Would it matter which inner product I choose in quantum mechanics?

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SUMMARY

The choice of inner product in quantum mechanics is crucial as it directly influences the formalism of the theory. The standard inner product is defined as $$\int^{∞}_{-∞}\psi^{*}\psi\;dV$$, which maps elements in Hilbert space to real numbers. This inner product is derived from the Dirac formalism, where normalized states and position eigenstates form a complete basis. The mathematical structure of quantum mechanics is inherently linked to separable Hilbert spaces, specifically isomorphic to ##L^2 (\Omega)##, which restricts the choice of inner products.

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patric44
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it seems that quantum mechanics formalism is dependent on the inner product
hi guys
i was thinking about the inner product we choose in quantum mechanics to map the elements inside the hilbert space to real number which is given by :
$$\int^{∞}_{-∞}\psi^{*}\psi\;dV$$
or in some cases we might introduce a weight function dependent on the wave functions i have , it seems that if i had chosen another completely different inner product the formalism of quantum mechanics will be different ?! , is there a particular reason for that inner product that we use in QM or choosing adiffernt inner product will not change any thing and why .
thanks
 
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patric44 said:
Summary:: it seems that quantum mechanics formalism is dependent on the inner product

hi guys
i was thinking about the inner product we choose in quantum mechanics to map the elements inside the hilbert space to real number which is given by :
$$\int^{∞}_{-∞}\psi^{*}\psi\;dV$$
or in some cases we might introduce a weight function dependent on the wave functions i have , it seems that if i had chosen another completely different inner product the formalism of quantum mechanics will be different ?! , is there a particular reason for that inner product that we use in QM or choosing adiffernt inner product will not change any thing and why .
thanks
The (position space) wave function and associated inner product may be derived from the general Dirac formalism:

We have a normalised state ##|\alpha \rangle## and the position eigenstates ##|x \rangle##, which form a complete basis:$$\int dx \ |x \rangle \langle x| = I$$ Hence:
$$ 1 = \langle \alpha | \alpha \rangle = \int dx \ \langle \alpha|x \rangle \langle x|\alpha \rangle$$
We now define the position space wave-function:
$$\psi(x) = \langle x|\alpha \rangle$$ which leads to:
$$\int dx \ \psi(x)^*\psi(x) = 1$$ and all the other formulas involving the wave-function.

In that sense, the inner product is determined by the formalism.
 
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thank you so much it becomes clear now
 
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That the choice of inner product is limited is a consequence of the famous mathematical statement: All infinite-dimensional complex separable Hilbert space are isomorphic to ##L^2 (\Omega)##, where ##\Omega## stands for an open subset of ##\mathbb{R}^n## endowed with a measure. Precisely because of this fact, QM works with separable Hilbert spaces (add to that the spectral theorem).
 
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dextercioby said:
That the choice of inner product is limited is a consequence of the famous mathematical statement: All infinite-dimensional complex separable Hilbert space are isomorphic to ##L^2 (\Omega)##, where ##\Omega## stands for an open subset of ##\mathbb{R}^n## endowed with a measure. Precisely because of this fact, QM works with separable Hilbert spaces (add to that the spectral theorem).

It's probably not that limiting, since it means even 3+1D relativistic QFT and quantum gravity (if they exist) have ##L^2 (\Omega)## as the Hilbert space.
 
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