Patent
US 10,505,193polyether ether ketone
doped polymer
boron doped polymer
porous graphene
doped graphene
boron-doped graphene
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIGS. 3B-C, black contrast is LIG after exposure to the laser, while the lighter background co rr esponds to P I. The laser power used to scribe the images was …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 6). [00191] The micro- and nano-structure of LIG flakes was investigated by transmission electron microscopy (TEM).
FIG. 7B provides a TEM image of a thick LIG flake showing entangled tree-like ripples. The scale bar is 100 nm. Inset is the high resolution TEM (HRTEM) image …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 9E. The scale bar is 5 n m. The d isordered graphene structure was enhanced. [0023] FIGURE 10 provides a BET specific surface area of L I G-3.6 W. The …
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 13). If the scan rate increases, higher threshold power needs to be applied in order to initiate the graphitization. Meanwhile, the sheet resistance (R S) …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 20B provides specific volumetric capacitances as a function of discharge cu rr ent densities in BMI M-BF 4. [0034] FIGURE 21 provides electrochemical …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 32B). [0046] FIGURE 33 shows XPS spectra of 5B-L I G and PI/H 3 B O 3 sheets.
FIG. 33D shows the N I s spectrum. [0047] FIGURE 34 provides an electrochemical performance comparison of L I G-MSCs with different H 3 B 0 3 loadings.
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 35H are identical to each other, suggesting that bending had little effect on the electrochemical performance of 5B-L I G-MSC. [00249] To further …
FIG. 36D provides galvanostatic CC curves of 5B-L I G-MSC at current densities of 10, 20 and 30 mA/cm 2. [0050] FIGURE 37 provides impedance performances of L …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 42C, with the highest capacitance being 9.11 mF/cm 2 at a co rr esponding current density of 0.01 mA/cm 2, comparable to the values reported in the …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 45B provides pore size distributions of LIGs. [0059] FIGURE 46 provides additional electrochemical performance of a flat, single L I G-SC.
FIG. 46B provides Galvanostatic CC curves of L I G-SCs at current densities of 0.5, 1.0 and 2.0 mA/cm 2. [0060] FIGURE 47 provides electrochemical performance …
FIG. 47C provides cyclability testing of flexible L I G-SCs. Capacitance retention was calculated from CC curves at a current density of 0.4 mA/cm 2. [0061] …
FIGS. 48A-B are illustrations of a series and parallel L I G-SC assembled from stacked solid- state L I G-SCs, where double-sided LIG sheets are layered with …
FIG. 49B provides galvanostatic charge-discharge curves of series L I G-SCs at cu rr ent densities of 0.1, 0.2 and 0.5 mA/cm 2. [0063] FIGURE 50 provides …
FIG. 50 C provides specific areal capacitance calculated from discharge runtime as a function of cu rr ent density. [0064] FIGURE 51 provides electrochemical …
FIG. 51 E provides capacity retention of L I G-MSC at different bending radii. Capacitance retention was calculated from CC curves at a current density of 0.5 …
FIG. 52C provides CC curves of L I G-MSCs at cu rr ent densities of 2, 5, 10 and 20 mA/cm 2. [0066] FIGURE 53 provides impedance performances of L I G-MSCs …
FIG. 55. As expected, the working voltage was doubled when LIG-MSCs were in series, while the discharge runtime increased nearly 100% when LIG-MSCs were in …
FIG. 59. The 9.3 micrometer band has a tuning range of 2 0.15 micrometers, and the other three bands have tuning ranges of z 0.2 micrometers. [00294] The …
