Lambda Theta Alpha

a 0 + a 1 θ + ⋯ + a n − 1 θ n − 1 {\displaystyle \alpha =a_{0}+a_{1}\theta +\cdots +a_{n-1}\theta ^{n-1}} 。ただし、 a 0 ,   a 1 , … ,   a n − 1 {\displaystyle

{\begin{aligned}0&=(\lambda -\sigma _{1})(\lambda -\sigma _{2})(\lambda -\sigma _{3})\\&=\lambda ^{3}-(\sigma _{1}+\sigma _{2}+\sigma _{3})\lambda ^{2}+(\sigma

2\Delta \theta ={\frac {\Delta nL2\pi }{\lambda }}} ここで λ {\displaystyle \,\lambda } は真空中での光の波長である。結局、偏光は角度 θ 0 + Δ θ {\displaystyle \,\theta _{0}+\Delta

{L}}_{z}\psi (r,\theta ,\varphi )} = i ℏ λ ∗ ( F ( 1 , 0 , 0 ) ) ψ ( r , θ , φ ) {\displaystyle =i\hbar \lambda _{*}(F_{(1,0,0)})\psi (r,\theta ,\varphi )}

( λ ) {\displaystyle x(\lambda )=x_{0}\cos(\lambda )-y_{0}\sin(\lambda ),\;y(\lambda )=x_{0}\sin(\lambda )+y_{0}\cos(\lambda )} または [ t x y z ] = [ 1