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    • https://phys.libretexts.org/Bookshelves/Quantum_Mechanics/Quantum_Mechanics_III_(Chong)/06%3A_Appendices/6.02%3A_B-_The_Transfer_Matrix_Method
      Hence, ik[ψ+(xa)ψ(xa)]=ik+[ψ+(xb)ψ(xb)]. These two equations can be combined into a single matrix equation: \[\begin{bmatrix}1 & 1 \\ k...Hence, ik[ψ+(xa)ψ(xa)]=ik+[ψ+(xb)ψ(xb)]. These two equations can be combined into a single matrix equation: [11kk][ψ+(xa)ψ(xa)]=[11k+k+][ψ+(xb)ψ(xb)]. After doing a matrix inversion, this becomes \[\Psi_b = \mathbf{M}_s(k_+,k_-) \, \Psi_a, \;\;\;\mathrm{where}\…
    • https://phys.libretexts.org/Bookshelves/Quantum_Mechanics/Quantum_Mechanics_(Walet)/06%3A_Scattering_from_Potential_Steps_and_Square_Barriers/6.02%3A_Potential_step
      ϕI(x)=A0eik0x+B0eik0x,ϕII(x)=A1eik1x. We define a transmission (T) and reflection (R...\boldsymbol{\begin{align} ϕ_I (x) &= A 0 e^{ i k_0 x} + B_0 e^{ − i k_0 x} , \label{6.7} \\[5pt] ϕ_{II} (x) &= A_1 e^{ i k_1 x} . \label{6.8} \end{align}} We define a transmission (T) and reflection (R) coefficient as the ratio of currents between reflected or transmitted wave and the incoming wave, where we have canceled a common factor A1=2k0k0+k1A0B0=k0k1k0+k1A0,

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