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The angular positions θN of the KKY resonance peaks are given as (Ref.) c kF cot θN =π (N- 1 4) -C, where c is the distance between adjacent conducting planes, kF is the wave vector whose projection is on the Fermi surface, and N is the index of resonance. C is a constant depending on the azimuthal angle.
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The angular positions θN of the KKY resonance peaks are given as (Ref.) c kF cot θN =π (N- 1 4) -C, where c is the distance between adjacent conducting planes, kF is the wave vector whose projection is on the Fermi surface, and N is the index of resonance. C is a constant depending on the azimuthal angle.
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The Lebed's original suggestion (Ref.) was extended to give the resonance angles θp/q for arbitrary azimuthal plane such as (Refs.) By Bz =cot θp/q sin φ = p q bsinγ csinβsin α -cot α*, regardless of Bx. Here, b, c, β, γ, and α* are lattice parameters and p and q are small integers.
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The Lebed's original suggestion (Ref.) was extended to give the resonance angles θp/q for arbitrary azimuthal plane such as (Refs.) By Bz =cot θp/q sin φ= p q bsinγ csinβsin α* -cot α*, regardless of Bx. Here, b, c, β, γ, and α* are lattice parameters and p and q are small integers.
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