By James Hamilton
The Aharonov-Bohm impression is linked to cyclic movement. it's considered one of a few anholonomic results, and which means the dynamical description relies on the present place of the procedure and at the direction through which it reached that place. An instance of an anholonomic influence is Foucault's well-known pendulum, which easily demonstrates the Earth's rotation. The Sagnac influence - a gentle beam passing round a circled method of mirrors - is one other instance. smooth dynamical advancements akin to Hannay's perspective and Berry's part are extra priceless examples.
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Additional info for Aharonov-Bohm and other Cyclic Phenomena
1 and that in the uniform field B are equal. 3) will differ somewhat, and higher levels of radial oscillation (n _> 1) need not agree in the two cases. Since it is the motion along the 0-direction that is of importance here, any other difference in X between CA and r will be ignored in our discussion. 17) is half of the phase change in r on passing round the arc 0 of the circle p = P0. The basic origin of this factor 89will be seen below in discussing the classical physics picture. In practice the phase of UAi21r) may be large, since M is of the order of 27rp0/A.
The cylinder in Fig. 3 has diameter 2rf < al. The position of the flux shown in Fig. 4 is in the "shadow" of the cylinder. 2a) should be remembered. Thus b0 -~ 4cm, a0 -~ 10~m, ~ _~ 10-11m, and 2rf is (say) 5gin. Hence the shadow of the cylinder (from the sources) is well defined. If the field B~ in Fig. e. 3a) Some authors suggest that the effect of the "hidden flux" in Fig. 3 is rather strange. The "hidden flux" is shown in Fig. 4, and it cannot move the profile since the rays do not pass through the induction.
4a). 1), deflects the moving electron, and thereby alters A. This phenomenon is easily seen from the simple scattering shown in Fig. 2. An electron coming from far away is deflected by an axially symmetric field Bz(p). The induction falls off to zero smoothly outside the batched 42 4. ClassicalPhysics and the Adiabatic Principle region around O. We choose Bz(p) >_0, so the Lorentz force always deflects the electron to the left. The angular momentum at the points -co, U, W, V, +co , is respectively mvb, O, - m v p m , O, m v b , where v is the velocity and b, Pm are the pedal distances shown in Fig.