# Zero Hamiltonian and its energies

1. Nov 27, 2006

Let's suppose we have a Hamiltonian of the form:

$$\bold H =0$$

then it's obivious that if you want to get its energies you would get $$E_{n}=0$$ for every n, this is a non-sense since you must have positive energies (and a ground state) ...then if we "cheat" and make:

$$\bold H \Phi =i\hbar \frac{\partial \Phi}{\partial u}=\lambda_{n} \Phi$$ (2)

where u is a parameter that dictates the "evolution" of the system..of course we must have that $$\frac{\partial H}{\partial u}=0$$

then using (2) we get the energies of the system.. but are they "really" the energies of our initial system with H=0 ??? i don't think so..perhaps we should put $$\lambda=0=\lambda (n_x ,n_y, n_z,n_t)$$ and from it recover the initial energies or consider that the factor..

$$\lambda_{n} \Phi$$ is an extra term inside our potential..:grumpy: :grumpy: how you can quantize H=0 and get finite and positive energies???..

2. Nov 27, 2006

### Epicurus

What physical system would possibly have H=0. In what way would this originate

3. Nov 28, 2006

### dextercioby

There's no way the H could be zero, unless you did something wrong along the way.

Daniel.

4. Nov 28, 2006

### hellfire

You get a zero Hamiltonian for theories that are invariant under reparametrizations, like, for example, a free relativistic particle. H = 0 is a constraint, and at least in principle you can try to quantize it two ways. Either solving the constraints first (obtaining a H different from zero with the new variables) and then applying the quantization procedure, or applying the quantization procedure and imposing the constraints as relations on the Hilbert space.

5. Nov 28, 2006

### dextercioby

H=0 is not a constraint. A constraint is some function of the phase space variables one gets when he cannot invert the Legendre transformation (primary constraint(s)), or when evolution of the primary constraint(s) generates other relation between the momenta and coordinates (secondary constraint(s)).

Daniel.

P.S. For the free relativistic particle one usually works with the einbein formulation specifically to avoid the $\sqrt{\dot{x}^{\mu}\dot{x}_{\mu}}$ ugliness.

6. Nov 28, 2006

### hellfire

I should have said: The total Hamiltonian is a linear combination of the constraints that vanish on the physical subspace. The Hamiltonian for the free relativistic particle is an example of this. Do you agree with this?

7. Nov 28, 2006

### Jheriko

Surely H = 0 for a particle at rest in empty space with no potentials/fields? I dont have a particularly thorough understanding of Hamiltonian mechanics, but here is my logic:

$$H\left(q_j,p_j,t\right) = \sum_i \dot{q}_i p_i - L(q_j,\dot{q}_j,t)$$

Since all the $q_j$ do not change $\dot{q}_j = 0$ and therefore also $p_j = \frac{\partial L}{\partial\dot{q}} = 0$. So we have that

$$H = - L(q_j,\dot{q}_j,t)$$

Since $L = T - V$ we can get $H = V - T$ from the above, and since $H = T + V$ we can create some equations and subtract them, where T is kinetic and V is potential energy:

$$\begin{equation*} \begin{split} H & = T - V\\ & = T + V \end{split} \end{equation*}$$
subtracting
$$0 = V$$

(Does this imply that potential energy must be zero for a particle to remain at rest?)

Since T is the kinetic energy term it should be zero if the particle is at rest and so $H = L = 0$ too? I don't have a good explaination for this without using some classical mechanics or relativistic mechanics... so I am not sure if this applies in the quantum case. Since there is uncertainty in positions and momentums I would guess that a particle always has the possiblity of having kinetic energy, and the nearest we can get to zero is having a distribution of possible energies centred on zero.

Right? Wrong? Ballpark?

Last edited: Nov 28, 2006
8. Nov 28, 2006

### dextercioby

Yes, surely, the Hamiltonian is proportional to the secondary constarint in the einbein formulation.

I'd suggest a path integral quantization for these reparametrization invariant problems. Canonical one is slightly more demanding.

Daniel.

9. Nov 28, 2006

### Epicurus

If you have invariance under reparemtrisations then you gave gauge degress of freedom that have to be fixed. Take the example of the E.M. Field. Integrate the lagrangian by parts, set surface terms to zero to get the lagrangian density L=AG^-1A where G^-1 is the inverse of the Greens function and A is the 4-potential. G^-1 is not invertible, all its eigenvalues are 0, but we have gauge degrees of freedom which need to be fixed (In the path integral formalism, the functional measure contains an infinite term due to U(1) gauge transformations).

