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click on it three times. This makes three identical studies go into the Price pane. These are all marked EMA(30), indicating in shorthand that three 30-period Exponential Moving Averages have been added. 4. Double-click on the rst EMA(30) and change the value in the period box to 10, then click OK. That will make it a 10-day moving average. 5. Double-click on the second EMA(30) and change its period value to 50, then click OK. Change the third EMA to 100 in the same manner. The Price pane will resemble Figure 6.16. 6. Click the OK button to nish.

up walls and out of a containing vessel. The reason is that it coats the wall with a thick film. At a height z above the free liquid surface (in equilibrium with its own vapor), the film adhering to a vertical wall has a thickness proportional to z~ 1/2. Derive this result b\ the following steps: (a) Suppose the temperature is such that the superfluid fraction is f. Consider an element of the adhering film at height z, of thickness d, vertical dimension ~z, and unit width in

the other direction (see sketch). Regard the superfluid component in this volume element as a free Bose gas. Write down its energy, with contributions from potential energy due to gravity and kinetic energy due to its being confined to a thickness d. ( b) Minimize the energy with respect to d.

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13.2 A pure superfluid contained in an infinite cylinder of radius a develops a vortex line along the axis of the cylinder, of core size b.

(a) Find the superfluid velocity V as a function of normal distance r from the axis of the s cylinder. (b) Find the energy per unit length of the cylinder. (c) Find the angular momentum per unit length of the cylinder.

be the differences in chemical potential and superfluid phases between A and B. In equilibrium !1/L = !1<j> = O. Now suppose vortex liens are created on one wall of the channel, migrate across the channel as indicated by the arrow in the accompanying top-view sketch, and are annihilated on the opposite wall. With the help of Anderson's equation

4 5 6

show that this mechanism maintains a finite chemical potential difference !1/L. Find the relation between !1/L and N, the rate of vortex creation.

V-- Vortex line if (top view)

13.4 The first-order perturbation for the ground state energy due to hard-sphere intera(

FIGURE 6.16 Three exponential moving averages being applied to the Price pane in the technical studies editor.

tions is calculated for a Bose system in (A.36) of the Appendix using configuration-spa c" methods. Repeat the calculation using the method of quantized fields. (You will find :: much neater.)

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