TITLE: is every element in a C* algebra a product of normal elements?
QUESTION [8 upvotes]: I have the following question and since I am not an expert on C*-algebras, I thought I ask it here:
I know that in general the sum and product of normal elements need not be normal. It is even true that every element in a C*-algebra is the sum of two normal elements. What I do not know is if that is true for multiplication, too, i.e. if every element in a C*-algebra is a product of normal elements.
I think I know that every invertible element can be written as a product of a unitary and a positive element but this decomposition does not work for non-invertible elements.
My standard example is the right shift operator on the l^2(N)-space. This is a non-normal operator, which is not invertible and I have no idea how to write it as a product of two normal operators.
I would be very grateful if anyone could help.
Greetings, Tom.

REPLY [10 votes]: Since the question was asked wrt C$*$-algebras, I guess there is room for a general remark. Suppose that $xy = 1$ where $x$ is a product of normal elements, say
$v_1v_2\cdots v_n$. Then $v_1$ is normal and has a right inverse;
therefore it is (two-sided) invertible. Thus $v_2\dots v_n y $ is
invertible, so $v_2$ has a right inverse, and thus is invertible. By
induction, we obtain that all the $v_i$ are two-sided invertible, so that
$x$ is too.
The upshot of this argument is that a product of normal elements that is
one-sided invertible, is actually invertible. In particular, the right
shift is not a product of normal elements---although of course, the index argument above is decisive in this case.
If every element of a C$*$-algebra were a product of normals,
then it would be directly finite (all one-sided inverses are two-sided).
Whether this is sufficient is unclear (as is the question as to whether the product of normals property extends to matrix rings over the original). But if the C*-algebra has one in
the stable range, then every element is an invertible times a positive, so
is a product of (three) normals. 
And for von Neumann algebras, if of finite type, then every element is a product of two normals, as the isometry in the polar decomposition argument (below) can be modified to be a unitary in that case. If not of finite type, the property fails.