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High rate CO2 photoreduction using flame annealed TiO2
nanotubes
Fig. 1. Schematic of synthesis of square shaped flame annealed
TiO2 nanotubes
Fig. 2. Cross-section FESEM images of LANT-eg (a), FANT-eg (b), LANT-aq (c) and
FANT-aq (d). Insets are top-view FESEM images of the same.
Fig. 3. HR-TEM images
showing fringe patterns
and 2d spacing of FANT-
eg (a), FANT-aq (b),
LANT-eg (e) and LANT-aq
(f); SAED patterns of
FANT-eg (c), FANT-aq (d),
LANT-eg and (g) LANT-aq
(h).
Fig. 4. (a) Glancing angle XRD patterns of
FANT-eg, LANT-eg, FANT-aq, and LANT-
aq (b) Glancing angle XRD pattern of
FANT-eg specifically, highlighting the
mixed phase nature by separating the
signal from each phase.
Fig. 5. Raman spectra of:
(a) FANT-eg, and LANT-
eg; and (b) FANT-aq, and
LANT-aq.
Fig. 6. UV–vis spectra of the nanotubes.
Fig. 7. High resolution XPS spectra of FANT-eg, LANT-eg, FANT-aq and LANT-aq in
(a–d) Ti 2p region and (e–h) in O 1s region respectively.
Fig. 8. (a) FTIR spectra of gas
sample generated by photoreduction
of 13CO2 using FANT-eg. Shifts to
lower wavenumbers (between 7 and
10 cm−1) of peaks in v3 bands of the
gas sample, from 12CH4 standard,
confirms presence of 13CH4 as a
product. (b) GS MS ion-
chromatogram at m/z = 17,
confirming presence of 13CH4 by
photoreduction of 13CO2.
Fig. 9. Poynting vector plots for (a) LANT and (b) FANT-eg for λ = 450 nm.
Electric field intensity plots for (c) LANT and (d) FANT-eg for λ = 400 nm.
Fig. 10. Plausible mechanism of photoreduction of CO2 by mixed phase
FANT-eg nanotubes. The mechanism is arrived at by closely considering
pertinent reactions and material properties reported in the literature
[98,103,113].
Figure S1. (a) Lorentz fits of anatase (101) and rutile (110) XRD peaks, from which
the peak widths at half of maximum intensities were obtained. Here: (a), (b), (c) and
(d) are for LANT-aq, FANT-aq, LANT-eg and FANT-eg, respectively.
Figure S3. Fluorescence lifetime
imaging lifetime decay plots FLIM
decay plots showing fluorescence
lifetime distributions for the different
nanotube types. Flame annealed TiO2
nanotubes (FANT-eg and FANT-aq)
have longer lifetimes than regular
nanotubes (LANT-eg and LANT-aq).
Figure S4. 2-photon fluorescence images of the nanotubes at excitation wavelength
of 750 nm. Emission was between 394 and 750 nm. Flame annealed TiO2 nanotubes
(FANT-eg and FANT-aq) have a brighter emission than regular nanotubes (LANT-eg
and LANT-aq).
Figure S5. XPS survey scan of FANT-eg (red), LANT-eg (navy blue), FANT-aq
(purple) and LANT-aq (black).
Figure S6. X band EPR spectra of FANT-eg sample recorded at 100 K under dark The Insets
show magnified view of regions and their respective g values. The signal intensity was not
optimal (loss of signal occurred) due to the following reasons: (i) The spectra were collected
in the presence of O2 and (ii) At a temperature of 100 K, electrons have enough energy to
exchange vacancy site which may lead to pairing of some fraction of unpaired electrons
resulting in reduced signal intensity.
Figure S7. Plots of CH4 yield (in terms of µmol g catalyst–1.hr–1) for FANT-eg and LANT-
eg, using LEDs of different wavelengths (400, 450, 500 and 600 nm). LED lights were
operated with a power density of 10 mW cm-2 and the photocatalytic reactions were
performed for 2 hours
Figure S8. CH4 yield (in terms of µmol cm-2
illuminated. area) of CO2 photoreduction using
FANT-aq and LANT-aq under different conditions of illumination. Experiments were
performed in presence of water vapor at 80 ºC.
Figure S9. Plots of the absorption and
scattering intensity of single nanotubes for (a)
LANT (b) FANT-eg and (c) FANT-aq.

