Temporaly uncertainty principle

[IRobot]

Hi, I am currently having problems solving a an exercise:
Let's make the assumption of the existence of an operator H such as [T,H]=i \hbar I.
by examining the state: |\psi\rangle}=He^{i \alpha T}|E\rangle} with H|E\rangle}=E|E\rangle}
show that the spetrum of H is not bounded below.

 

[Fredrik]

The idea is to show that for all \alpha, e^{i\alpha T}|E\rangle is an eigenstate of H with an eigenvalue that can be given any value you want by an appropriate choice of \alpha. To do this, you need to find the commutator [H,e^{i\alpha T}].

 

[IRobot]

Thank you Fredrik, it works well ;)

 

[Demystifier]

See also Sec. 3 of
http://xxx.lanl.gov/pdf/quant-ph/0609163v2
especially Eqs. (9)-(13).

 

[tom.stoer]

I suspect that such an operator T does not exist in general

 

[Fredrik]

I suspect that such an operator T does not exist in general

I think that's the point of this exercise. If it does exist, the Hamiltonian isn't bounded from below. This would mean e.g. that atoms don't have a ground state.

 

[naima]

The KG hamiltonian is not bounded from below but I never read one such T with it.

 

[tom.stoer]

The KG hamiltonian is not bounded from below but I never read one such T with it.

:-)

As far as I understand the idea is to show that given T with [T, H] = i one can show that H is not bounded from below; not the other way round that given H is not bounded from below one should construct T.

As a simple exercise one could try to construct T for the simple harminic oscillator

H = a^\dagger a + \frac{1}{2}

and check where this construction fails

 

[Fredrik]

The KG hamiltonian is not bounded from below but I never read one such T with it.

Isn't the vacuum state a minimum energy state?

 

[naima]

The Klein Gordon hamiltonian expressed with annihilation and creation operators
contains a term proportional to Dirac delta function.
After ignoring it (changing the Hamiltonian) one can find a ground state.
Refer to Peskin and Schroeder on page 21-22.
I hope i understand id correctly.

 

[dextercioby]

Hi, Naima, you are absolutely correct. The <natural quantization of the KG field> delivers a Hamiltonian operator not bounded from below. We then use the trick of <normal ordering> to get the physical boundedness from below of the spectrum of H.

 

[dextercioby]

I think that's the point of this exercise. If it does exist, the Hamiltonian isn't bounded from below. This would mean e.g. that atoms don't have a ground state.

Hi, Fredrik, Hrvoje, Tom and the rest of the crew. There was another thread last week briefly touching Pauli's theorem of 1926. I know I'm kind of repeating myself, but I say once more, probably this time more precisely and naming Eric Galapon to be responsible with the juicy math stuff.

Given the operator relation [T,H]=i1 valid on some properly chosen subset of a complex separable Hilbert space (or the antidual of this set wrt to some topology, if one uses RHS), H being a properly defined self-adjoint Hamiltonian with a spectrum bounded from below, one cannot conclude that there does not exist a self-adjoint T operator (let's call it <time operator>, because its spectral values are measured in seconds in the SI units) 'canonically conjugate to the Hamiltonian'. Rephrasing, T exists as a self-adjoint linear operator.

Such a statement is proved by simply building 2 operators -H and T- with the aforementioned properties for a quantum system.

Case closed.

 

[Fredrik]

Hi, Fredrik, Hrvoje, Tom and the rest of the crew. There was another thread last week briefly touching Pauli's theorem of 1926. I know I'm kind of repeating myself, but I say once more, probably this time more precisely and naming Eric Galapon to be responsible with the juicy math stuff.

Given the operator relation [T,H]=i1 valid on some properly chosen subset of a complex separable Hilbert space (or the antidual of this set wrt to some topology, if one uses RHS), H being a properly defined self-adjoint Hamiltonian with a spectrum bounded from below, one cannot conclude that there does not exist a self-adjoint T operator (let's call it <time operator>, because its spectral values are measured in seconds in the SI units) 'canonically conjugate to the Hamiltonian'. Rephrasing, T exists as a self-adjoint linear operator.

Such a statement is proved by simply building 2 operators -H and T- with the aforementioned properties for a quantum system.

Case closed.

That's interesting. Thanks for the information, and for spelling my name right. That only happens about 5% of the time, even though it's right there on the screen.

