Thought experiment / paradox question

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SUMMARY

The discussion centers on the paradox of measuring spin states in a neutral electron beam using Stein-Gerlach devices. The initial setup involves a spin filter accumulating spin-up electrons, leading to a net spin accumulation. However, when introducing a terminal that splits the beam into left and right spin electrons, the expected conservation of spin appears violated. The resolution lies in understanding the angular momentum transfer between the electrons and the magnetic field, where the net flow of Lz momentum from the electron beam to the magnetic field accounts for the observed phenomena.

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NateTG
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Let's say I start out with a (spin) neutral electron beam. Now, I can place an up/down Stein-Gerlach spin filter/detector in the beam so that I have a running tally of the "up" electrons, and a spin-down exit beam.
Since the measuring device is accumulating spin-up electrons, it should also be accumulating net spin-up.
Now, let's say I have a terminal for the beam, which splits the beam into left and right spin electrons using a Stein-Gerlach device, and takes counts of both. Now, the terminal is interacting with (what I expect to be) a roughly equal number of spin-up and spin-down electrons, so there should be no net accumulation of spin in the terminal.
This seems problematic because the filter is accumulating net spin without conservation of spin. What am I missing?
 
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NateTG said:
What am I missing?
The angular momentum in the magnetic field of the second apparatus.
For each individual |z+> -> |x+> transition, there is a transfer of Lz from the electron to the magnetic field ; and for each |z+> -> |x-> transition, there is an EQUAL transfer of Lz from the electron to the magnetic field.
Of course, for the |z+> -> |x+> transition, there was a positive contribution of Lx from the field to the electron, and for the |z+> -> |x-> transition, there was a negative contribution of Lx, so the Lx contribution averages out to 0, but not the Lz contribution.
There's a net flow of Lz momentum from the electron beam to the B-field (and hence to the magnet).
cheers,
Patrick.
 
Sure, that makes sense, but doesn't that lead to a problem because you could know the spin state in two dimensions for a bunch of electrons?
Let's say we have an EPR-like set up with an entangled electron source, and an up-down split count target on one side, and a left-right split target on the other. And, using timing we manage to restrict our runs to getting 5 electrons at a time. Then there's a 1 in 1024 chane that all the hits on the up/down detector will be up, and all the hits on the left-right detector will be right. Thus we would 'know' that all of the electrons that hit the up/down detector would have to have been up/left electrons, but those measurements don't commute, and thus be able to measure (and predict) the net spin of the targets?
 
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