Is it possible to deduce the conservation of angular momentum from the conservation of energy? Is it possible to deduce the law of conservation of angular momentum from the law of conservation of energy? If possible, by what sense the conservation of angular momentum has the status of law, if it can be deduced from other law (and therefore, strictly speaking, would be a theorem)?    
 A: The conservation of angular momentum and energy in a mechanical system are distinct, independent conservation laws. The deep reason for this is that, because of Noether's theorem, conservation laws are in correspondence with the symmetries of the system. Thus if a system is time-translation invariant - if experiments behave the same no matter what the starting time is - then energy is conserved. Analogously, if a system is rotation invariant - if the outcome of experiments is independent of the system's orientation - then angular momentum is conserved.
Because of that, angular momentum conservation can no more be derived from energy conservation than it is possible to derive rotation invariance from time-translation invariance.

To be clear: This answer explains the fundamental reason why the two conservation laws are independent, and why it would be useless to even try. This argument can be strengthened using this converse to Noether's theorem: conservation of energy and of angular momentum are equivalent to time-translation and rotation invariance. These symmetries are independent, and contribute independent dimensions to the Lie symmetry group of the system's evolution, so they cannot be derived from each other.
As Jerry Schirmer said, it is trivial to construct a counterexample, which is what his answer contains.
Further, this independence argument does also extend to linear momentum. (For a simple counterexample, try a particle in a box - conserved energy but not momentum - or a free particle in a time-dependent but spatially homogeneous electrostatic potential - conserved momentum but not energy.) Of course, neither of these systems obeys boost invariance.
The underlying theme is this. If I have two different conserved quantities, $A$ and $B$, then I can sometimes find a third conserved quantity by taking their Poisson bracket (or their commutator in QM), so long as that is not zero. For example, conservation of $p_x$ and $L_z$ implies conservation of $p_y$. The key to this is that the associated symmetries are also related: translation invariance along $x$ and rotation invariance about the $z$ axis, together, imply translation invariance along the $y$ axis. Similarly, space translation invariance and boost invariance imply time translation invariance.
A: No.  Angular momentum and energy are two different quantities.  In fact, angular momentum can be conserved when energy is not.  See, for instance, the famous case of the figure skater pulling their arms in and spinning more quickly.  
Let's say our figure skater reduces their moment of inertia to some fraction $n$ of their original moment of inertia.  Then:
$$\begin{align}
I_{0}\omega_{0} &= I_{f}\omega_{f}\\
I_{0}\omega_{0} &= nI_{0}\omega_{f}\\
\omega_{f} &= \frac{1}{n}\omega_{0}
\end{align}$$
However, we have:
$$KE_{i} = \frac{1}{2}I_{0}\omega_{0}^{2}$$
And 
$$\begin{align}
KE_{f} &= \frac{1}{2}I_{f}\omega_{f}^{2}\\
&= \frac{1}{2}nI_{0}\left(\frac{1}{n}\omega_{0}\right)^{2}\\
&= \frac{1}{2n}I_{0}\omega_{0}^{2}\\
&= \frac{1}{n}KE_{i}
\end{align}$$
So, the final kinetic energy of our figure skater is greater than their initial kinetic energy!  Angular momentum is conserved, but energy is not.  
(of course, we know that overall energy is conserved, so you may ask where this extra energy came from--the answer is that it requires net work in order to pull your hands in while you're spinning.  So no violation of the rules of physics here.)
A: Some conservation laws are related to conservation of angular momentum.
There is a famous example (from Feynman if I recall correctly), where you assume an infinite flat space and conservation of angular momentum about any point, and then you get conservation of linear momentum for free.
Intuitively, to get say the $x$ component of linear momentum is conserved in a region you consider a coordinate system centered at the region, and consider the angular momentum about a point way off in the $y$ (or $z$, or any direction orthogonal to $x$) such a super great distance away and then effectively conservation of angular momentum about that distance point requires conservation of the $x$ component of linear momentum.
There is also a conservation law for angular momentum:
$0 = (x^{\alpha} T^{\mu \nu} - x^{\mu} T^{\alpha \nu})_{,\nu}$,
from flat space Special Relativity and the symmetries of the stress-energy tensor.  In fairness, this might be considered cheating (as a derivation) since most derivations of the symmetry of the stress-energy tensor assume that little bits of matter don't spin arbitrary fast as you look at smaller and smaller bits of them.
