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Since only "1/ = is accessible to experiments, in our model a and b are both functions only of t, and we are going along some line in the ab plane that passes through the origin We show a comparison between experiments and our mean-field model in the neighborhood of the tricritical point in Fig 176 The resemblance is only qualitative However, the mean-field prediction y = 1 agrees with experiments This is not accidental, as we shall see later..

x= ( H-a o t)-l (t<O) (17.74) yields m = (H/e)1/5,

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By default, when you type text in a Word 2010 document, the program uses 11-point Calibri font. You can change the text font, size and colour to alter the appearance of text in a document. For example, you might change the font, size, and colour of your document s title text to emphasise it. You can also change the font that Word 2010 applies by default.

(17.76)

(11.147)

Paramagnetic susceptibility oi an imperfect Fermi gas with repulsive interactions. The model used is well founded only for kT/f F 1.

1 (11.1481

f ==

p,( N)

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which number on an astronomical scale, the index performs in a stunningly orderly and systematic fashion. Looking at another, broader index the S&P 500 we can see similar fascinating phenomena (Figure 13.20). The arrows show how the highest and lowest fan lines constrict the price movement. Keep in mind the graph is showing a period of more than 70 years. The price reverses on various fan lines in many instances, and the two rectangles that are drawn here highlight two multi-decade years where the prices were bound between two fan lines. Looking at a speci c portion of this index (from the year 1954 to 1985) we can see a neat, tidy progression of tilted rectangles (Figure 13.21). The rectangles move slightly down each time since this period of market history included several vicious bear markets, including the infamous 1973 1974 bear market. Even when prices made extreme moves, pushing

(11.149 )

a ( TX)

(11.150 )

Click the Home tab on the Ribbon. Click the Font Size Click a size. Word applies the font size to the text, in this case, 48 points.

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It reaches a maximum value, which is greater than unity, at kT/ f. F Z 1. Then it approaches unity as T --+ 00. A qualitative plot of TX/C is shown in Fig. 11.19. If we calculate X for an ideal Fermi gas endowed with the same magnetic moment, we find the slope

a (TX) 3 (ideal Fermi gas) (11.151) aT C T~O 2 The imperfect gas has a steeper slope, as (11.150) shows, which is again a reflection of the enhancement of spin alignment by the repulsive interaction. The result is sometimes described by saying that imperfect gas behaves like an ideal gas with a higher Fermi energy. *

Give numerical estimates for the Fermi energy of (a) electrons in a typical metal; ( b) nucleons in a heavy nucleus; (c) He 3 atoms in liquid He 3 (atomic volume = 46.2 P2 /atom). Treat all the mentioned particles as free particles.

11.2 Show that for the ideal Fermi gas the Helmholtz free energy per particle at low temperatures is given by

11.3 A collection of free nucleons is enclosed in a box of volume V. The energy of a single nucleon of momentum p is

FIGURE 13.20 The arrows here indicate extreme levels of support and resistance during this multi-decade movement of the S&P 500, with the rectangles showing just a couple of the bounded areas.

where me = 1000 MeV. (a) Pretending that there is no conservation law for the number of nucleons, calculate the partition function of a system of nucleons (which obey Fermi statistics) at temperature T. (b) Calculate the average energy density. (e) Calculate the average particle density. (d) Discuss the necessity for a conservation law for the number of nucleons, in the light of the foregoing calculations.

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