Can a Hamiltonian be unbounded ?

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SUMMARY

The discussion centers on the properties of Hamiltonians in one-dimensional quantum systems, specifically whether a Hamiltonian of the form H=p^2 + V(x) can be unbounded and possess negative energies. It is established that a Hamiltonian must be bounded from below to ensure system stability; otherwise, perturbations could lead to decay into singular states with infinite particles. The consensus is that in quantum field theory (QFT), boundedness from below is a necessary postulate for an acceptable Hamiltonian, while in nonrelativistic physics, it is derived for each system analyzed.

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zetafunction
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the idea is can a Hamiltonian in 1-D of the form H=p^2 + V(x) for a certain function V(x) be unbounded and have NEGATIVE energies , for example a Hamiltonian whose spectra may be E_{n} = ...,-3,-2,-1,1,2,3,... and so on, so we have an UNBOUNDED Hamiltonian with positive and negative energies with the property

E_{-n}=-E_{n}
 
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I think a Hamiltonian must always be bounded from below, b/c otherwiese it would be possible (e.g. due to perturbations) that there is a non-zero possibility for a state |n> to decay to |n-k>, where n is not bounded from below. So the whole system is unstable and decays into a singular state plus infinitly many photons, phonons or whatever.
 
In QFT, boundedness from below is a postulated for an acceptable Hamiltonian. In nonrelativistic physics, it is a derived result for each analyzed system.
 

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