When two immiscible polymer surfaces are contacted, it is expected that their surface functionality will arrange or structure to minimize free energy. Understanding the structure of polymer/ polymer interfaces is important in areas of adhesion, polymer blends, and nanocomposites. The current understanding of polymer/ polymer interface structure is based on interfacial energies, either measured or calculated on the basis of the Flory-Huggins parameter, which accounts for unfavorable interaction of the different monomer repeat units. 1,2 However, directly probing the structure and orientation at polymer/polymer interfaces has not been possible due to insufficient contrast between the bulk and the interface. In this work we have taken advantage of recent developments in infrared-visible sum frequency spectroscopy (SFG) to study polymer/polymer interfaces. This technique has been recently used to study a variety of polymer interfaces including polymer/ air, polymer/liquid, and polymer/solid interfaces. [3][4][5][6] Here we report the first SFG measurement of molecular structure at poly(vinyl-N-octadecylcarbamate-co-vinyl acetate)/poly(styrene) (Comb/PS) polymer/polymer interface. The carbamate Comb polymers are widely used as release coatings for pressure sensitive adhesives, and their low adhesion at polymer/polymer interfaces with adhesives is attributed to their interfacial structure. 7 SFG involves mixing a visible high-intensity laser beam of frequency ω 1 , with a tunable infrared wavelength source of frequency ω 2 . According to the dipole approximation, generation of a SFG photon (at ω 3 ) ω 1 + ω 2 ) is forbidden in the centrosymmetric bulk and is nonzero at interfaces where inversion symmetry is broken. The SFG is resonantly enhanced when ω 2 overlaps with the resonant frequency of a molecular vibrational mode that is both infrared and Raman active. The SFG output is also enhanced by 1 to 2 orders of magnitude when the incidence angle of the input beams is close to the critical angle for total internal reflection (explained by higher Fresnel coefficients of the reflected SFG signal near critical angles). The enhancement in SFG signal near critical angles has been used recently to study liquid/ liquid 8 and polymer/solid interfaces. 5,6 Further details of SFG theory and the details of SFG spectrometers have been discussed previously. 9,10 Samples for SFG were prepared by spin coating a film ∼300-nm thick from a 5 wt % solution of hPS (M w ) 108 kg/mol, M w / M n ≈ 1.06 or deuterated PS, M w ) 125 kg/mol M w /M n ≈ 1.13) in toluene onto the surface of a sapphire prism and annealing the film at 110°C under vacuum for 3 h. A second film ∼200 nm thick was then spin-cast on top of the first from a warm 6 wt % solution of Comb (M w ) 70 kg/mol M w /M n ≈ 3.0) in 50/50 mixture of octanol and butanol (both nonsolvents for PS), and the bilayer sample (Figure 1) was annealed again for 3 h at 110°C under vacuum. For comparison in separate experiments a film ∼200 nm thick was spin-cast from 6 wt % solution of Comb in t...