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High rate CO2 photoreduction using flame annealed TiO2 nanotubes

  • 1. High rate CO2 photoreduction using flame annealed TiO2 nanotubes
  • 2. Fig. 1. Schematic of synthesis of square shaped flame annealed TiO2 nanotubes
  • 3. Fig. 2. Cross-section FESEM images of LANT-eg (a), FANT-eg (b), LANT-aq (c) and FANT-aq (d). Insets are top-view FESEM images of the same.
  • 4. Fig. 3. HR-TEM images showing fringe patterns and 2d spacing of FANT- eg (a), FANT-aq (b), LANT-eg (e) and LANT-aq (f); SAED patterns of FANT-eg (c), FANT-aq (d), LANT-eg and (g) LANT-aq (h).
  • 5. Fig. 4. (a) Glancing angle XRD patterns of FANT-eg, LANT-eg, FANT-aq, and LANT- aq (b) Glancing angle XRD pattern of FANT-eg specifically, highlighting the mixed phase nature by separating the signal from each phase.
  • 6. Fig. 5. Raman spectra of: (a) FANT-eg, and LANT- eg; and (b) FANT-aq, and LANT-aq.
  • 7. Fig. 6. UV–vis spectra of the nanotubes.
  • 8. Fig. 7. High resolution XPS spectra of FANT-eg, LANT-eg, FANT-aq and LANT-aq in (a–d) Ti 2p region and (e–h) in O 1s region respectively.
  • 9. Fig. 8. (a) FTIR spectra of gas sample generated by photoreduction of 13CO2 using FANT-eg. Shifts to lower wavenumbers (between 7 and 10 cm−1) of peaks in v3 bands of the gas sample, from 12CH4 standard, confirms presence of 13CH4 as a product. (b) GS MS ion- chromatogram at m/z = 17, confirming presence of 13CH4 by photoreduction of 13CO2.
  • 10. Fig. 9. Poynting vector plots for (a) LANT and (b) FANT-eg for λ = 450 nm. Electric field intensity plots for (c) LANT and (d) FANT-eg for λ = 400 nm.
  • 11. Fig. 10. Plausible mechanism of photoreduction of CO2 by mixed phase FANT-eg nanotubes. The mechanism is arrived at by closely considering pertinent reactions and material properties reported in the literature [98,103,113].
  • 12.
  • 13.
  • 14.
  • 15. Figure S1. (a) Lorentz fits of anatase (101) and rutile (110) XRD peaks, from which the peak widths at half of maximum intensities were obtained. Here: (a), (b), (c) and (d) are for LANT-aq, FANT-aq, LANT-eg and FANT-eg, respectively.
  • 16.
  • 17.
  • 18. Figure S3. Fluorescence lifetime imaging lifetime decay plots FLIM decay plots showing fluorescence lifetime distributions for the different nanotube types. Flame annealed TiO2 nanotubes (FANT-eg and FANT-aq) have longer lifetimes than regular nanotubes (LANT-eg and LANT-aq).
  • 19. Figure S4. 2-photon fluorescence images of the nanotubes at excitation wavelength of 750 nm. Emission was between 394 and 750 nm. Flame annealed TiO2 nanotubes (FANT-eg and FANT-aq) have a brighter emission than regular nanotubes (LANT-eg and LANT-aq).
  • 20. Figure S5. XPS survey scan of FANT-eg (red), LANT-eg (navy blue), FANT-aq (purple) and LANT-aq (black).
  • 21. Figure S6. X band EPR spectra of FANT-eg sample recorded at 100 K under dark The Insets show magnified view of regions and their respective g values. The signal intensity was not optimal (loss of signal occurred) due to the following reasons: (i) The spectra were collected in the presence of O2 and (ii) At a temperature of 100 K, electrons have enough energy to exchange vacancy site which may lead to pairing of some fraction of unpaired electrons resulting in reduced signal intensity.
  • 22. Figure S7. Plots of CH4 yield (in terms of µmol g catalyst–1.hr–1) for FANT-eg and LANT- eg, using LEDs of different wavelengths (400, 450, 500 and 600 nm). LED lights were operated with a power density of 10 mW cm-2 and the photocatalytic reactions were performed for 2 hours
  • 23. Figure S8. CH4 yield (in terms of µmol cm-2 illuminated. area) of CO2 photoreduction using FANT-aq and LANT-aq under different conditions of illumination. Experiments were performed in presence of water vapor at 80 ºC.
  • 24. Figure S9. Plots of the absorption and scattering intensity of single nanotubes for (a) LANT (b) FANT-eg and (c) FANT-aq.