Field-assisted ionization theory for microscopists

Author(s):  
Patrick P. Camus

The theory of field ion emission is the study of electron tunneling probability enhanced by the application of a high electric field. At subnanometer distances and kilovolt potentials, the probability of tunneling of electrons increases markedly. Field ionization of gas atoms produce atomic resolution images of the surface of the specimen, while field evaporation of surface atoms sections the specimen. Details of emission theory may be found in monographs.Field ionization (FI) is the phenomena whereby an electric field assists in the ionization of gas atoms via tunneling. The tunneling probability is a maximum at a critical distance above the surface,xc, Fig. 1. Energy is required to ionize the gas atom at xc, I, but at a value reduced by the appliedelectric field, xcFe, while energy is recovered by placing the electron in the specimen, φ. The highest ionization probability occurs for those regions on the specimen that have the highest local electric field. Those atoms which protrude from the average surfacehave the smallest radius of curvature, the highest field and therefore produce the highest ionizationprobability and brightest spots on the imaging screen, Fig. 2. This technique is called field ion microscopy (FIM).

1998 ◽  
Vol 510 ◽  
Author(s):  
E. Ziemann ◽  
S.D. Ganichev ◽  
I.N. Yassievich ◽  
K. Schmalzv ◽  
W. Prettl

AbstractThe ionization of deep impurity centers by high intensity far-infrared radiation, with photon energies tens of times lower than the impurity binding energy, has been investigated. It is shown that the ionization is caused by phonon-assisted tunneling in the electric field of radiation, in which carrier emission is accompanied by electron tunneling and defect tunneling in the configuration space. The field and temperature dependencies of the ionization probability allow to obtain defect parameters like tunneling times and the Huang-Rhys factor as well as the basic structure of the defect adiabatic potentials. In very strong fields, the ionization changes to direct tunneling without assistance of phonons. It is shown that for the case of charged impurities and in a relatively low electric field strength the Poole-Frenkel effect plays a dominant role in ionization, which allows to identify the charge state of the center. Within a broad range of intensities, wavelengths and temperature, the terahertz electric field of the radiation acts as a static field. An enhancement of tunneling with increase of frequency has been observed for very high frequencies or low temperatures.


2021 ◽  
pp. 2101449
Author(s):  
Shenghan Zhou ◽  
Ke Chen ◽  
Matthew Thomas Cole ◽  
Zhenjun Li ◽  
Mo Li ◽  
...  

2018 ◽  
Vol 98 (5) ◽  
Author(s):  
A. M. Alonso ◽  
L. Gurung ◽  
B. A. D. Sukra ◽  
S. D. Hogan ◽  
D. B. Cassidy

2018 ◽  
Author(s):  
Thomas Kool

<div>Analysis were made to calculate the quadrupole interaction of the Jahn-Teller SrTiO3 system from enhanced EPR spectra due to an applied static electric field. The calculations gave a value for the quadrupole constant |P| = (-2.142 0.005)×10-4 cm-1</div>


Author(s):  
Xi Zhang ◽  
Wenyuan Wu ◽  
Yanchun Gong ◽  
Suhong He ◽  
Fangping Wu ◽  
...  

Abstract The nonlocal effects of dimers consisted of two cylinders are studied, whose cross section is elliptical. Importantly, the results with dimers whose cross section is circular are compared. For comparison, the curvature of the ellipse is set the same with the circle, and four different geometries are considered. The electric field enhancement at the gap center and the absorption spectrum of the dimers are calculated. For the second geometry, either the electric field enhancement at the gap center or the absorption spectrum is approximately calculated using the first geometry, the frequencies corresponding to the peaks are totally different. Similarly, for the fourth geometry, either the electric field enhancement at the gap center or the absorption spectrum is approximately calculated using the third geometry, the disciplines of the peak values change as radius of curvature increases are totally different.


2012 ◽  
Vol 32 (2) ◽  
pp. 0230001
Author(s):  
野仕伟 Ye Shiwei ◽  
戴长建 Dai Changjian ◽  
赵艳红 Zhao Yanhong

2015 ◽  
Vol 35 (6) ◽  
pp. 0602004 ◽  
Author(s):  
马学伟 Ma Xuewei ◽  
马小东 Ma Xiaodong ◽  
戴长建 Dai Changjian

Polymers ◽  
2020 ◽  
Vol 12 (2) ◽  
pp. 489 ◽  
Author(s):  
Ebrahim Yarali ◽  
Reza Noroozi ◽  
Armin Yousefi ◽  
Mahdi Bodaghi ◽  
Mostafa Baghani

Dielectric actuators (DEAs), because of their exceptional properties, are well-suited for soft actuators (or robotics) applications. This article studies a multi-stimuli thermo-dielectric-based soft actuator under large bending conditions. In order to determine the stress components and induced moment (or stretches), a nominal Helmholtz free energy density function with two types of hyperelastic models are employed. Non-linear electro-elasticity theory is adopted to derive the governing equations of the actuator. Total deformation gradient tensor is multiplicatively decomposed into electro-mechanical and thermal parts. The problem is solved using the second-order Runge-Kutta method. Then, the numerical results under thermo-mechanical loadings are validated against the finite element method (FEM) outcomes by developing a user-defined subroutine, UHYPER in a commercial FEM software. The effect of electric field and thermal stimulus are investigated on the mean radius of curvature and stresses distribution of the actuator. Results reveal that in the presence of electric field, the required moment to actuate the actuator is smaller. Finally, due to simplicity and accuracy of the present boundary problem, the proposed thermally-electrically actuator is expected to be used in future studies and 4D printing of artificial thermo-dielectric-based beam muscles.


Nanoscale ◽  
2017 ◽  
Vol 9 (27) ◽  
pp. 9520-9528 ◽  
Author(s):  
Songang Peng ◽  
Zhi Jin ◽  
Dayong Zhang ◽  
Jingyuan Shi ◽  
Yanhui Zhang ◽  
...  

The tunneling probability in metal/graphene contact is not constant, but highly dependent on the Fermi level of graphene under the metal.


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