Step 1: Recall Miller indices definition.
For a crystal plane:
1. Find the intercepts of the plane with the crystallographic axes in terms of the lattice constants $a, b, c$.
2. Take reciprocals of intercepts.
3. Clear fractions to smallest integers → gives Miller indices $(hkl)$.
Step 2: Identify intercepts from figure.
From the figure:
- Plane passes through $P$, $Q$, $R$.
- Along $a$ axis: intercept at full length $\Rightarrow$ $1a$.
- Along $b$ axis: intercept at $\tfrac{2}{3}b$.
- Along $c$ axis: intercept at $\tfrac{1}{2}c$.
So, intercepts = $(1a, \tfrac{2}{3}b, \tfrac{1}{2}c)$.
Step 3: Take reciprocals.
\[
\frac{a}{a} = 1, \frac{b}{2/3b} = \frac{3}{2}, \frac{c}{1/2c} = 2.
\]
So reciprocals = $(1, \tfrac{3}{2}, 2)$.
Step 4: Clear fractions.
Multiply through by 2:
\[
(2, 3, 4).
\]
Thus, Miller indices = $(234)$.
Step 5: Check orientation sign.
From the diagram, all intercepts are positive along $+a, +b, +c$ directions. No negative sign needed.
So final Miller indices = $(234)$.
Final Answer:
\[
\boxed{(234)}
\]