Linear operators & the uncertainty principle

[Ahmes]

Hi,
I try to understand the proof for the uncertainty principle for two Hermitian operators A and B in a Hilbert space. My questions are rather general so you don't need to know the specific proof.

The first thing I couldn't get into my head was the definition of uncertainty
(\Delta A)^2=\langle\psi|(A- \langle A \rangle)^2|\psi\rangle
Using the properties of the inner product I can be convinced this is equivalent to the ordinary definition of (\Delta A)^2=\langle A^2 \rangle-{\langle A \rangle}^2 BUT A is an operator and \langle A \rangle is a number! How can (A- \langle A \rangle)^2 even be defined?

Second - somewhere else in the proof a new vector is defined |\varphi \rangle=C| \psi \rangle OK, they can do it, but then they say that if so, then also \langle \varphi |= \langle \psi | C^\dagger and I just can't see why... Why the dagger I mean

Can anyone help?
Thanks in advance.

[Galileo]

There's nothing wrong with adding a scalar to an operator, since you can interpret every scalar itself as an operator. It just multiplies the vector it acts upon by the scalar. If it helps, you can also imagine the identity operator next to it.

By the way, the ordinary definition of (\Delta A)^2 is either \langle (A-\langle A \rangle)^2\rangle, or \langle A^2 \rangle-{\langle A \rangle}^2. They are identical ofcourse, but from the former you can easily see that
(\Delta A)^2=\langle\psi|(A- \langle A \rangle)^2|\psi\rangle

since, for any operator \langle Q \rangle = \angle \psi|Q|\psi \rangle.

The bra associated with the ket C|\psi \rangle is \langle \psi|C^\dagger, I`m sure that's explained in your book somewhere.
\langle \psi |C|\psi\rangle^*=\langle \psi |C^\dagger|\psi\rangle

[Ahmes]

Thanks.
It took me quite a while to convince myself about the latter...