To solve this problem, we need to evaluate a triple integral over a specified region \( E \). The region \( E \) is defined by \( x \geq 0 \), \( y \geq 0 \), and the bounds for \( z \) are given by \( \sqrt{x^2 + y^2} \leq z \leq 1 \). The integrand is \( xy \). We can use cylindrical coordinates to simplify the integration process, where \( x = r \cos \theta \), \( y = r \sin \theta \), and \( z = z \). The bounds for \( r \) will be from 0 to 1, \( \theta \) from 0 to \(\pi/2\), and \( z \) from \( r \) to 1.
We are tasked with evaluating the triple integral
\[
\iiint_{E} xy \, dV
\]
where \( E \) is defined by \( x \geq 0 \), \( y \geq 0 \), and \( \sqrt{x^2 + y^2} \leq z \leq 1 \). In cylindrical coordinates, we have \( x = r \cos \theta \), \( y = r \sin \theta \), and the volume element \( dV = r \, dr \, d\theta \, dz \). Thus, the integrand becomes
\[
xy = r^2 \cos \theta \sin \theta.
\]
The limits for the integration are as follows:
- For \( r \): from \( 0 \) to \( 1 \)
- For \( \theta \): from \( 0 \) to \( \frac{\pi}{2} \)
- For \( z \): from \( r \) to \( 1 \)
We first integrate with respect to \( z \):
\[
\int_{r}^{1} r^3 \sin \theta \cos \theta \, dz = r^3 \sin \theta \cos \theta (1 - r).
\]
Next, we integrate with respect to \( r \):
\[
\int_{0}^{1} r^3 (1 - r) \, dr = \frac{1}{40}.
\]
Finally, we integrate with respect to \( \theta \):
\[
\int_{0}^{\frac{\pi}{2}} \frac{1}{40} \sin \theta \cos \theta \, d\theta = \frac{1}{40} \cdot \frac{1}{2} = \frac{1}{80}.
\]
The value of the triple integral is
\[
\boxed{\frac{1}{40}}.
\]