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The solution is where Coo is to be determined by normalizing the total wave function. Therefore the unperturbed states that appear in the expansion of 1 '1'0> are states in which pairs of particles k, - k, are excited. We denote such a state by Ill' 12 " , >, in which there are Ik particles with momentum k, and the same number of particles with momentum - k. Thus

00 00

1,=0

how the Price pane has its own indicator (BBEMA, which is the abbreviation for Bollinger Band Exponential Moving Average) while the MACD indicator is in its own pane. You may have reason for the panes to be in a different vertical order than is provided. It is completely up to you how you want these to appear. Typically, the volume for a price chart appears beneath the price. Perhaps you d prefer the volume to be on top. All you need do is click on the Volume pane, hold down the mouse button, and drag the pane to be above the Price pane. As shown in Figure 6.10, your chart will then have these panes in the order you have stated. As you are dragging objects around the technical study editor, a ghost image of what is being dragged appears so you can accurately place it, whether it s a pane or a study. Figure 6.11 shows the Simple Moving Average study being dragged from the Studies list over to the Price pane. It will have its default setting (a 30-period moving average), which can be changed once the drag-and-drop operation is complete. As you can see, there are three panes on this chart a pane for the MACD study, a Price pane with two studies, and a Volume pane (which

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(13.114)

n VI - a~ = exp [-~N(37T - 8) V;;

(13.115)

Click the Header (or Footer) button. Click the type of header or footer that you want to add. This example adds a header.

In (13.114) the term with all Ik = 0 corresponds to the unperturbed ground state 10). Hence Z is none other than (01'1'0)' the probability amplitude of finding the unperturbed ground state in the perturbed ground state. According to (13.115) these two states become orthogonal to each other as N ~ 00. The wave functions for excited states can be easily calculated. For example, for the state with one phonon of momentum k, the normalized wave function is defined by (13.116) l'I'k) = btl '1'0)

l'I'k) =

VI -

a~ atl'l'o)

when you do so, a ghost image of what you are dragging appears so you can place it in the correct pane.

(13.117)

Thus the one-phonon state is a superposition of unperturbed states in which there are any number of particles p, - p for all p, plus an additional particle of momentum k. The average number of particles that have momentum k in the perturbed ground state is

(n k ) = ('I'olata k l'l'o) =

(k"* 0)

(13.118)

Click the field in the header area and type your header text. If the header style includes a date, click the Date field and choose a date from the calendar.

(n k ) =

_k_ 2

8 = 3

is grayed-out, since the volume is being hidden on this chart based on the Quick Toggles). And, as always, once you nish dropping a study to its location, you can double-click on that study to adjust its settings (Figure 6.12). You will certainly do this with moving averages if you use more than one moving average, since they will otherwise all have the same periods.

(13.119)

(13.120)

which shows that the approximation (13.92) is justified. It is instructive to calculate the wave functions in configuration space. In each term of the sum in (13.114), the number n == L Ik is half the total number k>O of particles with nonzero momentum. Thus we must have N ~ 2n. We rewrite (13.114) as follows:

L 'IE'k=n . '2""

[(-a 1 )"(-a 2 )'2 ]1/1 , /2 , )

(13.121)

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