Preliminary definitions and observations
What "spherical" means
That $f$ is "spherical" (often called "elliptical") means
$$f(Hx) = f(x)\tag{1}$$
for all $x\in\mathbb{R}^n$ and all orthogonal matrices $H$.
That $k$ is "spherical" means the same thing. Applying it to the argument in the integral gives
$$k\left(\frac{Hy - Hx}{h}\right) = k\left(H \frac{y-x}{h}\right) = k\left(\frac{y-x}{h}\right)\tag{2}$$
for all $x,y\in\mathbb{R}^n$, all positive real numbers $h$, and all orthogonal matrices $H$. (The first equality is a consequence of the linearity of $H$.)
Invariance of the volume element
Any orthogonal matrix $H$ has unit determinant due to the defining relation $H^\prime H = I_n$ because
$$1 = |I_n| = |H^\prime H| = |H^\prime| |H| = |H|^2,$$
whence the absolute value of $|H|$ must equal $1$. This implies the volume element $|dx|$ is invariant under orthogonal transformations, because
$$|\pm 1\, dx| = |\,|H|\,dx| = |d(Hx)| = |dx|.\tag{3}$$
Transitivity of the orthogonal group
Finally, whenever $||y||=||z||$, there is an orthogonal matrix $H$ for which
$$H y = z.\tag{4}$$
For instance, the matrix $H$ representing the reflection through the midpoint of the line segment from $z$ to $y$ will work.
The derivation
After finding an $H$ by virtue of $(4)$, substitute $z=Hy$ to produce
$$\lambda_z = \int_{\mathbb{R}^n} k\left(\frac{z-x}{h}\right) f(x) dx
= \int_{\mathbb{R}^n} k\left(\frac{Hy-x}{h}\right) f(x)dx.$$
Make the change of variable $x = H x^\prime$. The invariance of $|dx^\prime|$ under orthogonal transformations $(3)$ yields
$$\int_{\mathbb{R}^n} k\left(\frac{Hy-x}{h}\right) f(x) dx = \int_{\mathbb{R}^n} k\left(\frac{Hy-Hx^\prime}{h}\right) f(Hx^\prime) dx^\prime.$$
This is the point where we require the spherical invariance of both $f$ (equation $(1)$) and $k$ (equation $(2)$), for they allow us to simplify this expression as
$$\lambda_z = \int_{\mathbb{R}^n} k\left(\frac{Hy-Hx^\prime}{h}\right) f(Hx^\prime) dx^\prime = \int_{\mathbb{R}^n} k\left(\frac{y-x^\prime}{h}\right) f(x^\prime) dx^\prime = \lambda_y,$$
QED.