PHY 140A SOLID STATE PHYSICS SOLUTION TO HOMEWORK

Such an arrangement of spheres is called a close-packing arrangement. It is a Bravais lattice, since from whichever point the lattice is viewed, it appears exactly the same. Let us consider the distribution of T , the time interval between two successive collisions, as following. Nonetheless, these planes are more close packed than the others, and thus have fewer dangling bonds vulnerable to chemical attack. Say you have a micron thick wafer oriented in the direction, coated with silicon oxide not etched by KOH.

The side view of Si wafer, which is covered by SiO on both sides, is illustrated in Fig. Starting values can be found at Webelements. Even though the results are the same in those two ways of average in most of physical system, you should appreciate the physical meaning between them carefully. Since the fct unit cell constructed from bct lattice will always be larger than the bct unit cell, see Fig. This is a Bravais lattice, and is the unit cell for indium.

phy 140a solid state physics solution to homework

This actually follows from the similarity among triangles. Averaging over all possible direction, we get the average energy lost to the ions in the second of two collisions separated by a time t: A monatomic, cubic material has lattice spacing of a.

PHY A: Solid State Physics Solution to Homework 7 | FlipHTML5

By Paulo Roberto Silva. Calculate the dimensions of the initial front side rectangular hole in the oxide required to produce a 5 micron by micron suspended oxide film on the backside after a KOH etch. Free Electron Theory of Metals. Such an arrangement of spheres is called a close-packing arrangement. Consider a metal at uniform temperature in a static uniform electric field E. You can add this document to your saved list Sign in Available only to authorized users.

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Remember me on this computer. Let the lattice constant for the corresponding simple cubic be a. This argument holds for every infinitesimal time interval, so the total probability that the electron does not have any collision in the total time t will be the product of those probabilities in each infinitesimal interval: In fact, if you take a plane containing the side diagonals on the top surface and bottom surface, you will find why those 5 big spheres in Fig.

phy 140a solid state physics solution to homework

From simple geometry, the answer is: Even though the results soild the same in those two ways of average in most of physical system, you should appreciate the physical meaning between them carefully. Therefore, the packing fraction is: As a consequence of part dthe mean time between two successive collision is simply computed as: Upload document Create flashcards.

Lecture Notes on Solid State Physics. Problem 4 Kittel 6.

PHY 140A: Solid State Physics Solution to Homework #1

Explain why this is not inconsistent with the result in d. B, 47, Method We physicw the lattice Boltzmann LB model for thermal.

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phy 140a solid state physics solution to homework

The sketch of the structure solutiom etching the wafer. Average over all electrons, we get the mean time back to the last collision: The average is over all directions in which the electron emerged from the first collision.

For sc lattice, consider the side, as in Fig. Label the a and b lattice parameters for the fct and bct unit cells. For diamond lattice, it requires thinking carefully. Structure and X-ray Diffraction will count as 2. Substitute in the equation, we have: If it is, give 3 primitive vectors; if it is not describe it as Bravais lattice with as small as possible a basis. The ni are all even? Show that it will have no collision during the next t seconds with the same probability.

Suggest us how to improve StudyLib For complaints, use another form. It is a Bravais lattice, since from whichever point the lattice is viewed, it appears exactly the same.

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