durability under mechanical stress. When the device was bent and fixed (FIG. 35E) at different bending radii (from 7 to 17 mm), the calculated CA fr o m discharge runtime remained essentially constant, as shown in FIG. 3 5 F. Furthermore, after 8000 bending cycl
electronic device capacitance (claimed range) | 2–1000 | — |
electronic device power density (claimed range) | 5–200 | — |
capacitance retention ≥90% after >10,000 cycles | ≥ 90 | — |
Thickness | 5–10 nm | — |
Thickness | 10–400 nm | — |
Thickness | 400–800 nm | — |
— | 1–10 W | — |
— | 1–6 W | — |
— | 2–5 W | — |
— | 2–4 W | — |
— | 2–3 W | — |
— | 2.4–5.4 W | — |
Temperature | 500–2000 °C | — |
Thickness | 10000000–1000000000 nm | — |
Thickness | 1–10 cm | — |
Thickness | 1000000–10000000 nm | — |
Thickness | 0.3–10000000 nm | — |
Thickness | 1–10 mm | — |
Thickness | 1–5000 nm | — |
Temperature | 100–900 °C | — |
Thickness | 12–24 mm | — |
Thickness | 1–1700 cm | — |
Voltage | 1–5 V | — |
Temperature | 800–1500 °C | — |
Thickness | 7–17 mm | — |
Thickness | 9–11 µm | — |
Thickness | 1090–1776 cm | — |
Pressure | 1e-9 Torr | — |
Thickness | 2–10 nm | — |
Thickness | ≤ 50 nm | — |
Thickness | ≤ 9 nm | — |
Thickness | ≤ 2 nm | — |
— | ≤ 4.2 W | — |
— | ≤ 0.01 eV | — |
Thickness | ≤ 10 nm | — |
Temperature | ≥ 900 °C | — |
— | ≥ 4.2 W | — |
Temperature | ≥ 2500 °C | — |
— | 1–100 W | — |
polyether ether ketone
doped polymer
boron doped polymer
porous graphene
doped graphene
boron-doped graphene
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIGS. 3B-C, black contrast is LIG after exposure to the laser, while the lighter background co rr esponds to P I. The laser power used to scribe the images was …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 6). [00191] The micro- and nano-structure of LIG flakes was investigated by transmission electron microscopy (TEM).
FIG. 7B provides a TEM image of a thick LIG flake showing entangled tree-like ripples. The scale bar is 100 nm. Inset is the high resolution TEM (HRTEM) image …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 9E. The scale bar is 5 n m. The d isordered graphene structure was enhanced. [0023] FIGURE 10 provides a BET specific surface area of L I G-3.6 W. The …
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 13). If the scan rate increases, higher threshold power needs to be applied in order to initiate the graphitization. Meanwhile, the sheet resistance (R S) …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 20B provides specific volumetric capacitances as a function of discharge cu rr ent densities in BMI M-BF 4. [0034] FIGURE 21 provides electrochemical …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 32B). [0046] FIGURE 33 shows XPS spectra of 5B-L I G and PI/H 3 B O 3 sheets.
FIG. 33D shows the N I s spectrum. [0047] FIGURE 34 provides an electrochemical performance comparison of L I G-MSCs with different H 3 B 0 3 loadings.
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 35H are identical to each other, suggesting that bending had little effect on the electrochemical performance of 5B-L I G-MSC. [00249] To further …
FIG. 36D provides galvanostatic CC curves of 5B-L I G-MSC at current densities of 10, 20 and 30 mA/cm 2. [0050] FIGURE 37 provides impedance performances of L …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 42C, with the highest capacitance being 9.11 mF/cm 2 at a co rr esponding current density of 0.01 mA/cm 2, comparable to the values reported in the …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 45B provides pore size distributions of LIGs. [0059] FIGURE 46 provides additional electrochemical performance of a flat, single L I G-SC.