In the canonical formalism, this is fixed via the Ghosts fields.

10. Nov 29, 2006

### hellfire

When I talked about "reparametrization invariance" I actually meant "time reparametrization invariance", which, as far as I know, is the usual meaning of this expression. Lagrangians which are invariant under time reparametrizations lead to a zero Hamiltonian. For this to be true, the Lagrangian must be a homogeneous function of the $\dot q$. Then, due to Euler's homogeneous function theorem $(\partial L / \partial \dot q) \dot q = L$, and it follows that the Hamiltonian is zero. As the E.M. Lagrangian is not homogeneous in $\dot q$, its Hamiltonian is not equal to zero.

11. Nov 29, 2006

### Epicurus

Can you please give me an example of the 'time reparametrisation' you are talking about? I want to make sure that we are actually discussing is the same thing and if you are correct

12. Nov 30, 2006

### hellfire

The free relativistic particle:

$$\mathcal{L} = \left( g_{\mu \nu} \frac{\partial x^{\mu}}{\partial \tau}\frac{\partial x^{\nu}}{\partial \tau}\right) ^{1/2}$$

You may be interested in sections 1 and 2 of this lecture notes of Edmund Bertschinger:
http://ocw.mit.edu/NR/rdonlyres/Physics/8-962Spring2002/6D03860E-9C15-4EB8-B96A-8B720D68EFE8/0/gr5.pdf [Broken]

Last edited by a moderator: Apr 22, 2017 at 2:21 PM
13. Nov 30, 2006

### dextercioby

That's a nice reference, Hellfire. IIRC from second year analytical mechanics, in proving the Noether theorem for finitely many degrees of freedom, the evolution parameter is switched from time to an arbitrary "\tau" and the newly obtain action leads to a zero Hamiltonian as well.

Daniel.

14. Nov 30, 2006

### swimmingtoday



<<Wrong?>>

Quite wrong.

First of all, you are not understanding what he Hamiltonian is. The Hamiltonian is not the value of the energy, it is a relationship between position and momentum for a particular system. If the Hamiltonian is p^2 + q^2, and the value of p^2 + q^2 is zero, then the Hamiltonian is p^2 + q^2, not zero. It is analogous to Bush being the president. Bush is the current VALUE of "president", but the concept of president is not synonymous with "Bush".

As for how you got the obviously wrong result that the the potential energy must be zero for any particle at rest, you need to remember that your initial assumption was that he energy (what you referred to as the Hamiltonian) was zero and that he momentum was zero. So being that you made these assumptions earlier in the derivation, is is not surprising that you reached the result that the potential energy was zero. But you seen to have not realized that you had assumed more than just that the particle was at rest, you also assumed that he energy was zero.

15. Nov 30, 2006

### reilly

Zero is zero is zero. 'Nothin from nuthin' is nuthin' (with apologies to the late, great Billy Preston) If H=0 is an operator equation, then "next please". A universally null oR constant operator is of virtually no interest -- what's it good for? Why bother? Every matrix element of a null operator is zero.All eigenvalues of a null operator are zero."Next in line please."

On the other hand, if zero is an eigenvalue among other non-zero ones, all bets are off.

Regards,
Reilly Atkinson

16. Nov 30, 2006

### swimmingtoday

We might be in agreement. What caused you to think otherwise?

17. Dec 1, 2006

### Jheriko

I assumed the the kinetic energy, momenta and first derivatives of the coordinates are zero. The only assumptions I made regarding the Hamiltonian are:
$$H\left(q_j,p_j,t\right) = \sum_i \dot{q}_i p_i - L(q_j,\dot{q}_j,t)$$
and
$$H = T + V$$
I don't see how I started out assuming H was zero, unless at least one of the above assumptions is indentical with H=0.

The real error in my maths is that I swapped the order of T and V without noticing in one place, hence all that my working really shows is that the kinetic energy is zero, which was one of my starting assumptions.

$$\begin{equation*}\begin{split}H & = T - V\\ & = T + V\end{split}\end{equation*}$$

should have been

$$\begin{equation*}\begin{split}H & = V - T\\ & = T + V\end{split}\end{equation*}$$

Which shows that the kinetic energy is zero and that the Hamiltonian is only made up of the potential energy term, which is just a direct consequence of my starting assumptions anyway...

