Hermitian Operator: AB Hermitian if [A,B]=0

alisa
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show that if A and B are both Hermitian, AB is Hermitian only if [A,B]=0. where or how do io start?
 
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From the property (AB)+=B+a+

+ denoting hermitian conjugation
 
alisa said:
show that if A and B are both Hermitian, AB is Hermitian only if [A,B]=0. where or how do io start?

Expand [A,B]=0, then use the hint above.
 
Here's how i'd do it. Consider the scalar product

\langle x, AB y\rangle (1)

for "x" unspecified yet and y\in D(AB), \overline{D(AB)}=\mathcal{H} an arbitrary element.

\langle x, AB y\rangle = \langle x, A^{\dagger}B y\rangle (2)

,where D(A^{\dagger}B)=D(AB), since D(A)\subseteq D\left(A^{\dagger}\right)

\langle x, A^{\dagger}B y\rangle =\langle x, A^{\dagger}B^{\dagger} y\rangle (3)

as B\subseteq B^{\dagger}. Therefore y\in D\left(A^{\dagger}B^{\dagger}\right) and D(AB)\subseteq D\left(A^{\dagger}B^{\dagger}\right).

\langle x, A^{\dagger}B^{\dagger} y\rangle =\langle Ax, B^{\dagger} y\rangle (4),

if x\in D(A).

\langle Ax, B^{\dagger} y\rangle =\langle BAx, y\rangle (5),

if x\in D(BA)\subseteq D(A).

\langle BAx, y\rangle=\langle ABx, y\rangle (6),

since, by hypothesis AB=BA.
Finally

\langle ABx, y\rangle =\langle x, \left(AB)^{\dagger}y\rangle(7)

by the definition of the adjoint. Therefore y\in D\left((AB)^{\dagger}\right) and

ABy=(AB)^{\dagger} y {} \wedge D(AB)\subseteq D\left((AB)^{\dagger}\right) (8),

which means the operator AB is symmetric/hermitean.

QED.
 
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dextercioby said:
Here's how i'd do it. Consider the scalar product

\langle x, AB y\rangle (1)

for "x" unspecified yet and y\in D(AB), \overline{D(AB)}=\mathcal{H} an arbitrary element.

\langle x, AB y\rangle = \langle x, A^{\dagger}B y\rangle (2)

,where D(A^{\dagger}B)=D(AB), since D(A)\subseteq D\left(A^{\dagger}\right)

\langle x, A^{\dagger}B y\rangle =\langle x, A^{\dagger}B^{\dagger} y\rangle (3)

as B\subseteq B^{\dagger}. Therefore y\in D\left(A^{\dagger}B^{\dagger}\right) and D(AB)\subseteq D\left(A^{\dagger}B^{\dagger}\right).

\langle x, A^{\dagger}B^{\dagger} y\rangle =\langle Ax, B^{\dagger} y\rangle (4),

if x\in D(A).

\langle Ax, B^{\dagger} y\rangle =\langle BAx, y\rangle (5),

if x\in D(BA)\subseteq D(A).

\langle BAx, y\rangle=\langle ABx, y\rangle (6),

since, by hypothesis AB=BA.
Finally

\langle ABx, y\rangle =\langle x, \left(AB)^{\dagger}y\rangle(7)

by the definition of the adjoint. Therefore y\in D\left((AB)^{\dagger}\right) and

ABy=(AB)^{\dagger} y {} \wedge D(AB)\subseteq D\left((AB)^{\dagger}\right) (8),

which means the operator AB is symmetric/hermitean.

QED.

wouldn't it be easier to just say that x,y are in the domain of the operators A, B (which i agree IS important to state, as is actually applying the operator to an element as opposed to treating it as some "algebraic" quantity as many books do)? in which case the proof would reduce to about 4 lines. in other words, when would the domain of A and its hermitian conjugate NOT be the same?
 
alisa said:
show that if A and B are both Hermitian, AB is Hermitian only if [A,B]=0. where or how do io start?

Dear alisa, Does it go like this?

Let |n> be an eigenstate of A and B. Then:

AB|n> = Abn|n> = bn.an|n>.

Therefore AB is hermitean because bn.an is real.

In a similar expansion you will find that: [A, B]|n> = 0.

So, given |n>, AB is hermitean and [A, B] = 0.

This should point you in the right direction; check it out, wm
 
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quetzalcoatl9 said:
in which case the proof would reduce to about 4 lines.

I don't know about that. I don't claim that my proof is unique/the shortest possible.

quetzalcoatl9 said:
in other words, when would the domain of A and its hermitian conjugate NOT be the same?

By the Hellinger-Toeplitz theorem, iff the operator A is bounded. My proof accounts for the arbitrary character of the A and B operators.
 
wm said:
Dear alisa, Does it go like this?

Let |n> be an eigenstate of A and B. Then:

AB|n> = Abn|n> = bn.an|n>.

Therefore AB is hermitean because bn.an is real.

In a similar expansion you will find that: [A, B]|n> = 0.

So, given |n>, AB is hermitean and [A, B] = 0.

This should point you in the right direction; check it out, wm


The spectrum of a hermitean operator is not necessarily real. Actually only the eigenvalues (points in the pure point spectrum) are real, however, one cannot guarantee that |n\rangle is an element of the Hilbert space. Therefore one cannot guarantee that "a_{n}b_{n}" is real. And even if it was real, there are examples of nonhermitean operators with real spectral values.
 
dextercioby said:
The spectrum of a hermitean operator is not necessarily real. Actually only the eigenvalues (points in the pure point spectrum) are real, however, one cannot guarantee that |n\rangle is an element of the Hilbert space. Therefore one cannot guarantee that "a_{n}b_{n}" is real. And even if it was real, there are examples of nonhermitean operators with real spectral values.

Dear dextercioby, At alisa's level I thought it might go like this:

Let

(1) A|x> = a|x>. If A is hermitean then (by definition):

(2) <x|A|x> = <x|A|x>*. Substituting (1) into (2):

(3) <x|a|x> = <x|a|x>*; ie,

(4) a<x|x> = a*<x|x>; ie,

(5) a = a*; ie, a is real (zero being excluded as trivial).

Thus, in the example that I gave: bn.an is real (because each factor is real).

Would that be satisfactory at alisa's level? wm
 
  • #10
I don't know Alisa's level of education. And in this case i'd rather make no assumption, unlike you.
 
  • #11
dextercioby said:
I don't know Alisa's level of education. And in this case i'd rather make no assumption, unlike you.

Dear dextercioby, With alisa's best interests in view, may I suggest that you alert her to the ''level of education'' at which my analysis fails?

Thanks; and best regards, wm
 
  • #12
Your analysis is mathematically faulty. At best it can be considered a heuristic approach with made with disputable arguments. But this is already off-topic, so i'd say "let's drop it".
 
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