2021
DOI: 10.1039/d1ra01506k
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How do the doping concentrations of N and B in graphene modify the water adsorption?

Abstract: N and B doping content in graphene alters the microscopic geometrical structure and electronic properties of adsorbed water.

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Cited by 15 publications
(15 citation statements)
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“…The point charge in Table 3 shows that the C atom and O atoms of CO 2 always lose and gain negative charge, respectively. The N atom gains and the B atom loses negative charge, which agrees with then-type andp-type doping nature of these elements [29]. The final result is that the CO 2 -substrate interaction was established in such a way that the CO 2 molecule gains and the substrates donate negative charge for all cases.…”
Section: Resultssupporting
confidence: 76%
“…The point charge in Table 3 shows that the C atom and O atoms of CO 2 always lose and gain negative charge, respectively. The N atom gains and the B atom loses negative charge, which agrees with then-type andp-type doping nature of these elements [29]. The final result is that the CO 2 -substrate interaction was established in such a way that the CO 2 molecule gains and the substrates donate negative charge for all cases.…”
Section: Resultssupporting
confidence: 76%
“…Furthermore, there is a large work function difference between graphene and p-GaNthe most commonly used contact layer in GaN-based LEDs, as seen from Table 1. This mismatch in work function creates an interface contact barrier which further hinders the transport of electrons and holes, increasing contact resistance and operating voltage in LED devices [26], [76]- [78].…”
Section: General Transfer Process and Application Of Graphene To Thin...mentioning
confidence: 99%
“…x Table 1: Work functions of GaN and graphene [26], [78] important applications in disinfection (air, water and surfaces), sterilization, curing, and gas sensing [1]- [4]. Conventional deep-UV lighting systems make use of mercury lamps.…”
mentioning
confidence: 99%
“…Furthermore, the peaks of the adsorbed BTA (right panel of Figure ), particularly for those in the range of −6 to 0 eV, are significantly broadened compared to those of free BTA (left panel). It is well-known that the interaction between the adsorbate and surface is due to the attraction between the occupied states of the substrate and the unoccupied states of the adsorbate and vice versa. , In this work, this property was regulated by changing the energy gap between the valance band maximum (VBM) of the surfaces with the lowest unoccupied molecular orbital (LUMO) of free BTA. From the DOS data, the VBM–LUMO gaps are in the order 3.31 > 2.18 > 2.01 > 1.27 eV for the clean, Fe-, Zn-, and Cu-KLN(001) surfaces, respectively.…”
Section: Resultsmentioning
confidence: 99%