figure 3. thermal transformation of meso-hsio 1.5 to meso-ncsi

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Page 1: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi
Page 2: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 1. Compositional characterization of meso-HSiO1.5. A) FTIR spectrum showing characteristic SiH, SiOSi, and HSiO stretching modes from HSiO1.5 and residual SiOH from uncondensed silanol groups. B) 29Si HPDEC MAS NMR spectrum resolved into component T2, T3, Q3, and Q4 centers. C) Schematic representation of T and Q centers comprising the meso-HSiO1.5.

Page 3: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 2. Structural characterizations of meso-HSiO1.5. A) SEM image, B) TEM image, C) SAXS diffraction pattern, and D) N2 adsorptiondesorptionisotherms and DFT pore size distribution (inset) of meso-HSiO1.5.

Page 4: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 3. Thermal transformation of meso-HSiO1.5 to meso-ncSi/SiO2. Evolution of the Raman spectrum of meso-HSiO1.5 as a function of heating from 300 to 1100 C under a slightly reducing atmosphere (5%H2/95% Ar).

Page 5: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 4. Structural characterizations of meso-ncSi/SiO2. A) Evolution of SAXS pattern as a function of processing temperature. The SEM images after processing at B) 900 C and C) 1100 C.

Page 6: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 5. Structural characterizations of meso-ncSi/SiO2. HRTEM imaging of meso-ncSi/SiO2 processed at 900 C (A, C) and 1000 C (B, D, E)showing spherical morphology meso-ncSi/SiO2 particles with mesopores and ncSi. Focused-ion beam prepared cross sections (F) reveal ncSi with latticefringes of 0.31 nm throughout the spherical mesoporous particles. The additional dark spots are due to ca. 1 nm Ga droplets from the FIB processing.

Page 7: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 6. Optical properties of meso-ncSi/SiO2. PL and absorptionspectra for meso-HSiO1.5 processed at 900 and 1000 C showing intensesize-dependent emission at room temperature, consistent with quantumconfinement in ncSi. The absorption spectra are vertically shifted for clarity.

Page 8: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi
Page 9: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 2 . A,B) Optical microscopy images of a superhydrophilic pattern (photografted with AMPS) on a superhydrophobic porous polymer. Scale bars in (A) are 500 μ m and in (B) are 2 mm. The patterns were wetted with water making the hydrophilic areas more transparent. C) Water droplets on the superhydrophobic microporous poly(butyl methacrylate- co -ethylene dimethacrylate) (left) and on the same surface after photografting with AMPS (right). D,E) Superhydrophilic patterns with different geometries and sizes fi lled with water dye solutions. F) Cross-sections of 200- μ m-wide superhydrophilic microchannels (photografted with AMPS) colored with a water solution of neutral red. Polymer films: 50- and 25- μ m-thick microporous poly(butyl methacrylate- co -ethylene dimethacrylate) films. Scale bars are 100 μ m.

Page 10: Figure 3. Thermal transformation of meso-HSiO 1.5  to  meso-ncSi

Figure 3 . SEM images of the cross-sections of A,B) microporous and C,D) nanoporous poly(butyl methacrylate- co -ethylene dimethacrylate) fi lms. Scalebars in (A,C) are 10 μ m and in (B,D) are 1 μ m.