Stern-Gerlach With 3 Magnets

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Discussion Overview

The discussion revolves around a modified Stern-Gerlach experiment involving three magnets and the behavior of spin-one particles as they pass through the apparatus. Participants explore the implications of the setup on beam splitting and the conditions under which particles are deflected.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Richard Feynman's description of the modified Stern-Gerlach experiment suggests that a beam of spin-one particles will split into three beams when passing through the first magnet.
  • Some participants question why the third magnet, being identical to the first, does not cause the beam to split again into three beams.
  • One analogy compares the momentum transfer in the Stern-Gerlach experiment to a baseball being hit back and forth, suggesting that the sequence of magnets imparts zero net transverse momentum to the particles.
  • Another participant notes that the original Stern-Gerlach setup typically splits beams into two based on spin states, leading to confusion about the claim of three beams.
  • There is a suggestion that the splitting into three beams may be related to the nature of spin-one particles, which can have three distinct states: one up, one down, and one that continues straight.
  • Participants discuss the requirement for a magnetic moment for deflection in the Stern-Gerlach device, noting that neutral particles like silver atoms can still be used due to their magnetic properties.

Areas of Agreement / Disagreement

Participants express uncertainty regarding the behavior of the third magnet and the implications of spin-one particles. There is no consensus on the mechanics of the beam splitting or the conditions required for deflection.

Contextual Notes

Some participants highlight the distinction between spin-one and spin-half particles, indicating that this may influence the outcomes of the experiment. There are also mentions of the need for a magnetic moment rather than charge for deflection, which remains an area of exploration.

LarryS
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Richard Feynman describes a “modified Stern-Gerlach” experiment in which the apparatus consists of 3 magnets in a row, along the path of the beam. The first magnet is polarity “South on top, North on bottom”. The second magnet is twice as long as the first and of opposite polarity. The third magnet is identical to the first. He then states that a beam consisting of, say, spin-one particles will be split into 3 beams when it passes the first magnet. The second magnet, being of opposite polarity will force the 3 beams back together again. And, the third magnet will continue to bring the 3 beams back together so that just one beam exists the apparatus.

Finally my question: If the third magnet is identical to the first magnet then why does it not also split the beam into 3 beams again?

Thanks in advance.
 
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It's similar to this situation: I hit a baseball with my bat; now it's moving at some speed toward my partner. My partner hits it back to me twice as hard (transferring twice as much momentum), which exactly reverses its momentum. As it's coming back to me, I hit it again just as hard as I hit it originally, which brings the ball to a dead stop.

The only difference is that in the Stern-Gerlach experiment, the magnets impart different momenta to the particles depending on the particles' spin states. But whatever the spin state, this sequence of magnets will impart 0 net transverse momentum to a particle.
 
This webpage http://www.upscale.utoronto.ca/PVB/Harrison/SternGerlach/SternGerlach.html has some diagrams of a Stern-Gerlach set up with 3 magnets in a row. (Go about a third of the way down the page to the section titled "Building a Spin Filter"). In that set up the beam is split into two because electrons are either spin up or spin down. I am not sure why you are talking about splitting into 3 beams, but I am not much of an expert on this so I might be missing something.

eGun3Magnets.jpg
 
referframe said:
Finally my question: If the third magnet is identical to the first magnet then why does it not also split the beam into 3 beams again?
The first beam splits because it contains particles with different spin states. The paths of the three polarized beams will bend but not split, because particles in the same beam all have the same spin state. Also, I don't know the details, but I assume that the second magnet will have the beams going towards each other (as in the picture that yuiop posted) so none of them is parallel to the path of the original beam.

yuiop said:
I am not sure why you are talking about splitting into 3 beams,
It must have something to do with the fact that the spin is 1 instead of the usual 1/2. (This is news to me too).
 
Fredrik said:
It must have something to do with the fact that the spin is 1 instead of the usual 1/2. (This is news to me too).
That seems to be the case. A quick internet search indicates that spin 1 particles would split into 3 beams, one up, one down and one that continues in a straight line. Some examples of spin 1 particles are carbon 12 nuclei and Helium 4 atoms. (That's just general info. You probably already know that :wink:). Nice to know we have a quick easy way to determine if something is has spin 1 or spin 1/2. Presumably a particle has to have a charge to be deflected in a Stern-Gerlach device and that is why photons are not deflected in such a device.
 
Last edited:
yuiop said:
Presumably a particle has to have a charge to be deflected in a Stern-Gerlach device and that is why photons are not deflected in such a device.
What they need is a magnetic moment. The original SG experiment used silver atoms, which are of course neutral.
 
Fredrik said:
What they need is a magnetic moment. The original SG experiment used silver atoms, which are of course neutral.
Thanks :)
 
The_Duck said:
It's similar to this situation: I hit a baseball with my bat; now it's moving at some speed toward my partner. My partner hits it back to me twice as hard (transferring twice as much momentum), which exactly reverses its momentum. As it's coming back to me, I hit it again just as hard as I hit it originally, which brings the ball to a dead stop.

The only difference is that in the Stern-Gerlach experiment, the magnets impart different momenta to the particles depending on the particles' spin states. But whatever the spin state, this sequence of magnets will impart 0 net transverse momentum to a particle.

Great analogy. Thanks to all.
 

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