Re: The time it takes to emit one photon
- From: Igor Khavkine <igor.kh@xxxxxxxxx>
- Date: Wed, 7 Sep 2005 06:26:44 +0000 (UTC)
On 2005-09-02, Eugene Stefanovich <eugenev@xxxxxxxxxxxx> wrote:
> Igor Khavkine wrote:
>> Quantization of a regular field theory yields a bosonic quantum field
>> theory, whose excitations translate to identical particles with
>> symmetrized wave functions. Quantization of a Grassmann field theory
>> yields a fermionic quantum field theory, whose excitations translate to
>> identical particles with antisymmetrized wave functions.
>> Field approach: 1, particle approach: 0.
>
> You may be right here. The identity of electrons looks
> more natural in the field approach.
> But the QM postulate that two electrons are
> identical doesn't seem so unreasonable to me. Why in the world they
> should be different?
But why in the world should they be the same? The matter of fact is that
a particle theory can handle both possibilities. The identical particle
principle is empirically selected by fitting experiments (cf. Gibbs
paradox). The field formulation is more predictive, since it is only
consistent with a particle formulation supplemented by the identical
particle principle. If you dislike ad-hoc rules, then field theory is
coming out a clear winner.
>> False attack on QED. Its Hamiltonian is there to calculate for anyone
>> who cares/dares.
>
> This "anyone" would have a hard time calculating the time evolution of
> real particles using a Hamiltonian written in terms of bare particles
> and with infinite coefficients. Good luck!
Luck has nothing to do with this, and neither do infinite bare
coefficients. Let me supplement my earlier statement. "QED's Hamiltonian
is there to calculate for anyone competent who cares/dares."
Igor
.
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