kingwinner said:
Say, for example, if we consider C^2 with the standard inner product and T: C^2->C^2 is defined by T(x,y)=(x+(1-i)y, (1+i)x+2y), how exactly can I find T*(x,y)?
The definition of T* seems obscure to me...
Since T* is also linear, T*(u,v) must be (au+ bv, cu+ dv) for some complex numbers, a, b, c, and d.
You want <(x+(1-i)y, (1+i)x+2y), (u,v)>= xu+ (1-i)\overline{u}y+ (1+i)x\overline{v}+ 2y\overline{v} to be equal to
< (x,y), (au+ bv,cu+dv)>= \overline{a}x\overline{u}+ \overline{b}x\overline{v}+ \overline{c}\overline{u}y+ \overline{d}\overline{v}y. Since this must be true for all x, y, u, v, coefficients of the same products must be equal: 1= \overline{a}, 1- i= \overline{c}, 1+i= \overline{b}, 2= \overline{d}. That is, z= 1, b= 1- i, c= 1+i, and d= 2. T*(x,y)= (x+ (1-i)y, (1+i)x+ 2y). That happens to be exactly the same as T! This T is "self-adjoint".
I did that directly from the definition of adjoint to show how it works.
It is much simpler to just write this as a matrix:
T= \left[\begin{array}{cc}1 & 1- i \\ 1+i & 2\end{array}\right]
and take the "Hermitian adjoint": first swap row and columns (the "transpose")
T= \left[\begin{array}{cc}1 & 1+ i \\ 1-i & 2\end{array}\right]
then take the complex conjugate of each number.
T= \left[\begin{array}{cc}1 & 1- i \\ 1+i & 2\end{array}\right]
again, we see that T is self adjoint.
For linear transformations on a finite dimensional vector space over the real numbers, where the transformation can be written as a matrix with real number entries, its "adjoint" is the transpose and a linear transformation is "self adjoint" if and only if its matrix form is symmetric.
For linear transformations on a finite dimensional vector space over the complex numbers, where the transformation can be written as a matrix with complex number entries, its "adjoint" is the "Hermitian adjoint" described above. A transformation is "self adjoint" if and only if its matrix form is "Hermitian"- a
mn is the complex conjugate of a
nm.
By the way, if a linear transformation is from a vector space U of dimension m to a vector space V of dimension n, then it can be written as an m by n matrix. Its adjoint is a linear transformation from V to U and can be written as an n by m matrix- again the transpose.
Of course, to be "self adjoint", a matrix must be from vector space U to itself and represented by square matrix.