# Reaction force in electron spin measurements

Consider the following (thought) experiment, where an electron is emitted, then deflected by a magnetic field, and then detected: Because the momentum of the electron changes when it gets deflected, it seems intuitively clear that there should be a reaction force on the magnet, which could in principle be detected.

But now consider the following modified setup: Here electrons are emitted, with their spin aligned in some arbitrary direction. The first Stern-Gerlach magnet, A, can deflect electrons either up or down. B and C deflect the paths of the two beams, and the final magnet, D, combines them back into a single beam, effectively reversing the action of A. This system of magnets is followed by a detector, which can measure the spin of the electron in the $z$ direction, perpendicular to the plane of the rest of the diagram.

According to my understanding of quantum mechanics, the measurements from this detector should be the same as if the magnets were not there. That is, if the electrons are emitted with their spins always pointing in the $z$ direction, the detector should also find that their spins are always 'up' in the $z$ direction.

The problem is that if we can measure the reaction force on any of the four deflecting magnets then we can work out which of the two paths the electron took, and thus we would have measured its spin in two directions simultaneously. Clearly this isn't possible, so where have I gone wrong? Is there a reaction force on the magnets? If there isn't, what happened to the conservation of momentum? Is it just that the reaction force does exist but we can't measure it? (And if so, what prevents us from doing so?) Or have I just made a mistake in reasoning about how this setup would behave?

• no images appear. ?? – anna v Feb 25 '13 at 12:28
• Really? That's annoying, I can see them fine on my machine. – Nathaniel Feb 25 '13 at 12:30
• The image URLs are i.stack.imgur.com/SKqat.png and i.stack.imgur.com/motIz.png if that helps. – Nathaniel Feb 25 '13 at 12:32
• I see the images here. – Luboš Motl Feb 25 '13 at 12:35
• the url's you give do not work either. firefox, chrome, or internet explorer in windows. – anna v Feb 25 '13 at 12:42

Yes, you may arrange the magnets in such a way that the splitting of the original beam is "undone". The two parts of the wave functions "reinterfere".

The reason why you can't measure both $j_y$ and $j_z$ is pretty much the same reason as the reason why you can't see the interference pattern as well as the "which slit" information in a double slit experiment and your setup may actually be closer to the thought experiments that were intensely discussed during the Bohr-Einstein debates etc. Conceptually, however, the two situations are isomorphic.

The uncertainty principle and/or the destructive effect of your apparatus will always prevent you from learning $j_y,j_z$ at the same moment.

If you want to measure the impulse $\Delta p$ transferred from the electron to the magnets and see it's there, it implies that you must know the magnets' initial momentum with precision $\Delta p$ or better (or something of the same order). The uncertainty principle then guarantees that the vertical position of the magnets is undetermined, with $\Delta x\geq \hbar / \Delta p$.

The electrons also get a kick $\Delta p$ from the magnets – by the momentum conservation, it's the same $\Delta p$ as above, the kick to the magnets – and because you want to be able to distinguish the two beams, you must have $\Delta x\leq \hbar/\Delta p$ for the electrons. That directly contradicts the previous condition. So you either make the split beams focused enough to the two magnets in the middle i.e. small enough $\Delta x$ or you will have a small enough $\Delta p$ which is needed to measure the change of the momentum of the magnets but you can't have both, by the uncertainty principle.

You could also invent a more invasive way to measure which path the electron took. But to claim that your apparatus preserved the original state, especially the relative phase of "up" and "down" that is needed to predict the probabilities of various values of spin $j_z$ (which you untypically take orthogonal to the screen), you need the position of the magnets to be non-intrusive enough. Again, in analogy with the double slit experiment, you will find out that if you can find out about the path or momentum of the electrons, you will modify the electrons' wave functions so that the relative phase will be modified and the results for $j_z$ will be different than if the apparatus weren't there in the middle. You will change the rules of the game.

• That makes perfect sense. I just wasn't thinking about it in terms of $\Delta x$ and $\Delta p$ for some reason. Thanks for the clear explanation. – Nathaniel Feb 25 '13 at 13:14

Unable to see your setup, I am nevertheless intrigued by the question of whether there is a back reaction on the magnets and how could one measure it.

If I have a magnetic field that is creating a potential well for the electron, I would see the electron occupying a quantized state in this potential well, the initial capture momentum balance being taken up by an electromagnetic radiation/photon.

Classically that is what is happening continuously to the electron anyway. brehmstrahlung which is what is seen in this image, electrons loosing energy in the field and getting a diminishing radius.

So momentum is balanced by the electromagnetic radiation leaving tangentially to the curve, not by changing the magnetic field itself with a reaction force (vector), except in terms of energy balance (scalar).

• That's interesting - so I guess in principle you can do it in such a way that the magnet doesn't feel any back reaction, as long as you set it up so that the EM radiation escapes, rather than being absorbed by the magnet. – Nathaniel Feb 25 '13 at 13:19
• it will be very low frequency radiation . It will not be detectable in practice even if it is all absorbed somehow by the magnet. Magnets are very heavy systems. – anna v Feb 25 '13 at 13:29