Step 1: Use de-Broglie wavelength relation in Bohr orbit.
For an electron moving in the \(n^{th}\) orbit of a hydrogen-like species,
\[
2\pi r=n\lambda
\]
From Bohr theory,
\[
r_n=\frac{n^2a_0}{Z}
\]
Hence,
\[
\lambda=\frac{2\pi r_n}{n}
\]
Substituting \(r_n\),
\[
\lambda=\frac{2\pi}{n}\left(\frac{n^2a_0}{Z}\right)
\]
Therefore,
\[
\lambda \propto \frac{n}{Z}
\]
Step 2: Wavelength in ground state of hydrogen atom.
For hydrogen atom,
\[
Z=1
\]
Ground state means
\[
n=1
\]
Thus,
\[
\lambda_H \propto \frac{1}{1}=1
\]
Given,
\[
\lambda_H=y
\]
Step 3: Wavelength in fourth orbit of \(He^+\).
For \(He^+\),
\[
Z=2
\]
Fourth orbit means
\[
n=4
\]
Therefore,
\[
\lambda_{He^+}\propto \frac{4}{2}=2
\]
Comparing with hydrogen ground state,
\[
\lambda_{He^+}=2y
\]
But in Bohr’s quantization,
\[
n\lambda=2\pi r
\]
and for hydrogen-like atoms,
\[
r_n=\frac{n^2a_0}{Z}
\]
Thus,
\[
\lambda=\frac{2\pi n a_0}{Z}
\]
For hydrogen ground state:
\[
\lambda_H=2\pi a_0
\]
For \(He^+\) fourth orbit:
\[
\lambda_{He^+}=\frac{2\pi (4)a_0}{2}
=4\pi a_0
\]
Hence,
\[
\lambda_{He^+}=2\lambda_H
\]
Therefore,
\[
\lambda_{He^+}=2y
\]
Step 4: Final conclusion.
Hence, the wavelength of electron in the fourth orbit of \(He^+\) ion is
\[
\boxed{2y}
\]