Density of states of Cs3Sb calculated using density-functional theory for modeling photoemission

An analysis is presented that provides a density of states (DOS or D(E)) factor for Cs3Sb in the calculation of its quantum efficiency QE and emittance εn;rms using a Moments Approach. The analysis is based on density functional theory (DFT) adapted for the practical application of treating photoemission from bulk metal and semiconductor materials, and the interfaces between them. The Moments approach treats the processes of absorption, transmission and emission separately, for which DFT affects parameters and processes associated with each step, of which D, the optical constants n and k, and materials parameters such as effective mass mn and band gap Eg are paramount. Such factors are required to provide the components of an evaluation similar to the Tsu-Esaki formula for calculating current density over and through and over barriers, and will become more important when a proper quantum mechanical treatment of the emission barrier is considered beyond the simplistic thermal model (transmission probability is unity only for energy levels in excess of the barrier height and zero otherwise). Such features are expected to be far more consequential if the barrier supports resonant levels, e.g., heterostructures.

[1]  S. Curtarolo,et al.  Finding the Stable Structures of N1-xWx with an Ab Initio High-Throughput Approach , 2014, 1403.2762.

[2]  M. Mehl,et al.  From graphene to graphite: A general tight-binding approach for nanoribbon carrier transport , 2007 .

[3]  C. Hernandez-Garcia,et al.  Electron sources for accelerators , 2008, 2207.08875.

[4]  D. Chadi,et al.  Special points for Brillouin-zone integrations , 1977 .

[5]  J. D. Levine,et al.  Work Function Variation of Metals Coated by Metallic Films , 1962 .

[6]  Hafner,et al.  Ab initio molecular-dynamics simulation of the liquid-metal-amorphous-semiconductor transition in germanium. , 1994, Physical review. B, Condensed matter.

[7]  A. Zunger,et al.  Self-interaction correction to density-functional approximations for many-electron systems , 1981 .

[8]  K. Jensen,et al.  Theory of photoemission from cesium antimonide using an alpha-semiconductor model , 2008 .

[9]  Hafner,et al.  Ab initio molecular dynamics for open-shell transition metals. , 1993, Physical review. B, Condensed matter.

[10]  K. D. Friddell,et al.  First operation of a photocathode radio frequency gun injector at high duty factor , 1993 .

[11]  G. Kresse,et al.  From ultrasoft pseudopotentials to the projector augmented-wave method , 1999 .

[12]  M. Mehl,et al.  Active bialkali photocathodes on free-standing graphene substrates , 2017, npj 2D Materials and Applications.

[13]  P. Hohenberg,et al.  Inhomogeneous electron gas , 1964 .

[14]  Nicola Marzari,et al.  Surface energies, work functions, and surface relaxations of low index metallic surfaces from first principles , 2008, 0801.1077.

[15]  J. Topping On the mutual potential energy of a plane network of doublets , 1927 .

[16]  B. Alder,et al.  THE GROUND STATE OF THE ELECTRON GAS BY A STOCHASTIC METHOD , 2010 .

[17]  W. E. Spicer,et al.  Photoemissive, Photoconductive, and Optical Absorption Studies of Alkali-Antimony Compounds , 1958 .

[18]  Daniel Finkenstadt,et al.  Interphase energies of hcp precipitates in fcc metals: A density-functional theory study in Al-Ag , 2010 .

[19]  Blöchl,et al.  Projector augmented-wave method. , 1994, Physical review. B, Condensed matter.

[20]  Daniel Finkenstadt,et al.  Analysis of nonequilibrium hcp precipitate growth in fcc matrices: Application to Al-Ag , 2009 .

[21]  W. Kohn,et al.  Self-Consistent Equations Including Exchange and Correlation Effects , 1965 .