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One study, which is somewhat like Bollinger Bands in its application, is the Linear Regression Channel. There is actually a variety of Linear Regression studies, but they all are based on the same principle: a trendline is laid down which corresponds to an equilibrium in price. That is, a line is drawn that is the best t based on past price activity. Two other lines are then laid down one above and one below that are the same distance from the equilibrium line and whose distance is based on past price volatility. What this results in is a channel with an upper half and a lower half. Some Linear Regression studies have straight lines, and others are curved. Figure 5.15 shows one style of Linear Regression Channel with curved lines. The prices are generally bound by the lines, bouncing between the upper and lower boundaries and hugging the center line. As the area with the rounded rectangle illustrates, the prices sometimes do go outside their boundaries. These extremes are usually corrected, however, which means that these outlier prices can be viewed as special buying or selling opportunities. While the prior gure showed price action that had dipped beneath the lower boundary, Figure 5.16 shows a stock whose upward movement

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(11.88)

0,1,2, ... )

The magnetization per unit volume and the magnetic susceptibility per unit volume are respectively given by

(x> 1)

/lon [2(j + 1)(j + 2)x - (2j + 3)] (

(x>l)

(11.89) 0,1,2, ... )

9 11

FIGURE 5.15 A linear regression study will typically keep a boundary on prices, but sometimes price movement is so extreme it goes outside the lines.

(j ~ 2 < x < j ~ 1 ' j = 0,1,2, ... )

(11.90)

The Hall effect was discovered in the nineteenth century: When crossed magnetic and electric fields are applied to a metal, a voltage is induced in a direction orthogonal to the crossed fields, as evidenced by an induced current flowing in

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that direction-the Hall current. This effect is easy to understand on the basis of the free electron theory of a metal, as follows. Crossed magnetic and electric fields, denoted, respectively, by Hand E, act as velocity filters to free charges, letting through only whose those velocity v is such that E + (vje)B = 0, or

(11.91)

(11.92)

where q is the charge, and n the density. The Hall resistivity Pxy is defined as the ratio of the electric field (in the y direction) to the Hall current density (in the x direction): E j=(11.93)

(11.94)

was so swift and strong that it moved above its upper boundary. Events like this can sometimes be exploited for quick trading pro ts, since the stock has moved to an extreme level based on its past price behavior.

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Measurements of the Hall resistivity in various metals has yielded charge carrier densities and provided the first demonstrations that there are not only negative charge carriers (electrons), but also positive ones (holes). The two-dimensional electron system used as a model in the last section can now be created in the laboratory, thanks to developments in the transistor technology. It can be made by injecting electrons into the interface of an alloy sandwich, which confines the electrons in a thin film about 500 A thick. The Hall experiment has been performed on such two-dimensional electron systems at very low temperatures, and the direct resistivities Pxx and the Hall resistivities Pxy have been measured, as indicated in Fig. 11.11. The experimental results are quite dramatic, as shown in Fig. 11.12. As the magnetic field H increases the degeneracy of the Landau levels increases. Since the electron density does not depend on the field the filling fraction p of the lowest Landau level decreases: hen

Repeat Steps 5 and 6 to add more fields. Click Next. Click the field you want to use to group the data. Click the Add button (

(11.95)

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