Dark matter and QFT

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My understanding is that the particle is a somewhat artificial notion in QFT (see: Quantum Mechanics: Myths and Facts), and that in general it is possible for a quantum field to have unstable excitations that don't look anything like particles. Is this an active field of research (what is it called)? Are there experimental searches for detection of such non-particles? For example, could dark matter be non-matter: some large-scale unstable oscillation of a quantum field?

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user user1247

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There is nothing artificial about particles as quanta of a field. Each finite-energy configuration of a quantum field may be written as a complex linear superposition of $N$-particle states with various values of $N$. A general and generic state in the Hilbert space isn't an eigenstate of the "number of particles operator" but that's true for any other observable, too: most states in the Hilbert space aren't eigenstates of a predetermined operator.

This is not a "problem"; it just means that if the observable expressed by the operator is measured, one may get different values as the result of the measurement. The probabilities of individual results are calculated using the standard quantum formula – the Born rule – as the squared absolute values of the complex probability amplitudes (inner products of the state vector with an eigenstate etc.).

In nonlinear field theories, one may often write down classical solutions called "solitons" which are stationary yet localized; there also exist quantum states in the Hilbert space whose support is close to the classical solution. Magnetic monopoles are a good example. Strictly speaking, the quantum states corresponding to these solitons may still be formally written down as combinations of the usual $N$-particle states but this way of writing them becomes useless because the nonlinearities in the equations of motion for the fields totally change the expected behavior relatively to a free field theory for which the $N$-particle-state basis is most useful.

If the fields are only excited by field modes with a long (macroscopic) wavelength, the interpretation in terms of ordinary particles becomes – in contrast with your expectations – most appropriate. The long wavelength is interpreted as the particles' having a very low momentum.

There is no "active field of research" of the type you suggest. Instead, the field you are describing is "learning the first classes in a basic undergraduate course of quantum mechanics". For example, if the dark matter is composed of neutralinos, they're the excitations of an ordinary fermionic field $\chi(x,y,z,t)$ transforming as a spinor, and the basis with $N$-particle states of several neutralinos with different momenta is a perfectly valid basis of the whole Hilbert space and it is therefore enough to describe anything that may physically occur to this field.

I have mentioned solitons. Dark matter could perhaps be made of solitons except that I am not aware of any viable models of this kind.

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user Luboš Motl
answered Feb 25, 2013 by (10,178 points)
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Maybe you mean something like Howard Georgi's unparticle theory, see here or here for example?

This is a high energy theory which extends the standard model by an additional scale invariant sector of particles whose properties such as energy, momentum, and mass can simultaneously be scaled up or down (therefore the term scale invariant). In the standard model, these would only work for photons which are massless.

These new particles, if there are expected to coupling only weakly with "normal" matter at low observable energy scales and behave some kind of similar to neutrinos. At the LHC, such unparticles would for example become noticeable by missing energy. There are indeed ideas, that dark matter could be made of such unparticles, see for example this paper.

answered Feb 25, 2013 by (4,225 points)
Dear Dilaton, it's the same word, "unparticle", but be sure that user1247's ideas behind this word have nothing to do with the ideas of Howard Georgi. It's a linguistic coincidence. ;-)

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user Luboš Motl
This is definitely an example of what I am asking about, although it is not the sort of general description I am looking for, since it is restricted to the topic of a scale invariant hidden sector. The fact that such possibilities are more general is described for example in section 9.2 of the link I gave (Quantum Mechanics: Myths and Facts).

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user user1247
No Lubos, that really is an example of precisely what I am asking about.

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user user1247
Lubos, I am asking about something more general than Georgi's unparticles, and I am not asking only about dark-matter. I don't think scale-invariance is the only prerequisite for such phenomenology.

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user user1247
Dear user1247, it's not because you're talking about "unstable excitations". There are no excitations in the unparticle scenario, and no unstable excitations to boot. That's why it is called "unparticles" because these quantum fields don't have excitations. Instead, their effect on everything else is described by local operators of the CFT kind and phenomenological power laws. In some sense, the reason why the excitations are gone in "unparticles" is that the would-be excitations are too stable - confined - not unstable.

This post imported from StackExchange Physics at 2014-03-17 04:25 (UCT), posted by SE-user Luboš Motl
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