2017
DOI: 10.1021/acsami.7b00352
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Designing the Interface of Carbon Nanotube/Biomaterials for High-Performance Ultra-Broadband Photodetection

Abstract: Inorganic/biomolecule nanohybrids can combine superior electronic and optical properties of inorganic nanostructures and biomolecules for optoelectronics with performance far surpassing that achievable in conventional materials. The key toward a high-performance inorganic/biomolecule nanohybrid is to design their interface based on the electronic structures of the constituents. A major challenge is the lack of knowledge of most biomolecules due to their complex structures and composition. Here, we first calcul… Show more

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Cited by 39 publications
(35 citation statements)
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“…When the wavelength of the incident light is longer than 1240 nm, the graphene would be the only remaining light absorber. This photogating effect (light‐induced electric field that causes charge doping into a semiconductor) is unique at the interface with semiconductor quantum dots, 2D TMDs, carbon nanotubes or other nanostructures due to the strong quantum confinement and therefore significantly enhanced exciton lifetime in these low‐dimensional nanomaterials . With assistance of the built‐in electric field designed at the interface with these low‐dimensional nanostructures, excitons dissociate into electrons and holes and one of them can be transfer out across the interface.…”
mentioning
confidence: 99%
“…When the wavelength of the incident light is longer than 1240 nm, the graphene would be the only remaining light absorber. This photogating effect (light‐induced electric field that causes charge doping into a semiconductor) is unique at the interface with semiconductor quantum dots, 2D TMDs, carbon nanotubes or other nanostructures due to the strong quantum confinement and therefore significantly enhanced exciton lifetime in these low‐dimensional nanomaterials . With assistance of the built‐in electric field designed at the interface with these low‐dimensional nanostructures, excitons dissociate into electrons and holes and one of them can be transfer out across the interface.…”
mentioning
confidence: 99%
“…As the consequence of this charge transfer from Cyt c to graphene, the oppositely charged carriers remain trapped in the biomolecular layer before charge recombination occurs. Based on the theoretical calculation of density of states for Cyt c and experimental confirmation using ultraviolet photoemission spectroscopy, the highest occupied molecular orbital (HOMO) (−7.24 eV) and lowest unoccupied molecular orbital (LUMO) (−4.92 eV) levels of Cyt c can be determined . The valence band offset between Cyt c and pristine graphene Fermi level (−4.6 eV) is about 2.64 eV, which results in a built‐in electric field across the Cyt c/GFET interface to facilitate exciton dissociation to free charge carriers.…”
Section: Resultsmentioning
confidence: 99%
“…Compared with the inorganic materials used primarily in MOS microelectronics, biomolecules are attractive candidates for high‐performance optoelectronics due to not only their unique electronic and optical properties originated for their complex structures which may not be replicated in synthetic processes, but also the possible control in their bindings in a nonvacuum environment for large‐scale device fabrication. Despite exciting progress made in molecular electronics, main challenges remain in fabrication of the molecular electronic devices. They include (1) complicated and tedious electrode fabrication using advanced lithography on individual molecules and (2) difficulties in implementation of “conventional” diode or transistor designs on molecular devices, such as a p–n type of interface for dissociation of the photoexcited excitons and charge transfer from molecule to electrode .…”
Section: Introductionmentioning
confidence: 99%
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