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Sum Frequency Generation in a Co- Propagating Beam Geometry from Thin Films Lei Li PhD Candidate, Department of Physics and Astronomy & The Forest Bioproducts.

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Presentation on theme: "Sum Frequency Generation in a Co- Propagating Beam Geometry from Thin Films Lei Li PhD Candidate, Department of Physics and Astronomy & The Forest Bioproducts."— Presentation transcript:

1 Sum Frequency Generation in a Co- Propagating Beam Geometry from Thin Films Lei Li PhD Candidate, Department of Physics and Astronomy & The Forest Bioproducts Research Institute, The University of Maine

2  Sum Frequency Spectroscopy (SFS) is a surface specific non-linear pulsed laser technique capable of providing detailed molecular level orientation & conformational information of interfacial species.  Application of the technique to thin film structures may result in complex spectra which require deconvolution.  In the co-propagating beam geometry, three periodicities describing the relationship between film thickness & SF intensity are found.

3 Thickness/Phase Effect In SFS Spectra( 3 SF beam theoretical model) The phase and intensity of the SF signal arising from thin cellulose films on reflective substrates (gold) is a function of the cellulose film thickness. reflective substrates (gold) is a function of the cellulose film thickness. a) water/cellulose/gold interface. interface. IR=2878cm -1 (r+) IR=2878cm -1 (r+) Dominant Periodicity=268nm Minor Periodicities=296nm, 2857nm b) water/cellulose/gold interface. interface. IR=2966cm -1 (r-) IR=2966cm -1 (r-) c) air/cellulose/gold interface. interface. IR=2878cm -1 (r+) IR=2878cm -1 (r+) d) air/cellulose/gold interface. interface. IR=2966cm -1 (r-) IR=2966cm -1 (r-) Dominant Periodicity=267nm Minor Periodicities=294nm, 2857nm Dominant Periodicity=238nm Minor Periodicities=248nm, 6024nm Dominant Periodicity=237nm Minor Periodicities=247nm, 6024nm

4  If further sources of SF generation are considered, seven additional periodicities can be simulated.

5 Air/cellulose/gold interface, IR=2878cm -1, r+ vibrational mode  Applying the 5 SF beam theoretical model, we can describe the cellulose thickness/phase effect more explicitly.  The three periodicities (red) which are also derived from the 3 beam model are predicted by the 5 beam model, although they do not have the highest intensities.  We have not accounted for beam attenuation which will decrease SF intensity.  Substrates of well defined thickness are presently being prepared for experimental verification of the model’s predictions.Periodicity(nm) SF Intensity(arb) 6024.10.860062 2551.020.438371 1798.5616.4394 1392.767.26852 342.2317.8651 302.1150.344439 287.85321.7658 274.8768.6449 248.260.484184 238.5518.9202 d(nm ) Normalized SF Intensity Normalized SF intensity on resonance versus cellulose thickness

6 Funding  NSF Forest Bioproducts Research Initiative of The University of Maine  The University of Maine Graduate School Acknowledgements : Advisor Dr. David Neivandt Dr. Michael Mason Postdoctoral Dr. Joerg Fick Fellow Graduate Student Sarah Sterling


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