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In the late nineties Bender has started a research program on what is called PT symmetric QM, or non hermitian QM, in which he has shown that if the hamiltonian enjoys a PT symmetry then the spectrum is real even if the hamiltonian was not hermitian. Now a search for "PT symmetric" on the arxiv will return over 400 papers.

This relaxation of the hermiticity of the hamiltonian has led to new forms of hamiltonians that have been rejected before because they were non hermitian. It turns out that such PT symmetric hamiltonians can describe real physical systems.

Since this PT symmetric QM cannot be considered a generalization to conventional quantum mechanics I suppose in which observables are mathematically represented by hermitian operators, I find it intriguing that something like this can describe real physical systems. So how can one understand PT symmetric QM from first principles? I mean how does it fit in the grand picture, why it works?

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Quoting Ali Mostafazadeh in arXiv:quant-ph/0307059:

It can also be shown that whenever $H$ is a diagonalizable operator with a real spectrum, then it can be mapped to a Hermitian operator via a similarity transformation.

The $PT$-symmetric operators are of this type.

Though I haven't read it (yet), arXiv:0810.5643 by the same author should answer your questions in detail.

Update: Skimming over the article, I found the following remark:

The main disadvantage of employing the Hermitian representation is that in general the Hamiltonian $h$ is a terribly complicated nonlocal operator. Therefore, the computation of the energy levels and the description of the dynamics are more conveniently carried out in the pseudo-Hermitian representation. In contrast, it is the Hermitian representation that facilitates the computation of the expectation values of the physical position and momentum operators as well as that of the localized states in physical position or momentum spaces.

Note that the Klein-Gordon field is probably a good example for this, whose treatment in terms of classical quantum mechanics is the subject of the first paper I linked.

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It is the formulation of Hamiltonian QM in a nontraditional inner product, in which certain (in the standard inner product) nonhermitian Hamiltonians become selfadjoint.

Calling it a generalization of QM is not appropriate. It has very little impact on most of quantum mechnaics, and is nothing of general interest, just a theoretical playground for afficionados.

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Yeah but my question is, we know that nature is quantum mechanical, the quantum mechanics of usual hermitian operators that guarantee the reality of the eigen values. Now since this nonhermitian quantum mechanics turns out to have applications and was checked experimentally, why is that? is nature also nonhermitian quantum mechanical? –  Revo Aug 17 '12 at 11:34
    
By a nonunitary similarity transformation, the PT-symmetric Hamiltonian becomes hermitian. This corresponds to a change of the inner product. Thus nature is quantum mechanical, and in a few cases, this can be expressed in terms of a noncanonical inner product and a corrresponding PT-symmetric Hamiltonian. Nothing fundamentally new is going on. –  Arnold Neumaier Aug 17 '12 at 12:18
    
I am perplexed, so what is the usefulness of that if it is mere transformations, what advantages do we gain? Why 400 publications, some of them with physical applications? –  Revo Aug 17 '12 at 12:43
    
People need publications for their career, so everything novel in some respect is published. Most of what is published in every field of science is of interest only for a tiny minority of scientists. –  Arnold Neumaier Aug 17 '12 at 13:16
    
@Revo: In the present case, the merit is that the PT-Hamitonian may have a much simpler form (and consequent analysis) than the corresponding standard Hamiltonian. But the interpretative framework of QM is exactly the same. –  Arnold Neumaier Aug 17 '12 at 13:17
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My experience is based on pseudo hermitian hamiltonians, which are reducible to an hermitian one, but they end up to be complicated hamiltonians that are generally not interpretable from a physics point of view.

Hermitian hamiltonians are more physical in the sense of reciprocity of the interaction; the interaction of 2 on 1 is also the interaction of 1 on 2.

The mathematics of pseudo hermitian quantum physics is not new at all; it reduces to a Sturm Liouville formalism that is a natural generalization of Schrodinger.

Therefore I think that workers in this field have quite a struggle ahead of them to make any of this really usefull or novel.

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