A collection of problems in atomic and nuclear physics - download pdf or read online

By I. E Irodov

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Take into account that A 3> kT. 17. 10 3 times. 18. Having determined the concentrations of free electrons and holes, demonstrate that at sufficiently low temperatures the Fermi level in an impurity-free semiconductor is in the middle of the forbidden band. 19. E their activation energy. • (a) Derive this expression using the Fermi distribution. (b) Find the location of the Fermi level. 20. ,) = 1: (v); (v) is the mean velocity of electrons. 10- 6 Q. cm. ,) with the interatomic distance in copper.

71 A. 21. 0 em from the fIlm. 1 mm. Calculate the lattice constant. The lattice is known to be a space-centered cubic one. 22. 4. Taking into account that the diameters of these rings are considerably smaller than the distance between the film and the screen, determine the type of the lattice (face- or space-centered). 0 n BINDING ENERGY. 3 mm. The incident beam direction is perpendicular to the rotation axis (the camera's axis). The X-ray pattern comprises the system of maxima distributed over the layer lines (Fig.

3 mm. The incident beam direction is perpendicular to the rotation axis (the camera's axis). The X-ray pattern comprises the system of maxima distributed over the layer lines (Fig. 26). 5 mm respectively, the rotation being performed a bout directions [110] and [111]. 17. What orders of monochromatic X-ray reflection will disappear on transition from the simple cubic lattice to space- and facecentered ones? The lattice constants are assumed to be equal in all three cases. Consider the reflections from the planes (100), (110), and (111).

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A collection of problems in atomic and nuclear physics by I. E Irodov


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