1-3 Appendix B

For k⊥=k⊥(ω,X)=ksin⁡ψ and k∥=k∥(ω,X)=kcos⁡ψ, the Jacobian is given by

(B1)|J(k⊥,k∥ω,X)|=|∂k⊥∂ω∂k⊥∂X∂k∥∂ω∂k∥∂X|

Using the standard rules for manipulating derivatives (e.x., Chain rule) gives

(B2)∂k⊥∂ω|X=sin⁡ψ∂k∂ω|X

and

(B3)∂k∥∂ω|X=cos⁡ψ∂k∂ω|X+k∂(cos⁡ψ)∂X|ω(B4)=cos⁡ψ∂k∂ω|X−ksin⁡ψcos2⁡ψ

Similarly,

(B5)∂k⊥∂X|ω=sin⁡ψ∂k∂X|ω+kcos3⁡ψ(B6)∂k⊥∂X|ω=cos⁡ψ∂k∂X|ω

Combining these results gives the Jacobian as

(B7)|J(k⊥,k∥ω,X)|=−kcos2⁡ψ∂k∂ω|X

The derivative term, ∂k∂ω, in the above equation can be found by differentiating the dispersion relation D(k,ω,X)=0 to give

(B8)dDdω=∂D∂ω+∂D∂k∂k∂ω=0

so

(B9)|J(k⊥,k∥ω,X)|=kcos2⁡ψ∂D∂ω(∂D∂k)−1

Thus in 1-3 Appendix A, one find

N(ω)=12π2∫XminXmaxg(X)|J(k⊥,k∥ω,X)|k⊥dX(add)=12π2∫XminXmaxg(X)k2(1+X2)32∂D∂ω[∂D∂k]−1XdX