Patent
US 10,573,517dielectric layer
carbon-containing gas
silicon wafer
Si
hydrogen gas
H₂
silicon dioxide
SiO₂
silicon nitride
Si₃N₄
silicon oxynitride
SiON
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 3. These bands include: (i) the D band (~ 1,350 cm 1) attributing to the breathing mode of sp 2 carbons activated by presence of defects, (ii) the G band …
graphene quality factor (Raman I_2D/I_G ratio), higher bound claim 35 | ≥ 7.5 | C |
single crystalline cobalt layer thickness (claim 10) | 50–20000 | Co |
single crystalline cobalt layer thickness (claim 11) | 50–10000 | Co |
single crystalline cobalt layer thickness (claim 12) | 50–1000 | Co |
Thickness | 50–20000 nm | — |
Thickness | 50–10000 nm | — |
Thickness | 50–1000 nm | — |
Method for Growing High-Quality Graphene Layer
dielectric layer
carbon-containing gas
silicon wafer
Si
hydrogen gas
H₂
silicon dioxide
SiO₂
silicon nitride
Si₃N₄
silicon oxynitride
SiON
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 3. These bands include: (i) the D band (~ 1,350 cm 1) attributing to the breathing mode of sp 2 carbons activated by presence of defects, (ii) the G band …
graphene quality factor (Raman I_2D/I_G ratio), higher bound claim 35 | ≥ 7.5 | C |
single crystalline cobalt layer thickness (claim 10) | 50–20000 | Co |
single crystalline cobalt layer thickness (claim 11) | 50–10000 | Co |
single crystalline cobalt layer thickness (claim 12) | 50–1000 | Co |
Thickness | 50–20000 nm | — |
Thickness | 50–10000 nm | — |
Thickness | 50–1000 nm | — |
Method for Growing High-Quality Graphene Layer
dielectric layer
carbon-containing gas
silicon wafer
Si
hydrogen gas
H₂
silicon dioxide
SiO₂
silicon nitride
Si₃N₄
silicon oxynitride
SiON
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 3. These bands include: (i) the D band (~ 1,350 cm 1) attributing to the breathing mode of sp 2 carbons activated by presence of defects, (ii) the G band …
graphene quality factor (Raman I_2D/I_G ratio), higher bound claim 35 | ≥ 7.5 | C |
single crystalline cobalt layer thickness (claim 10) | 50–20000 | Co |
single crystalline cobalt layer thickness (claim 11) | 50–10000 | Co |
single crystalline cobalt layer thickness (claim 12) | 50–1000 | Co |
Thickness | 50–20000 nm | — |
Thickness | 50–10000 nm | — |
Thickness | 50–1000 nm | — |
Method for Growing High-Quality Graphene Layer
dielectric layer
carbon-containing gas
silicon wafer
Si
hydrogen gas
H₂
silicon dioxide
SiO₂
silicon nitride
Si₃N₄
silicon oxynitride
SiON
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 2A. The strong peak at 44 0 corresponds to either hexagonal closed packed (h c p) Co(0002) or face centered cubic (f c c) Co(111). See Ago et a l., ACS …
FIG. 3. These bands include: (i) the D band (~ 1,350 cm 1) attributing to the breathing mode of sp 2 carbons activated by presence of defects, (ii) the G band …
graphene quality factor (Raman I_2D/I_G ratio), higher bound claim 35 | ≥ 7.5 | C |
single crystalline cobalt layer thickness (claim 10) | 50–20000 | Co |
single crystalline cobalt layer thickness (claim 11) | 50–10000 | Co |
single crystalline cobalt layer thickness (claim 12) | 50–1000 | Co |
Thickness | 50–20000 nm | — |
Thickness | 50–10000 nm | — |
Thickness | 50–1000 nm | — |