FIG. 46B provides Galvanostatic CC curves of L I G-SCs at current densities of 0.5, 1.0 and 2.0 mA/cm 2. [0060] FIGURE 47 provides electrochemical performance …
FIG. 47C provides cyclability testing of flexible L I G-SCs. Capacitance retention was calculated from CC curves at a current density of 0.4 mA/cm 2. [0061] …
FIGS. 48A-B are illustrations of a series and parallel L I G-SC assembled from stacked solid- state L I G-SCs, where double-sided LIG sheets are layered with …
FIG. 49B provides galvanostatic charge-discharge curves of series L I G-SCs at cu rr ent densities of 0.1, 0.2 and 0.5 mA/cm 2. [0063] FIGURE 50 provides …
FIG. 50 C provides specific areal capacitance calculated from discharge runtime as a function of cu rr ent density. [0064] FIGURE 51 provides electrochemical …
FIG. 51 E provides capacity retention of L I G-MSC at different bending radii. Capacitance retention was calculated from CC curves at a current density of 0.5 …
FIG. 52C provides CC curves of L I G-MSCs at cu rr ent densities of 2, 5, 10 and 20 mA/cm 2. [0066] FIGURE 53 provides impedance performances of L I G-MSCs …
FIG. 55. As expected, the working voltage was doubled when LIG-MSCs were in series, while the discharge runtime increased nearly 100% when LIG-MSCs were in …
FIG. 59. The 9.3 micrometer band has a tuning range of 2 0.15 micrometers, and the other three bands have tuning ranges of z 0.2 micrometers. [00294] The …
durability under mechanical stress. When the device was bent and fixed (FIG. 35E) at different bending radii (from 7 to 17 mm), the calculated CA fr o m discharge runtime remained essentially constant, as shown in FIG. 3 5 F. Furthermore, after 8000 bending cycl
electronic device capacitance (claimed range) | 2–1000 | — |
electronic device power density (claimed range) | 5–200 | — |
capacitance retention ≥90% after >10,000 cycles | ≥ 90 | — |
Thickness | 5–10 nm | — |
Thickness | 10–400 nm | — |
Thickness | 400–800 nm | — |
— | 1–10 W | — |
— | 1–6 W | — |
— | 2–5 W | — |
— | 2–4 W | — |
— | 2–3 W | — |
— | 2.4–5.4 W | — |
Temperature | 500–2000 °C | — |
Thickness | 10000000–1000000000 nm | — |
Thickness | 1–10 cm | — |
Thickness | 1000000–10000000 nm | — |
Thickness | 0.3–10000000 nm | — |
Thickness | 1–10 mm | — |
Thickness | 1–5000 nm | — |
Temperature | 100–900 °C | — |
Thickness | 12–24 mm | — |
Thickness | 1–1700 cm | — |
Voltage | 1–5 V | — |
Temperature | 800–1500 °C | — |
Thickness | 7–17 mm | — |
Thickness | 9–11 µm | — |
Thickness | 1090–1776 cm | — |
Pressure | 1e-9 Torr | — |
Thickness | 2–10 nm | — |
Thickness | ≤ 50 nm | — |
Thickness | ≤ 9 nm | — |
Thickness | ≤ 2 nm | — |
— | ≤ 4.2 W | — |
— | ≤ 0.01 eV | — |
Thickness | ≤ 10 nm | — |
Temperature | ≥ 900 °C | — |
— | ≥ 4.2 W | — |
Temperature | ≥ 2500 °C | — |
— | 1–100 W | — |
polyether ether ketone
doped polymer
boron doped polymer
porous graphene
doped graphene
boron-doped graphene
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIGS. 3B-C, black contrast is LIG after exposure to the laser, while the lighter background co rr esponds to P I. The laser power used to scribe the images was …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 6). [00191] The micro- and nano-structure of LIG flakes was investigated by transmission electron microscopy (TEM).
FIG. 7B provides a TEM image of a thick LIG flake showing entangled tree-like ripples. The scale bar is 100 nm. Inset is the high resolution TEM (HRTEM) image …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 9E. The scale bar is 5 n m. The d isordered graphene structure was enhanced. [0023] FIGURE 10 provides a BET specific surface area of L I G-3.6 W. The …
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 13). If the scan rate increases, higher threshold power needs to be applied in order to initiate the graphitization. Meanwhile, the sheet resistance (R S) …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 20B provides specific volumetric capacitances as a function of discharge cu rr ent densities in BMI M-BF 4. [0034] FIGURE 21 provides electrochemical …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 32B). [0046] FIGURE 33 shows XPS spectra of 5B-L I G and PI/H 3 B O 3 sheets.
