Modeling of the Photoelectron Space-Energy Distribution Based on a Contemporary Coupled Photon-Electron Transport Approach

2020 ◽  
Author(s):  
Alexei Kouznetsov ◽  
Levan Lomidze ◽  
Johnathan Burchill ◽  
David Knudsen
2004 ◽  
Vol 832 ◽  
Author(s):  
Yoshishige Tsuchiya ◽  
Takuya Nakatsukasa ◽  
Hiroshi Mizuta ◽  
Shunri Oda ◽  
Akira Kojima ◽  
...  

ABSTRACTMechanism of electron transport through planerized nanocrystalline-Si (nc-Si) cold cathode surface emitting devices was investigated. The energy distribution of electrons emitted from nc-Si emitter was obviously not Maxwellian, which was usually obtained at conventional cold cathode devices, but was similar to that from the nanocrystalline porous silicon diode emitter. These results strongly suggest that electrons are emitted quasiballistically from our devices and indicate that the planarized nc-Si layer play an important role in this high efficiency cold cathode emitter.


2001 ◽  
Vol 693 ◽  
Author(s):  
Ramón Collazo ◽  
Raoul Schlesser ◽  
Amy Roskowski ◽  
Robert F. Davis ◽  
Z. Sitar

AbstractThe energy distribution of electrons transported through an intrinsic AlN film was directly measured as a function of the applied field, and AlN film thickness. Following the transport, electrons were extracted into vacuum through a semitransparent Au electrode and their energy distribution was measured using an electron spectrometer. Transport through films thicker than 95 nm and applied field between 200 kV/cm -350 kV/cm occurred as steady-state hot electron transport represented by a Maxwellian energy distribution, with a corresponding carrier temperature. At higher fields (470 kV/cm), intervalley scattering was evidenced by a multi-component energy distribution with a second peak at the energy position of the first satellite valley. Electron transport through films thinner than 95 nm demonstrated velocity overshoot under fields greater than 550 kV/cm. This was evidenced by a symmetric energy distribution centered at an energy above the conduction band minimum. This indicated that the drift component of the electron velocity was on the order of the “thermal” component. A transient length of less than 80 nm was deduced from these observations.


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