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for a very plain con rmation that the price is well away from the indicator and will not likely be crossing it again. Because lagging indicators by de nition will trail the price movement of a security, you will not get in or out of a position at the optimum time. That is the price you pay for catching broad trends. It is virtually impossible to pinpoint the precise top or bottom of any market. But if you are able to capture 80 percent of the movement from one extreme to another, you will do very well as a trader. Figure 5.6 shows a good example of this with the stock Yahoo! (YHOO). The indicator used is a slow-moving 200-day DMA. The price of this stock bottomed at about $4.50 (which, as with all the examples in this book, is a split-adjusted price) and crossed above its DMA at about $7.50. So the price of the stock had moved up handsomely before a buy signal was generated. The stock got as high at $40 and then started softening up, and eventually the price crossed beneath the DMA at about $34. The move from $4.50 to $40 was about a nine-fold move in the stock, whereas the move from $7.50 (the entry point, based on the DMA) to $34 (the exit point, based on the DMA) was only about a ve-fold move. But

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o = eH/mc,

where (' = ( - h 2k;/2m. The natural frequency of the harmonic oscillator W o is the "cyclotron frequency," that of a classical charge moving in a circular orbit normal to a uniform magnetic field. The energy eigenvalues are thus

(( Pz, j) =

Type a name for the query. Click the Open the query to view information radio button. Click Finish. A query datasheet appears, listing the fields.

~: + hwoU + I),

(j=0,1,2, ... )

(11.68)

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where pz = hk 2 These are the Landau energy levels. Since they are independent of k x' they have a degeneracy equal to the number of allowed values of k x' such that Yo lies within the container of the system. Let us put the system in a large cube of size L, and impose periodic boundary conditions. The allowed values of k x are of the form 2'1Tn x /L, where n x = 0, 1, 2, .... For Yo to lie between and L, the values of n x must be positive and bounded by g = (eH/hc)L 2 (11.69)

FIGURE 5.6 An owner of Yahoo might have held on to YHOO from $7 to $34 using just a moving average, since the stock stayed clearly above it during most of this graph prior to the crossunder.

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which is the degeneracy of a Landau level. The proportionality to L 2 reflects the fact that the projection of the electron orbit onto the xy plane can be centered anywhere in the plane without changing the energy. Thus, when the external field is turned on, the energy spectrum associated with the motion in the xy plane changes from a continuous spectrum to a discrete one, and the level spacing and degeneracy increases with the external field. This is illustrated in Fig. 11.7.

=:>-

...L-_

The Landau levels and the degeneracies derived above are all we need to calculate the partition function. However, we take the opportunity to discuss flux quantization briefly, to help us better understand the wave functions. Consider a plane with a hole in it, which contains a certain amount of magnetic flux <P, as shown in Fig. 11.8. Suppose there is no magnetic field anywhere else. Then the vector potential in the plane must be "pure gauge," i.e., of the form A = '\7w We cannot transform this to zero through any continuous gauge transformation, because necessarily (11.70)

Fig. 11.8 Charged particle moving in plane with a hole containing magnetic flux. The particle will not notice the flux if either (a) it is in a localized state, or (b) the flux is quantized in units of he/e.

iP()/277

12 13 11

(11.71)

where () is the angle around the hole, measured from some arbitrary axis. Now consider an electron moving in the plane, with the boundary condition that its wave function vanish in the hole. In general it is affected by the flux, because the Schrodinger equation involves A, which is nonzero where the electron moves. But since A is pure gauge, we are tempted to try to remove it from the Schrodinger equation through the gauge transformation

the fact is that only in hindsight could one pinpoint these precise low and high values, and using a relatively conservative approach, the majority of the upward movement was still captured.

exp ( -

i::)

= exp [ -

i() (:~ )]

(11.72)

which is generally unacceptable because it will render the wave function discontinuous in space (for () increases by 277 each time we go around the hole). The objection is circumvented under either of the following circumstances:

(a) The electron is "localized," i.e., its wave function is nonvanishing only in the neighborhood of some point. In this case, where (11.72) might

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