FIG. 33D shows the N I s spectrum. [0047] FIGURE 34 provides an electrochemical performance comparison of L I G-MSCs with different H 3 B 0 3 loadings.
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 35H are identical to each other, suggesting that bending had little effect on the electrochemical performance of 5B-L I G-MSC. [00249] To further …
FIG. 36D provides galvanostatic CC curves of 5B-L I G-MSC at current densities of 10, 20 and 30 mA/cm 2. [0050] FIGURE 37 provides impedance performances of L …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 42C, with the highest capacitance being 9.11 mF/cm 2 at a co rr esponding current density of 0.01 mA/cm 2, comparable to the values reported in the …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 45B provides pore size distributions of LIGs. [0059] FIGURE 46 provides additional electrochemical performance of a flat, single L I G-SC.
FIG. 46B provides Galvanostatic CC curves of L I G-SCs at current densities of 0.5, 1.0 and 2.0 mA/cm 2. [0060] FIGURE 47 provides electrochemical performance …
FIG. 47C provides cyclability testing of flexible L I G-SCs. Capacitance retention was calculated from CC curves at a current density of 0.4 mA/cm 2. [0061] …
FIGS. 48A-B are illustrations of a series and parallel L I G-SC assembled from stacked solid- state L I G-SCs, where double-sided LIG sheets are layered with …
FIG. 49B provides galvanostatic charge-discharge curves of series L I G-SCs at cu rr ent densities of 0.1, 0.2 and 0.5 mA/cm 2. [0063] FIGURE 50 provides …
FIG. 50 C provides specific areal capacitance calculated from discharge runtime as a function of cu rr ent density. [0064] FIGURE 51 provides electrochemical …
FIG. 51 E provides capacity retention of L I G-MSC at different bending radii. Capacitance retention was calculated from CC curves at a current density of 0.5 …
FIG. 52C provides CC curves of L I G-MSCs at cu rr ent densities of 2, 5, 10 and 20 mA/cm 2. [0066] FIGURE 53 provides impedance performances of L I G-MSCs …
FIG. 55. As expected, the working voltage was doubled when LIG-MSCs were in series, while the discharge runtime increased nearly 100% when LIG-MSCs were in …
FIG. 59. The 9.3 micrometer band has a tuning range of 2 0.15 micrometers, and the other three bands have tuning ranges of z 0.2 micrometers. [00294] The …
durability under mechanical stress. When the device was bent and fixed (FIG. 35E) at different bending radii (from 7 to 17 mm), the calculated CA fr o m discharge runtime remained essentially constant, as shown in FIG. 3 5 F. Furthermore, after 8000 bending cycl
electronic device capacitance (claimed range) | 2–1000 | — |
electronic device power density (claimed range) | 5–200 | — |
capacitance retention ≥90% after >10,000 cycles | ≥ 90 | — |
Thickness | 5–10 nm | — |
Thickness | 10–400 nm | — |
Thickness | 400–800 nm | — |
— | 1–10 W | — |
— | 1–6 W | — |
— | 2–5 W | — |
— | 2–4 W | — |
— | 2–3 W | — |
— | 2.4–5.4 W | — |
Temperature | 500–2000 °C | — |
Thickness | 10000000–1000000000 nm | — |
Thickness | 1–10 cm | — |
Thickness | 1000000–10000000 nm | — |
Thickness | 0.3–10000000 nm | — |
Thickness | 1–10 mm | — |
Thickness | 1–5000 nm | — |
Temperature | 100–900 °C | — |
Thickness | 12–24 mm | — |
Thickness | 1–1700 cm | — |
Voltage | 1–5 V | — |
Temperature | 800–1500 °C | — |
Thickness | 7–17 mm | — |
Thickness | 9–11 µm | — |
Thickness | 1090–1776 cm | — |
Pressure | 1e-9 Torr | — |
Thickness | 2–10 nm | — |
Thickness | ≤ 50 nm | — |
Thickness | ≤ 9 nm | — |
Thickness | ≤ 2 nm | — |
— | ≤ 4.2 W | — |
— | ≤ 0.01 eV | — |
Thickness | ≤ 10 nm | — |
Temperature | ≥ 900 °C | — |
— | ≥ 4.2 W | — |
Temperature | ≥ 2500 °C | — |
— | 1–100 W | — |
polyether ether ketone
doped polymer
boron doped polymer
porous graphene
doped graphene
boron-doped graphene
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIG. 2B. The scale bar is 10 m. The inset is the corr esponding higher magnification SEM image with a scale bar of 1 m.
FIGS. 3B-C, black contrast is LIG after exposure to the laser, while the lighter background co rr esponds to P I. The laser power used to scribe the images was …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 5 D provides high resolution N i s XPS spectrum of a LIG-3.6 W film and P I. The intensity of the N I s peak was greatly reduced after laser exposure. …
FIG. 6). [00191] The micro- and nano-structure of LIG flakes was investigated by transmission electron microscopy (TEM).
FIG. 7B provides a TEM image of a thick LIG flake showing entangled tree-like ripples. The scale bar is 100 nm. Inset is the high resolution TEM (HRTEM) image …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 8A. Moreover, ripple-like wrinkled structures can be observed from the surface of the flakes. These structures in graphene have been shown to improve the …
FIG. 9E. The scale bar is 5 n m. The d isordered graphene structure was enhanced. [0023] FIGURE 10 provides a BET specific surface area of L I G-3.6 W. The …
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 12D. The L a values calculated from the average IG"I D rati o using eq 4 and the methods described in this Example is shown in the lower panel of
FIG. 13). If the scan rate increases, higher threshold power needs to be applied in order to initiate the graphitization. Meanwhile, the sheet resistance (R S) …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 14) that had been peeled off the P I substrate. Raman spectroscopy is a powerful tool to obtain crystalline size (L a) along the a-axis of graphitic …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 15B provides a Raman spectrum of P EI -derived LIG obtained with a laser power of 3.0 W. [0029] FIGURE 16 provides electrochemical performances of …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 16N. Clearly, a polycrystalline sheet has a much higher C q than perfect graphene, as a result of a higher density of states near the Fermi level due to …
FIG. 20B provides specific volumetric capacitances as a function of discharge cu rr ent densities in BMI M-BF 4. [0034] FIGURE 21 provides electrochemical …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 21. Monkhorst-Pack (MP) k-points sampling is used, with a vacuum space >15 A in the non-periodic direction. To obtain the density of states (DOS), …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 26B. The dehydration from PAA to PI is preferred for successful formation of LIG and will be discussed in detail herein. [00235] Finally, a standard C O 2 …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIG. 27B). After that, Pellco ® colloidal silver paint (No. 16034, Ted Pella) was first applied on the common areas of both electrodes for better electrical …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIGS. 28-29). No significant difference was found among these samples, indicating that the loading of H 3 B 0 3 has little effect on the morphology of the …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 30D shows the pore size distribution of 5B-L I G, which are all < 10 nm (26 A, 41 A and 73 A). [00241] To confirm the boron doping in the product, X-ray …
FIG. 32B). [0046] FIGURE 33 shows XPS spectra of 5B-L I G and PI/H 3 B O 3 sheets.
FIG. 33D shows the N I s spectrum. [0047] FIGURE 34 provides an electrochemical performance comparison of L I G-MSCs with different H 3 B 0 3 loadings.
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 34A. A solid-state electrolyte made from poly(vinyl alcohol) (PVA) and H 2 S O 4 was used to ensure the flexibility of the device (as discussed in Example …
FIG. 35H are identical to each other, suggesting that bending had little effect on the electrochemical performance of 5B-L I G-MSC. [00249] To further …
FIG. 36D provides galvanostatic CC curves of 5B-L I G-MSC at current densities of 10, 20 and 30 mA/cm 2. [0050] FIGURE 37 provides impedance performances of L …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 39E is a TEM image of a LIG thin film showing nano-sized wrinkles and ripples. The inset is a HRTEM image of a LIG nanosheet showing numerous graphene …
FIG. 42C, with the highest capacitance being 9.11 mF/cm 2 at a co rr esponding current density of 0.01 mA/cm 2, comparable to the values reported in the …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 43B provides an XRD spectrum of LIGs. [0057] FIGURE 44 provides a TGA plot of LIG and P I substrates under argon. P I starts to decompose at-550 ° C, …
FIG. 45B provides pore size distributions of LIGs. [0059] FIGURE 46 provides additional electrochemical performance of a flat, single L I G-SC.
FIG. 46B provides Galvanostatic CC curves of L I G-SCs at current densities of 0.5, 1.0 and 2.0 mA/cm 2. [0060] FIGURE 47 provides electrochemical performance …
FIG. 47C provides cyclability testing of flexible L I G-SCs. Capacitance retention was calculated from CC curves at a current density of 0.4 mA/cm 2. [0061] …
FIGS. 48A-B are illustrations of a series and parallel L I G-SC assembled from stacked solid- state L I G-SCs, where double-sided LIG sheets are layered with …
FIG. 49B provides galvanostatic charge-discharge curves of series L I G-SCs at cu rr ent densities of 0.1, 0.2 and 0.5 mA/cm 2. [0063] FIGURE 50 provides …
FIG. 50 C provides specific areal capacitance calculated from discharge runtime as a function of cu rr ent density. [0064] FIGURE 51 provides electrochemical …
FIG. 51 E provides capacity retention of L I G-MSC at different bending radii. Capacitance retention was calculated from CC curves at a current density of 0.5 …
FIG. 52C provides CC curves of L I G-MSCs at cu rr ent densities of 2, 5, 10 and 20 mA/cm 2. [0066] FIGURE 53 provides impedance performances of L I G-MSCs …
FIG. 55. As expected, the working voltage was doubled when LIG-MSCs were in series, while the discharge runtime increased nearly 100% when LIG-MSCs were in …
FIG. 59. The 9.3 micrometer band has a tuning range of 2 0.15 micrometers, and the other three bands have tuning ranges of z 0.2 micrometers. [00294] The …
durability under mechanical stress. When the device was bent and fixed (FIG. 35E) at different bending radii (from 7 to 17 mm), the calculated CA fr o m discharge runtime remained essentially constant, as shown in FIG. 3 5 F. Furthermore, after 8000 bending cycl
electronic device capacitance (claimed range) | 2–1000 | — |
electronic device power density (claimed range) | 5–200 | — |
capacitance retention ≥90% after >10,000 cycles | ≥ 90 | — |
Thickness | 5–10 nm | — |
Thickness | 10–400 nm | — |
Thickness | 400–800 nm | — |
— | 1–10 W | — |
— | 1–6 W | — |
— | 2–5 W | — |
— | 2–4 W | — |
— | 2–3 W | — |
— | 2.4–5.4 W | — |
Temperature | 500–2000 °C | — |
Thickness | 10000000–1000000000 nm | — |
Thickness | 1–10 cm | — |
Thickness | 1000000–10000000 nm | — |
Thickness | 0.3–10000000 nm | — |
Thickness | 1–10 mm | — |
Thickness | 1–5000 nm | — |
Temperature | 100–900 °C | — |
Thickness | 12–24 mm | — |
Thickness | 1–1700 cm | — |
Voltage | 1–5 V | — |
Temperature | 800–1500 °C | — |
Thickness | 7–17 mm | — |
Thickness | 9–11 µm | — |
Thickness | 1090–1776 cm | — |
Pressure | 1e-9 Torr | — |
Thickness | 2–10 nm | — |
Thickness | ≤ 50 nm | — |
Thickness | ≤ 9 nm | — |
Thickness | ≤ 2 nm | — |
— | ≤ 4.2 W | — |
— | ≤ 0.01 eV | — |
Thickness | ≤ 10 nm | — |
Temperature | ≥ 900 °C | — |
— | ≥ 4.2 W | — |
Temperature | ≥ 2500 °C | — |
— | 1–100 W | — |