# Diagonal squeezing of an electron beam by a pair of bar magnets

While coordinating an introductory physics lab on the Lorentz force, I came across a behavior which I hadn't seen before and for which I didn't have a ready explanation. The experiment consisted of putting a CRT tube in a uniform magnetic field causing the electron beam to curve and therefore move visibly on the screen. For this purpose, they placed the CRT in a Helmholtz coil.

To get some qualitative sense of what's going on, they also had some bar magnets on hand. They were only supposed to use one such magnet for this purpose, and in that case the dot on the CRT screen moves as expected: If the north pole is placed on the left side of the CRT (relative to the front screen) the electron beam moves down; if it's placed on the right side, it moves up. If both are done at the same time, these two effects could be expected to approximately cancel out. And, indeed, the center of the dot remains near the center of the screen in that case.

However, in practice I furthermore observe that the circular dot on the screen becomes squeezed into an ellipse: the closer the magnets are placed to the electron gun, the stronger this effect. In addition, the squeezing appears to be at a 45 angle to the line of the magnets i.e. half the electrons are deflected up-and-to-the-right of the center, and half are deflected the other direction. (If the magnets are flipped so that their south poles are close to each side of the CRT, then the pattern flips from left-to-right.)

My basic guess is that magnetic fields of the two magnets are serving as a 'lens' for the electron beam; indeed, I think the CRT itself contains a quadrupole magnetic lens near its filament for this purpose. However, in that case I'd have naively expected the squeezing to occur along either parallel or perpendicular to the axis of the magnets. Is there an easy explanation for why the squeezing is along the diagonal instead?