On Aug 4, 2008, at 7:49 PM, Zhu, Lei wrote:
I guess the field enhancement that you mentioned is the Raman scattered field enhancement. Therefore, the E0 is the incident field and the E is the scattered field. You can do the simulation twice. Take a sphere for an example: first, you can just do a calculation without the sphere. Then you can do the calculation with the sphere. You can use the fields gotten with object subtract the fields without the object. I think this is the scattered field which is the E. Then the field without sphere is E0.

Actually, for surface-enhanced Raman scattering you really need to do (at least) four simulations, I think, because the field is enhanced twice.

1) First, you have some incident wave propagating towards the surface with your sphere (or whatever). By having a small metal object like a sphere you will tend to increase the resulting field near the object. This calculation gives you the field near the object.

2) Second, you suppose you have some molecule (analyte) on the surface of your object somewhere, with some (known, experimental) Raman polarizability coefficient. You multiply the field you computed in (1) by this polarizability to get the induced dipole moment of the Raman scatterer. Then you have to do a new simulation with a dipole source at this point, with the given dipole moment determining the current amplitude/direction, to get the Raman-scattered field back at your detector (wherever that is). Note that this simulation is at a slightly different frequency than the first (depending on the process, Stokes or anti-Stokes).

Then, you want to repeat steps (1) and (2) for some reference calculation (e.g. a flat surface) to get the enhancement factor. The increased local density of states near the small object enhances both steps (1) and (2), which is why I said the field is enhanced twice. Hence, four simulations.

You also may want to repeat step (2) multiple times -- in general, there are molecules all over your objects, with some distribution, so you will need to integrate the detected field from step (2) over all positions of the analytes.

Regards,
Steven G. Johnson
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