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The alkali-based semiconductor cathodes, such as Cs 3Sb that possesses high quantum efficiency, low electron emittance and short spectral response time, can be considered as ideal next-generation electron sources. However, the alkali-based emitters are found to be sensitive to the oxygen gases, which causes a series of problems such as structural instability, short lifetime, and reduced electron emitting efficiency. It is known that the employing of the ultra-thin layered two-dimensional (2D) materials to protect Cs 3Sb basement can promote the development of novel cathodes with excellent performances. However, there is a lack of efficient 2D materials to maintain low work-function ( W) and high quantum efficiency. Recently, the MXene materials which contain layered transitional metal carbides, nitrides and carbonitrides, have attracted great attention particularly in the fields of catalysis and energy. Notably, their flexible types of dangling bonds can lead to tunable structural and electronic properties of MXene-based materials. Here in this work, the MXene-Cs 3Sb heterostructures are modeled by using home-made script and systematically investigated by using first-principle calculations based on density functional theory. Further, the effects of transitional metal element (M), M/C ratio, stacking configuration and types of dangling bonds on the calculated Wof heterostructures are studied. The result indicates that the type of dangling bond shows a more pronounced effect, and the MXene-Cs 3Sb heterostructures with —OCH 3/—OH possess lower W than other dangling bonds. The charge density difference and band alignment analysis are further used to illustrate the underlying reason for the change of W. And it is found that interlayer charge redistribution can result in different surface dipole directions, and thus emitting electrons with varying barriers. After computational screening based on the change of W, the M 2C(OH) 2(M = V, Ti, Cr) and M 2C(OCH 3) 2(M = Ti, Cr, Nb) can be potentially considered as ideal coating materials, and especially for V 2C(OH) 2-Cs 3Sb ( W= 1.602 eV) and Ti 2C(OCH 3) 2-Cs 3Sb ( W= 1.877 eV) with significantly reduced W. Finally, we believe that this work can not only give an in-depth insight into the electronic and optical properties of Cs 3Sb-MXene heterostructures, but also provide the useful criteria for the computational screening of superior cathodes. Meanwhile, we further urgently expect the cooperative efforts from an experimental perspective to demonstrate the superior performances of those screened MXene-Cs 3Sb photocathodes for practical applications.
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Keywords:
- alkali-based cathodes/
- two-dimensional materials/
- heterostructures/
- first-principle theory
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M2CT2 M2CT2-Cs3Sb in Model-1 M2CT2-Cs3Sb in Model-2 W0/eV W1/eV ∆W1/eV Eb1/(meV·Å–2) W2/eV ∆W2/eV Eb2/(meV·Å–2) Sc2CO2 5.484 3.547 –1.937 –4.161 2.096 –3.388 –5.705 Ta2CS2 5.383 4.490 –0.893 –6.122 5.076 –0.307 –5.364 Zr2C(OH)2 1.701 2.064 0.363 –1.701 2.078 0.377 –1.778 —OH M2C(OH)2-Cs3Sb —OCH3 M2C(OCH3)2-Cs3Sb W0/eV W1/eV ∆W1/eV Eb1/(meV·Å–2) W0/eV W2/eV ∆W2/eV Eb2/(meV·Å–2) Sc2CT2 1.549 1.969 0.05 –2.036 2.869 2.025 0.106 –2.101 Ti2CT2 1.642 1.897 –0.022 –2.235 1.571 1.877 –0.042 –1.678 V2CT2 1.743 1.602 –0.317 –2.065 1.88 1.965 0.046 –1.658 Cr2CT2 1.441 1.813 –0.106 –1.848 2.088 1.896 –0.023 –2.418 Y2CT2 1.348 2.096 0.177 –3.714 2.404 2.118 0.199 –1.696 Zr2CT2 1.700 2.047 0.128 –1.783 1.267 2.003 0.084 –1.300 Nb2CT2 2.012 2.126 0.207 –2.941 1.090 1.904 –0.015 –1.265 Mo2CT2 2.153 1.974 0.055 –1.934 1.610 1.961 0.042 –2.602 Hf2CT2 2.018 2.376 0.457 –3.441 1.582 1.964 0.045 –1.219 Ta2CT2 2.511 2.492 0.573 –2.497 1.375 1.952 0.033 –1.359 W2CT2 2.962 2.599 0.680 –0.600 2.732 1.946 0.027 –1.456 V2CT2 V2CT2-Cs3Sb EA/eV W/eV ∆W/eV Eb/(meV·Å–2) V2C 4.637 4.525 2.606 –5.846 V2CF2 5.542 5.373 3.454 –7.515 V2CO2 6.787 6.441 4.522 –12.23 V2C(OH)2 1.743 1.602 –0.317 –2.065 V2CS2 4.476 4.638 2.719 –5.140 V2CCl2 5.551 5.085 3.166 –7.342 V2C(OCH3)2 1.88 1.965 0.046 –1.659 V2C(NH)2 2.629 2.578 0.659 –3.062 -
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