Do you understand why this exercise seems to prove that such a T can't exist? I mean, do you know what parts of the reckless proof are invalid? I mean this reckless proof:

The commutation relation [T,H]=i implies [T^n,H]=niT^{n-1}. From this we get

[H,e^{iaT}]=\left[H,\sum_{n=0}^\infty\frac{(iaT)^n}{n!}\right]=\sum_{n=1}^\infty\frac{(ia)^n}{n!}[H,T^n]=a\sum_{n=1}^\infty\frac{(ia)^{n-1}}{(n-1)!}T^{n-1}=ae^{iaT}

He^{iaT}|E\rangle=(e^{iaT}H+[H,e^{iaT}])|E\rangle=(E+a)e^{iaT}|E\rangle

 

[dextercioby]

Well, it's incredibly easy to see what's wrong in the <proof> in the post 13. The domain of the commutator between T and H is equal to the domain of the commutator between H and exp (iaT) and does not contain the 'eigenvectors' of the Hamiltonian. Thus, under these circumstances, the last line of what Fredrik wrote makes no sense.

 

[tom.stoer]

The domain of the commutator between T and H is equal to the domain of the commutator between H and exp (iaT) and does not contain the 'eigenvectors' of the Hamiltonian.

Why? Can you elaborate?
In this case already the equation [T, H] = i would be wrong; it would have to contain a projector on the r.h.s. As it's written here it is defined globally.

What I see immediately is that the spectrum must not be discrete as otherwise the new state |E+a> would no longer has the chance to be an eigenstate. Looking at the same calculation for the operators x and p the shift |p> to |p+a> is valid; that means that p is not bounded from below; what goes wrong with this argument when using H?

 

[dextercioby]

[T,H]=i1 is not a global relation, it holds only on some subset of a Hilbert space. And the Hilbert space needn't be the L^2 on whole of R, but only on a subset of it. This means that T and H may be conjugate to one another, but they needn't be a system of imprimitivities on the real line, as the Q and P operator for the free particle are.

It actually turns out that the commutation relation does not imply that the spectrum of the Hamiltonian is necessarily continuous, so a thorough analysis can be made without resorting to rigged Hilbert spaces. The same commutation relation doesn't imply that both operators be unbounded, one of them can be bounded.

For the maths I refer you to the article by E. Galapon published in Proc.Roy.Soc. Lond. A, volume 458, page 2671 and the theorem 4.1 on the page 2687.

 

[tom.stoer]

Why? Can you give me an example where it fails (I mean on the original Hilbert space, not on its dual)?

 

[dextercioby]

Why? Can you give me an example where it fails (I mean on the original Hilbert space, not on its dual)?

Sorry, I've changed my post. It took a lot to write it and the system logged me off. A thorough analysis has been included in the article I've sent reference to. Actually there's a series of articles which should serve as a back up, all of them written by Eric Galapon.

 

[tom.stoer]

I don't think we need a thorough analysis and a lot of math.

The original post talks about T, H and [T, H]=i. Of course H should become a Hamiltonian eventually, but currently we do not need this interpretation; we do neither need properties like self-adjointness.

I would rather turn the whole story round and ask about properties of H that are enforced or preculed by the relation [T, H]=i

Looking at x and p the situation is rather trivial. One can use

x \to x
p \to -i\partial_x
[x,p]=i \to [x, -i\partial_x]\psi(x) = -i(x\partial_x - \partial_x x)\psi(x) = i(\partial_x x)\psi(x) = i\psi(x)

In that sense there is no problem with the argument; all one needs is the definition of the two operators. Now one can check whether the relation [T, H]=i enforces properties on H which preclude H from being a reasonable Hamiltonian.

 

[Fredrik]

I think this is also relevant here:

Now suppose that two hermitian operators have a commutator that's proportional to the identity operator: [A,B]=cI, and eigenvectors satisfying A|a>=a|a> and B|b>=b|b>.

1=\frac c c\langle a|a\rangle=\frac 1 c\langle a|cI|a\rangle=\frac 1 c\langle a|[A,B]|a\rangle=\frac 1 c\langle a|(aB-Ba)|a\rangle=0

(Thanks to George Jones for posting this in some other thread).

The same thing happens if we use |b> instead of |a>. What this means is that two hermitan operators that satisfy such a commutation relation (like x and p) can't have eigenvectors. Bounded hermitian operators always do, so this is one way to see that x and p must be unbounded.

