The dispersion relation for a one dimensional monatomic crystal with lattice spacing a, which interacts via nearest neighbor harmonic potential is given by: W=A Asin (), where A is a constant of appropriate unit. The group velocity at the boundary of the first Brillouin zone is: A. 0 B. 1 C. D. Aa² 2 Aa² 2 QUESTION 24 - For a diatomic linear chain, the phonon dispersion relation (k) has two branches corresponding to and sign respectively: 2 1 4 1 (M₁ + M₁ ) ± √ [(M₁ + M₁₂) - M₁ M₂ There are two atoms in the unit cell with masses and M2 and the force constant of nearest M₁M₂ M₁ + M₂ neighbor interaction is F and the effective mass, = sound will be: A) B) a M₁ + M₁ 2√2(M₁+M₁) C) a w(k) = f M₁ + M₁ -sin² (9) 1/2 is kept constant. The velocity of
The dispersion relation for a one dimensional monatomic crystal with lattice spacing a, which interacts via nearest neighbor harmonic potential is given by: W=A Asin (), where A is a constant of appropriate unit. The group velocity at the boundary of the first Brillouin zone is: A. 0 B. 1 C. D. Aa² 2 Aa² 2 QUESTION 24 - For a diatomic linear chain, the phonon dispersion relation (k) has two branches corresponding to and sign respectively: 2 1 4 1 (M₁ + M₁ ) ± √ [(M₁ + M₁₂) - M₁ M₂ There are two atoms in the unit cell with masses and M2 and the force constant of nearest M₁M₂ M₁ + M₂ neighbor interaction is F and the effective mass, = sound will be: A) B) a M₁ + M₁ 2√2(M₁+M₁) C) a w(k) = f M₁ + M₁ -sin² (9) 1/2 is kept constant. The velocity of
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Transcribed Image Text:The dispersion relation for a one dimensional monatomic crystal with lattice spacing a, which
interacts via nearest neighbor harmonic potential is given by:
w=A
Asin (), where A is a constant of appropriate unit.
The group velocity at the boundary of the first Brillouin zone is:
A. 0
B. 1
C.
D.
2
Aa²
2
www.
Aq²
QUESTION 24
For a diatomic linear chain, the phonon dispersion relation (k) has two branches corresponding to +
and sign respectively:
1
1
(M₁₂ + M₁₂) ± P | (M₁ + M₁₂
1
There are two atoms in the unit cell with masses and M2 and the force constant of nearest
neighbor interaction is F and the effective mass,
sound will be:
A)
NA
B) =
2
C) a
M₁ + M₁
2(M₁+M₁)
w(k) = f
M₁ + M₁
2
4
M₂)²³ - M₁M₂
M₁M₂
M₁+M₂
sin²
(29/1/²
is kept constant. The velocity of
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