Solid state exam Flashcards

1
Q

Bravais lattice

A

a set of points generated by multiples of “primitive vectors”

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2
Q

Primitive unit cell

A

The volume of space which, when translated through all the vectors of a BL, fills space without overlapping or leaving voids

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3
Q

Wigner-Seitz cell

A

the region of space which is closer to one given lattice point than any other (a special primitive unit cell)

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4
Q

Basis

A

the atom(s) that we place on each lattice point

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5
Q

Packing fraction

A

the volume percentage of a unit cell occupied by atoms as hard spheres - higher is better!

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6
Q

Kinematic approximation

A

that x-rays are only scattered once in a solid

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7
Q

Bragg condition

A

the condition for constructive interference when x-rays specularly reflect by successive lattive planes nl = 2dsin(x)

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8
Q

Lattice plane

A

a plane containing at least three non-colinear points of a given Bravais lattice, characterised by “Miller indices”

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9
Q

Reciprocal lattice

A

A set of vectors G for which G.R = 2PiL (L = integer)

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10
Q

G vectors

A

Plane waves that are periodic with the reciprocal lattice (frequencies)

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11
Q

Laue condition

A

When K = G. Physical meaning is constructive interference

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12
Q

Phase problem

A

Rho-G (the structure factor) is complex, so intensity measurements tell us the modulus, not the phase

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13
Q

Ewald construction

A

a geometrical construction which helps to visualise the Laue condition

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14
Q

Structure factor

A

takes the atomic basis into account mathematically

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15
Q

Atomic form factor

A

fj, describes the scattering power of the atom

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16
Q

Brillouin condition

A

2k.G = G^2 (comes from Laue condition)

17
Q

Independent electrons

A

no interaction with each other

18
Q

Free electrons

A

no interaction with ion cores

19
Q

Born-Oppenheimer approximation

A

ignore motion of ions

20
Q

Born-von-Karman boundary conditions

A

like a box wrapping round on itself (periodic)

21
Q

Density of states

A

How many allowed states there are within dE at E

22
Q

Fermi energy

A

maximum energy level (at 0K) occupied when all electrons are assigned levels

23
Q

Fermi wavevector

A

maximum wavevector at Ef

24
Q

How can we get the Fermi energy from the density of states?

A

By integrating the density of states from 0 up to the Fermi energy

25
Q

Fermi surface

A

Surface of constant energy in reciprocal space which separates occupied states from unoccupied ones

26
Q

Soft zone

A

smearing of electron distribution at finite temperature (approx 4kBT)

27
Q

Thomas-Fermi screening length

A

the distance at which the potential is no longer infinitely ranged

28
Q

Mott transtition

A

the amount of doping which causes as insulator to become a conductor

29
Q

Bloch’s theorem

A

For a particular k, there is a “Bloch wave” which is a plane wave x a function with the periodicity of the lattice

30
Q

Central equation

A

the SE in a periodic lattice written as algebraic, (rather than differential) equations

31
Q

Band structure

A

E eigenvalues of Bloch states, E(k)

32
Q

Band gaps

A

gaps in band structure when U = 0