What Does the Third-Rank Tensor Represent in Nonlinear Optics?

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The discussion focuses on the representation of polarization in nonlinear optics, specifically addressing the role of third-rank tensors, denoted as X2 or β_{ijk}. In the power series expansion of polarization P(t), X1 represents linear response, while X2 captures the nonlinear response. The indices of the third-rank tensor β_{ijk} indicate the induced electric field in direction i due to the application of incident fields in directions j and k. The conversation clarifies the physical interpretation of these tensors and their application in understanding the polarization of incident light.

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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)
 
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My supervisor told me this:

Polarisability \alpha_{ij}, which is X1 in the power series, is the amplitude of the electric field induced in the molecule in the i direction given a unit amplitude field in the j direction, hence

E_i^{induced} = \alpha_{ij} E_j^{incident}
(observing summation convention)

Extending this physical interpretation, \beta_{ijk} (X2) is the amplitude of the electric field induced in the i direction given an unit incident field in the j direction applied after unit incident field in the k direction has already been applied, so

E_i^{induced} = \beta_{ijk} E_j^{incident2} E_k^{indicent1}

Did I explain that in a way that makes sense?

Thanks
Scott
 
xGAME-OVERx said:
My supervisor told me this:

Polarisability \alpha_{ij}, which is X1 in the power series, is the amplitude of the electric field induced in the molecule in the i direction given a unit amplitude field in the j direction, hence

E_i^{induced} = \alpha_{ij} E_j^{incident}
(observing summation convention)

Extending this physical interpretation, \beta_{ijk} (X2) is the amplitude of the electric field induced in the i direction given an unit incident field in the j direction applied after unit incident field in the k direction has already been applied, so

E_i^{induced} = \beta_{ijk} E_j^{incident2} E_k^{indicent1}

Did I explain that in a way that makes sense?

Thanks
Scott
Yes that makes a lot of sense and is a great start in the right direction. For the linear response, I understand it completely. For for the second order response, there is only one applied (incident) field in the experiment. So when we talk about the direction of the applied field we are talking about the polarization of the incident light?
 

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