Light's orbital angular momentum

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Light possesses both orbital and spin angular momentum, even in a vacuum, though the concept of orbital angular momentum can be confusing as it implies an orbit around something. The discussion highlights that light can exhibit angular momentum without a physical orbit, similar to how massive objects can have angular momentum without rotating. The existence of Laguerre-Gaussian modes, which are associated with orbital angular momentum, is acknowledged, but their presence in free space versus laser resonators is questioned. The distinction between total angular momentum and its orbital and spin components is emphasized, as the latter split lacks a gauge-invariant definition in the context of electromagnetic fields. Ultimately, while light has angular momentum, the classification into orbital and spin components is debated, with total angular momentum being the only physically meaningful quantity.
Khashishi
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I read this article, and I'm confused about several things.
http://scitation.aip.org/content/aip/magazine/physicstoday/article/57/5/10.1063/1.1768672

Apparently, light can have orbital angular momentum as well as spin. But I don't see how this is possible, at least in vacuum. Is this in vacuum or a waveguide? (It wasn't too clear in the article or first reference) To have orbital momentum, one has to orbit around something. What is light orbiting around? The article says the center of the beam, but there's nothing there, right?

I see there are various modes for Gaussian beams called Laguerre-Gaussian modes. Do these exist in free space or only in some kind of laser resonator?
 
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It can have "orbital" angular momentum in vacuum. You don't need an orbit, in a similar way a massive object can have angular momentum without rotating or orbiting, if its flight direction does not point towards/away from the origin of the coordinate system.
 
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I thought of that, but that would mean that the light beam must be diverging/converging quite rapidly. Is this the case for this kind of beam?
 
I don't have access to the article here. Orbital angular momentum is a common thing in nuclear transitions, for example.
 
I've to read the article first, to say anything about it, but for sure it's highly misleading to talk about orbital and spin angular momentum for a relativistic (classical or quantum) field and particularly for the electromagnetic field, which is a massless vector field, because there is no gauge invariant way to define this split of the total angular momentum (which is of course well defined) for the electromagnetic field.

The correct mathematical treatment is well known as "multipole expansion" in classical electrodynamics. For QED the corresponding mode decomposition of the electromagnetic field operator is the use of simultaneous single-photon eigenstates for energy, and total angular momentum (quantum numbers ##\ell## and ##m## as in the multipole expansion). For a very thorough treatment of this, see

Landau/Lifshitz Vol. 4 (Quantum Electrodynamics).
 
Just a layman here, but let me take a stab.

A collapsing star gravitates and has angular momentum. If it becomes a black hole, it still gravitates and has the same angular momentum. But we do not know (and can not know) if the stuff inside the BH has rest mass or if it has all been converted to radiation. But we need not know, because it has the same gravity and angular momentum either way.

By that reasoning, I say light must have angular momentum. Whether that qualifies as "orbital angular momentum" is a different question.
 
Of course, light (i.e., the electromagnetic field) has angular momentum. That's well known since the 19th century. It's only impossible to make sense of a split into orbital and spin parts of angular momentum. Only total angular momentum has a physical meaning.

A black hole is defined uniquely by its conserved bulk properties (invariant mass, angular momentum, electric charge). There are (within classical Einstein-Maxwell theory) no other structures characterizing a black hole. This is known as Wheeler's "no-hair theorem".
 

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