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Image Search Results
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: ( a ) Optical images of the graphene samples in high- and low-humidity air and in vacuo at 300, 400, 450, and 500 K. Optical images of copper at 500 K are shown for comparison. Visible reflectance spectra of graphene after 420 days at 300 K ( b ), 40 days at 400 K ( c ), 25 days at 450 K ( d ), and 13 days at 500 K ( e ) in high-humidity air (red), in low-humidity air (blue), in vacuo (green), and a bare copper substrate (dotted curves). The visible reflectance spectra of as-prepared graphene (black) are shown for comparison.
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques: Comparison
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: Optical images of graphene samples in high-humidity air, low-humidity air and vacuo at 400 ( a ), 450 ( b ), and 500 K ( c ).
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: ( a ) Raman scattering spectra of graphene after laser irradiation at 0.3 mW. ( b ) D/G and 2D/G band ratios as a function of the irradiation time.
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques: Irradiation
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: Raman spectra of graphene at 300 K, acquired at different times (0–1000 days) after graphene synthesis in high-humidity air, low-humidity air and vacuo.
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: Time dependence of D/G ( a ), 2D/G ratios ( b ), G peak position ( c ), 2D peak position ( d ), FWHM of G bands ( e ), and 2D bands ( f ) in the Raman spectra of graphene in high-humidity air (red), low-humidity air (blue) and vacuo (green). All graphene samples were maintained at 300 K.
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: Raman spectra of graphene at 400 ( a ), 450 ( b ), and 500 K ( c ). Spectra were acquired at 0–40 days (400 K), 0–25 days (450 K), and 0–10 days (500 K) after graphene synthesis in low-humidity air, high-humidity air and vacuo.
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: The 2D/G and D/G ratios in the Raman spectra of graphene in high-humidity air (red), low-humidity air (blue) and vacuo (green) at 400 ( a ), 450 ( b ), and 500 K ( c ).
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: G and 2D peak position in the Raman spectra of graphene in high-humidity air (red), low-humidity air (blue) and vacuo (green) at 400 ( a ), 450 ( b ), and 500 K ( c ).
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: G and 2D peak FWHM in the Raman spectra of graphene in high-humidity air (red), low-humidity air (blue) and vacuo (green) at 400 ( a ), 450 ( b ), and 500 K ( c ).
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: Raman spectra of graphene at 450 on Cu ( a ), Pt ( b ), and quartz ( c ). Spectra were taken after graphene synthesis in low-humidity air, high-humidity air and vacuo.
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques:
Journal: Nanomaterials
Article Title: Degradation of Graphene in High- and Low-Humidity Air, and Vacuum Conditions at 300–500 K
doi: 10.3390/nano14020166
Figure Lengend Snippet: The 2D/G and D/G ratios in the Raman spectra of graphene in high-humidity air (red), low-humidity air (blue) and vacuo (green) at 450 K on Cu ( a ), Pt ( b ), and quartz ( c ).
Article Snippet: The layer numbers and crystallinity changes during the natural degradation of graphene were evaluated from Raman scattering spectra of the
Techniques: