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. 2024 Dec 10;7(3):766-783.
doi: 10.1039/d4na00463a. eCollection 2025 Jan 28.

Laser writing of metal-oxide doped graphene films for tunable sensor applications

Affiliations

Laser writing of metal-oxide doped graphene films for tunable sensor applications

Shasvat Rathod et al. Nanoscale Adv. .

Abstract

Flexible and wearable devices play a pivotal role in the realm of smart portable electronics due to their diverse applications in healthcare monitoring, soft robotics, human-machine interfaces, and artificial intelligence. Nonetheless, the extensive integration of intelligent wearable sensors into mass production faces challenges within a resource-limited environment, necessitating low-cost manufacturing, high reliability, stability, and multi-functionality. In this study, a cost-effective fiber laser direct writing method (fLDW) was illustrated to create highly responsive and robust flexible sensors. These sensors integrate laser-induced graphene (LiG) with mixed metal oxides on a flexible polyimide film. fLDW simplifies the synthesis of graphene, functionalization of carbon structures into graphene oxides and reduced graphene oxides, and deposition of metal-oxide nanoparticles within a single experimental laser writing setup. The preparation and surface modification of dense oxygenated graphene networks and semiconducting metal oxide nanoparticles (CuO x , ZnO x , FeO x ) enables rapid fabrication of LiG/MO x composite sensors with the ability to detect and differentiate various stimuli, including visible light, UV light, temperature, humidity, and magnetic fluxes. Further, this in situ customizability of fLDW-produced sensors allows for tunable sensitivity, response time, recovery time, and selectivity. The normalized current gain of resistive LiG/MO x sensors can be controlled between -2.7 to 3.5, with response times ranging from 0.02 to 15 s, and recovery times from 0.04 to 6 s. Furthermore, the programmable properties showed great endurance after 200 days in air and extended bend cycles. Collectively, these LiG/MO x sensors stand as a testament to the effectiveness of fLDW in economically mass-producing flexible and wearable electronic devices to meet the explicit demands of the Internet of Things.

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Conflict of interest statement

The authors declare that they have no conflicts of interest regarding the publication of this article.

Figures

Fig. 1
Fig. 1. (a) Fabrication mechanism and schematic of LiG/MOx sensor with fLDW. (b) XRD spectra analysis and (c) SEM images with EDS results of LiG/MOx films.
Fig. 2
Fig. 2. (a) Schematic of electron transport modification on LiG film. (b) Resistive metal-oxide sensing mechanism for p-type and n-type LiG. (c) XRD spectra of GO and rGO films produced through fLDW (d) Laser energy density vs. Conductivity nature of induced LiG films. (e) Laser energy density vs. change in functional groups, data educed from XPS C 1s scans. (f) Time vs. normalized current gain of P-type and N-type LiG/ZnOx samples under 1 V bias and UV stimulus.
Fig. 3
Fig. 3. (a) XPS C 1s scan of a high energy density 1.2 (J mm−3) LiG film. (b) XPS C 1s scan of low energy density 0.8 (J mm−3) LiG film. (c) Laser energy density of fLDW process vs. sp2 fraction. (d) IV curve of LiG films with increasing sp2 C–C fraction. (e) Electron hopping mechanism on GO surface morphology.
Fig. 4
Fig. 4. (a) Nano-particle induced crumpling of rGO mechanism in LiG/MOx films. (b) Sensing mechanism in crumpled rGO sheets with MO nanoparticles. (c) SEM image of LiG crumpling after nanoparticle deposition, low laser energy density (left), and high laser energy density (right). Time vs. change in current output of (d) LiG/FeOx and (e) LiG/ZnOx with different rGO crumpling.
Fig. 5
Fig. 5. Normalized current gain vs. metal oxide percentage extrapolated from XPS spectra of, (a) copper oxide film (b) zinc oxide and (c) iron oxide.
Fig. 6
Fig. 6. (a) XPS Cu 2p scans of LiG/CuOx sensor films with high CuO and Cu2O content; (b) XPS Zn 2p scans of LiG/ZnOx sensor films with different ZnO content; and (c) XPS Fe 2p scans of LiG/FeOx sensor films with different FeOx compositions.
Fig. 7
Fig. 7. IV curves of time vs. normalized change in current of (a) n-type LiG/CuOx sensor (left) and p-type LiG/CuOx (right), (b) n-type LiG/ZnOx sensor (left) and p-type LiG/FeOx sensor (right), and (c) n-type LiG/FeOx sensor (left) and p-type LiG/FeOx sensor (right).
Fig. 8
Fig. 8. Demonstration of different sensors. (a) Schematic of LiG/MOx sensor application on a mechanical finger. (b) Applying as electrode for LiG/ZnOx sensors. (c) Schematic and photo of a multifunctional LiG/MOx sensor grid.
Fig. 9
Fig. 9. (a) LiG sensor 1 V bias without stimuli (b) temperature response of LiG sensor.
Fig. 10
Fig. 10. UV responses of (a) p-type and (b) n-type, LiG/ZnOx sensors.
Fig. 11
Fig. 11. Visible light responses of (a) p-type and (b) n-type LiG/CuOx sensors.
Fig. 12
Fig. 12. Humidity responses of (a) p-type and (b) n-type LiG/MOx sensors.

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