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(1) (refractive index) at a sizable interface provides an additional mechanism for THG signal generation.
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84894011544
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note
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2] = 0.12 under the tight-focusing (NA = 1.4) condition. As THG is a third-order nonlinear process, the contributions from the y and z components are negligible. For the same reason, the azimuth-dependent part of the x-polarized component can be neglected.
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25
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Allowed and forbidden light in near-field optics. II. Interacting dipolar particles
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84893992249
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note
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1|, is calculated to be 13.3 μm, which is much larger than the axial length of the focal volume under the tight-focusing condition.
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27
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0035249710
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An epidetected coherent anti-Stokes Raman scattering (E-CARS) microscope with high spectral resolution and high sensitivity
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