Miller indices are used to describe the orientation of a crystal plane in a lattice. The Miller indices are the reciprocals of the fractional intercepts of the plane with the crystallographic axes. For a plane cutting at \( x = a \), \( y = \infty \), and \( z = c \), the Miller indices are calculated by taking the reciprocal of these intercepts.
- The intercept on the \( x \)-axis is \( a \), so the reciprocal is \( \frac{1}{a} \). This gives a Miller index of 1 for the \( x \)-direction.
- The intercept on the \( y \)-axis is infinite, so the reciprocal is zero, leading to a Miller index of 0 for the \( y \)-direction.
- The intercept on the \( z \)-axis is \( c \), so the reciprocal is \( \frac{1}{c} \), giving a Miller index of 1 for the \( z \)-direction.
Thus, the correct Miller indices for this plane are \( (1 0 1) \).