I still don't see any good reason why H can not be zero. If it is equivalent to the sum of potential and kinetic energies, then a classical particle in free space at rest with no potentials will have H = 0. Perhaps what I am missing is knowing how to go from a classical Hamiltonian to a quantum one... I have been reading some books that cover the topic, but I haven't made much progress yet... the mathematical hurdles are quite high for me.

Last edited: Dec 1, 2006
18. Dec 1, 2006

### swimmingtoday

<<I don't see how I started out assuming H was zero, unless at least one of the above assumptions is indentical with H=0.>>

You're right--I was wrong in saying you did that. I went back to your post and found the actual error--it was just a dropping of a minus sign.

<<The real error in my maths is that I swapped the order of T and V without noticing in one place, hence all that my working really shows is that the kinetic energy is zero, which was one of my starting assumptions.
>>

Exactly. I went back to your original post after reading the beginning of your current post, and that is exactly what happened: You argued that when p and q dot were zero, as when the particle is at rest, that the formulala for H gives H = L. You dropped a minus sign. It should have been H = negative L. Proceeding with the minus sign error you set L= T-V to the standard Hamiltonian formula H= T +V, and got T-V = T+V, yielding V=0. However, if the minus sign was not inadvertantly dropped ypou would have argued negative (T-V) = (T+V), which gives the correct result that T (rather than V) equals zero when p and q dot are zero.

<<I still don't see any good reason why H can not be zero. If it is equivalent to the sum of potential and kinetic energies, then a classical particle in free space at rest with no potentials will have H = 0. >>

It's largely a matter of a tricky definition. The Hamiltonian of a particle is a relationship between a particle's position and its momentum, that when calculated out would give its energy. The energy is the actual *number* you get when you do the calculation. The Hamiltonian is a recipe, and the energy is the number you get applying the recipe .

Consider a harmonic oscillator. The Hamiltonian is (p^2)/2m + (k/2)x^2. And suppose it happened to have values of p=0 and x=0. If you are asked "What is the energy of the systen?" you have to answer that the energy is zero. If you are asked "What is the Hamiltonian of the systen?" you have to answer that the Hamiltonian is (p^2)/2m + (k/2)x^2..

As I said earlier, it is like Bush being the president. "President" is like the Hamiltonian, and "Bush" is like the energy. The President is a person with certain powers, and Bush happens to be that particular person under the situation we have before us. But the words "Bush" and "President" do not mean the same thing, just as "Hamiltonian" and "energy" do not mean the same thing.

19. Dec 1, 2006

### Jheriko

I understand what you are saying, but I don't think it is particularly relevant or insightful... the Hamiltonian may be identified with an equation which allows you to derive useful equations of motion, but that doesn't reduce the validity of a statement like H=0. Regardless as to what useful things you can do in whatever form any expression takes, it doesn't invalidate the fact that you can evaluate said expression and write an identity just like H=0.

If my notation or terminology is non-standard, then the standard is needlessly confusing imo since there is nothing real to gain by making such a distinction. (Other than confusing me )

So I am still curious as to why it is that some of the responses have indicated that a Hamiltonian which evaluates to zero is a such a flawed concept, since there hasn't been an actual explanation given. Given that H = T + V it would seem that a particle at rest in empty, potential free space, would always have H evaluate to zero, at least classically. I really can't see anyway that this can be wrong so I am going to need someone to point out the "what probably should be obvious".

20. Dec 1, 2006

### swimmingtoday

I should point out that it is not me that came up with the way the terms are used!

Here though is why a distinction is made between "the Hamiltonian" and "the energy".

Hamilton's equations are dH/dp = q dot, dH/dq = p dot. (The derivatives are partial derivatives; and I don't care about factors of negative one) If you have a harminic oscillator with an energy of 14, then inserting "14" for H in Hamilton's equations gives q dot= 0, p dot =0, because the derivative of a constant ( "14" is a constant, rather than a function of p and q) is zero. So for H in Hamilton's equations, you cannot use the value of the energy, but ratther the Hamiltonian recipe for energy as a function of p and q.

Likewise in quantum physics if you want to find the averged time derivative of a physical quantity by taking the commutator of the operator for that quantity with the Hamiltonian operator you cannot use "14" as the Hamiltonian operator if 14 is the value of the energy-- a *number* such as 14commutes with anything. You need to write out the Hamiltonian Operator in terms of position and momentum operators.