 

[dextercioby]

What's wrong in that line that determines you to conclude that 1=0 ?

 

[tom.stoer]

I think this is also relevant here:

Of course you have to avoid sandwiching!

 

[dextercioby]

I don't think we need a thorough analysis and a lot of math.

The original post talks about T, H and [T, H]=i. Of course H should become a Hamiltonian eventually, but currently we do not need this interpretation; we do neither need properties like self-adjointness.

I would rather turn the whole story round and ask about properties of H that are enforced or preculed by the relation [T, H]=i

[...]

In that sense there is no problem with the argument; all one needs is the definition of the two operators. Now one can check whether the relation [T, H]=i enforces properties on H which preclude H from being a reasonable Hamiltonian.

What are the properties which would "preclude H from being a reasonable Hamiltonian" ? Could you, please, spell them out ? Thank you

 

[tom.stoer]

H should be self adjoint or at least symmetric; H should allow for "generalized eigenvectors"; H should be bounded from below; in QFT H should be "finite after normal ordering / regularization".

 

[dextercioby]

Do you agree then with the claim that assuming [T,H]=i1 on some subset of a Hilbert space/RHS, with T a s-adj operator and H satisfying all your requirements, doesn't lead to any inconsistencies, both mathematically and physically ?

 

[tom.stoer]

Do you agree then with the claim that assuming [T,H]=i1 on some subset of a Hilbert space/RHS, with T a s-adj operator and H satisfying all your requirements, doesn't lead to any inconsistencies, both mathematically and physically ?

a) I do not understand why you are talking about a subset
b) I guess that - coming back to the original post - one can show that the requirement of H being bounded from below is in conflict with [T,H]=i1 (of course I would keep H and forget about T)
So except for the subset in a) and ruling out the existence of T accoring to b) I do not have a problem

 

[Fredrik]

What's wrong in that line that determines you to conclude that 1=0 ?

As you can see in the text after that line, I was thinking that the problem wasn't in that line, but in the assumptions before it, in particular the assumption that two operators with a commutator like that can both have eigenvectors. But now I'm thinking that since |b> doesn't appear in that line, that explanation can't be right. Based on what you said before, I guess it has to be that if A has an eigenvector, it can't be in the domain of B.

a) I do not understand why you are talking about a subset

Unbounded operators are usually (always?) defined on a dense subset of the Hilbert space, not on the entire space. Suppose e.g. that Q is defined by Qf=xf for all functions f in L²(ℝ). Then Qf isn't square integrable for each choice of f. To ensure that the range of this linear operator doesn't contain any functions that are outside of L²(ℝ), we must choose its domain to be a proper subset of L²(ℝ).

b) I guess that - coming back to the original post - one can show that the requirement of H being bounded from below is in conflict with [T,H]=i1 (of course I would keep H and forget about T)
So except for the subset in a) and ruling out the existence of T accoring to b) I do not have a problem

The proof assumes that |E> is in the domain of T, which implies that 1=0. I'd call that a problem.

1=\langle E|E\rangle=-i\langle E|iI|E\rangle=-i\langle E|[T,H]|E\rangle=-iE\langle E|(T-T)|E\rangle=0

Hey, wait a second, this also implies that [T,H]=iI is impossible. It might make sense if we replace the identity operator with its restriction to the domain of T, but it doesn't make sense as it stands.

 

[tom.stoer]

Unbounded operators are usually (always?) defined on a dense subset of the Hilbert space, not on the entire space. Suppose e.g. that Q is defined by Qf=xf for all functions f in L²(ℝ). Then Qf isn't square integrable for each choice of f. To ensure that the range of this linear operator doesn't contain any functions that are outside of L²(ℝ), we must choose its domain to be a proper subset of L²(ℝ).

The problem is to use L²(ℝ)

 

[Fredrik]

The problem is to use L²(ℝ)

Since all infinite-dimensional complex separable Hilbert spaces are isomorphic to L²(ℝ), I don't think you can solve any problems of this magnitude by using a different Hilbert space.

 

[tom.stoer]

Hey, wait a second, this also implies that [T,H]=iI is impossible. It might make sense if we replace the identity operator with its restriction to the domain of T, but it doesn't make sense as it stands.

But the problem is not |E> but sandwiching H and T between |E>, or simply writing down <E|!

Please do the same for x and p; there is no problem with x and p and there is no problem with [x,p] acting on a wave function; the problem is sandwiching [x,p] between |p> states!