Abstract

Zero-dimensional graphene quantum dots (GQD) dispersed in conducting polymer matrix display a striking range of optical, mechanical, and thermoelectric properties which can be utilized to design next-generation sensors and low-cost thermoelectric. This exotic electrical property in GQDs is achieved by exploiting the concentration of the GQDs and by tailoring the functionalization of the GQDs. However, despite extensive investigation, the nonlinear resistivity behavior leading to memristive like characteristic has not been explored much. Here, we report electrical characterisation of nitrogen functionalized GQD (NGQD) embedded in a polyaniline (PANI) matrix. We observe a strong dependence of the resistance on current and voltage history, the magnitude of which depends on the NGQD concentration and temperature. We explain this memristive property using a phenomenological model of the alignment of PANI rods with a corresponding charge accumulation arising from the NGQD on its surface. The NGQD-PANI system is unique in its ability to design neuromorphic logic and synaptic architectures.

Abstract

Zero-dimensional graphene quantum dots (GQD) dispersed in conducting polymer matrix display a striking range of optical, mechanical, and thermoelectric properties which can be utilized to design next-generation sensors and low-cost thermoelectric. This exotic electrical property in GQDs is achieved by exploiting the concentration of the GQDs and by tailoring the functionalization of the GQDs. However, despite extensive investigation, the nonlinear resistivity behavior leading to memristive like characteristic has not been explored much. Here, we report electrical characterisation of nitrogen functionalized GQD (NGQD) embedded in a polyaniline (PANI) matrix. We observe a strong dependence of the resistance on current and voltage history, the magnitude of which depends on the NGQD concentration and temperature. We explain this memristive property using a phenomenological model of the alignment of PANI rods with a corresponding charge accumulation arising from the NGQD on its surface. The NGQD-PANI system is unique in its ability to design neuromorphic logic and synaptic architectures.

Abstract

Zero-dimensional graphene quantum dots (GQD) dispersed in conducting polymer matrix display a striking range of optical, mechanical, and thermoelectric properties which can be utilized to design next-generation sensors and low-cost thermoelectric. This exotic electrical property in GQDs is achieved by exploiting the concentration of the GQDs and by tailoring the functionalization of the GQDs. However, despite extensive investigation, the nonlinear resistivity behavior leading to memristive like characteristic has not been explored much. Here, we report electrical characterisation of nitrogen functionalized GQD (NGQD) embedded in a polyaniline (PANI) matrix. We observe a strong dependence of the resistance on current and voltage history, the magnitude of which depends on the NGQD concentration and temperature. We explain this memristive property using a phenomenological model of the alignment of PANI rods with a corresponding charge accumulation arising from the NGQD on its surface. The NGQD-PANI system is unique in its ability to design neuromorphic logic and synaptic architectures.

Abstract

Zero-dimensional graphene quantum dots (GQD) dispersed in conducting polymer matrix display a striking range of optical, mechanical, and thermoelectric properties which can be utilized to design next-generation sensors and low-cost thermoelectric. This exotic electrical property in GQDs is achieved by exploiting the concentration of the GQDs and by tailoring the functionalization of the GQDs. However, despite extensive investigation, the nonlinear resistivity behavior leading to memristive like characteristic has not been explored much. Here, we report electrical characterisation of nitrogen functionalized GQD (NGQD) embedded in a polyaniline (PANI) matrix. We observe a strong dependence of the resistance on current and voltage history, the magnitude of which depends on the NGQD concentration and temperature. We explain this memristive property using a phenomenological model of the alignment of PANI rods with a corresponding charge accumulation arising from the NGQD on its surface. The NGQD-PANI system is unique in its ability to design neuromorphic logic and synaptic architectures.