ in the $x$-direction
($D$) Semi circular bright and dark bands centered at point $\mathrm{O}$