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Suppose that the channel鈥檚 outgoing end is in the hydrogen l=0Stem-Gerlach apparatus of the figure. You place a second such apparatus whose channel is aligned with the first but rotated 90about the x-axis, so that its B 鈥揻ield lines point roughly in the y-direction instead of the. What would you see emerging at the end of your added apparatus? Consider the behavior of the spin-up and spin-down beams separately. Assume that when these beams are separated in the first apparatus, we can choose to block one or the other for study, but also assume that neither deviates too far from the center of the channel.

Short Answer

Expert verified

The one that emerges at the end of the added apparatus will be a beam with either a left-pointing or right-pointing spin.

Step by step solution

01

Stern-Gerlach experiments.

The Stern-Gerlach experiment provides the demonstration for the quantization of the spatial orientation of the angular momentum, in this experiment a silver atom is used which is made to go through a spatially varying magnetic field.

02

The one that emerges at the end of added apparatus.

In the experiment, each atom is not in a specific dipole up or down until it passes through the magnet that will measure its state with equal probability. Once the state is filtered, either it is dipole upstate or dipole downstate, not in a single left state.

So, when the beam is passed through the second apparatus. It is divided into two beams, depending on whether the second measuring process results in measuring a left-pointing or right-pointing spin.

Conclusion: Therefore, The one that emerges at the end of the added apparatus will be a beam with either a left-pointing or right-pointing spin.

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Most popular questions from this chapter

Question: In classical electromagnetism, the simplest magnetic dipole is a circular current loop, which behaves in a magnetic field just as an electric dipole does in an electric field. Both experience torques and thus have orientation energies -p.Eand-B.(a) The designation "orientation energy" can be misleading. Of the four cases shown in Figure 8.4 in which would work have to be done to move the dipole horizontally without reorienting it? Briefly explain. (b) In the magnetic case, using B and u for the magnitudes of the field and the dipole moment, respectively, how much work would be required to move the dipole a distance dx to the left? (c) Having shown that a rate of change of the "orientation energy'' can give a force, now consider equation (8-4). Assuming that B and are general, write-B.in component form. Then, noting thatis not a function of position, take the negative gradient. (d) Now referring to the specific magnetic field pictured in Figure 8.3 which term of your part (c) result can be discarded immediately? (e) Assuming thatandvary periodically at a high rate due to precession about the z-axis what else may be discarded as averaging to 0? (f) Finally, argue that what you have left reduces to equation (8-5).

The wave functions for the ground and first excited states of a simple harmonic oscillator are Aebx2/2andBxebx2/2. Suppose you have two particles occupying these two states.

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Using f2=L2+S2+2L-Sto eliminate L - S. as wellas L=l(l+1)h,S=s(s+1)andj(j+1)h, obtain equation (8- 32 )from the equation that precedes it.

The general form for symmetric and antisymmetric wave functions isn(x2)n(x2)n(x1)n(x2) but it is not normalized.

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(c) Discuss the relationship between your answers in (a) and (b)?

The 21cm Line: One of the most important windows to the mysteries of the cosmos is the 21cm line. With it astronomers map hydrogen throughout the universe. An important trait is that it involves a highly forbidden transition that is, accordingly, quite long-lived. But it is also an excellent example of the coupling of angular momentum. Hydrogen's ground state has no spin-orbit interaction鈥攆orl=0there is no orbit. However, the proton and electron magnetic moments do interact. Consider the following simple model.

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