DanSandberg
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In nonlinear optics the polarization of a molecule can be represented as a power series:
P(t)=X1E(t)+X2E2(t)+X3E3(t)+...
Where X1E(t) is the linear response and everything after is nonlinear. The polarization, P(t) and field strength E(t) are both vectors and X2 is a third-rank tensor, X3 is a fourth-rank, etc.
My question is... why is X2 a third-rank tensor? I'm having difficulty getting a straight answer as to what the indices represent. So in a paper where they say \betaxxx what does that mean? (Where \beta is commonly used in place of X2)
P(t)=X1E(t)+X2E2(t)+X3E3(t)+...
Where X1E(t) is the linear response and everything after is nonlinear. The polarization, P(t) and field strength E(t) are both vectors and X2 is a third-rank tensor, X3 is a fourth-rank, etc.
My question is... why is X2 a third-rank tensor? I'm having difficulty getting a straight answer as to what the indices represent. So in a paper where they say \betaxxx what does that mean? (Where \beta is commonly used in place of X2)