Influence of space charges on the field transition in gas-insulated DC systems

2016 IEEE International Conference on Dielectrics (ICD) ◽

10.1109/icd.2016.7547537 ◽

2016 ◽

Cited By ~ 1

Author(s):

Maria Hering ◽

Thomas Gotz ◽

Joachim Speck ◽

Steffen Grossmann ◽

Uwe Riechert

Keyword(s):

Space Charges ◽

Field Transition

Download Full-text

Equilibrium space charges effect at halide perovskite interactions: The role of ionic charge carriers

10.29363/nanoge.hopv.2019.095 ◽

2019 ◽

Author(s):

Gee Yeong Kim ◽

Alessandro Senocrate ◽

David Moia ◽

Joachim Maier

Keyword(s):

Charge Carriers ◽

Ionic Charge ◽

Space Charges ◽

Halide Perovskite

Download Full-text

Faculty Opinions recommendation of Epithelial fluid transport: protruding macromolecules and space charges can bring about electro-osmotic coupling at the tight junctions.

Faculty Opinions – Post-Publication Peer Review of the Biomedical Literature ◽

10.3410/f.1032491.374200 ◽

2006 ◽

Author(s):

Richard J Naftalin

Keyword(s):

Tight Junctions ◽

Fluid Transport ◽

Space Charges

Download Full-text

Effects of Space Charge on ESEM Gas Amplification

Microscopy and Microanalysis ◽

10.1017/s1431927600009934 ◽

1997 ◽

Vol 3 (S2) ◽

pp. 609-610 ◽

Cited By ~ 1

Author(s):

B.L. Thiel ◽

M.R. Hussein-Ismail ◽

A.M. Donald

Keyword(s):

Electric Field ◽

Electrostatic Field ◽

Secondary Electron ◽

Sample Surface ◽

Cascade Process ◽

Secondary Electrons ◽

Positive Ions ◽

Space Charges ◽

Cascade Amplification ◽

Environmental Sem

We have performed a theoretical investigation of the effects of space charges in the Environmental SEM (ESEM). The ElectroScan ESEM uses an electrostatic field to cause gas cascade amplification of secondary electron signals. Previous theoretical descriptions of the gas cascade process in the ESEM have assumed that distortion of the electric field due to space charges can be neglected. This assumption has now been tested and shown to be valid.In the ElectroScan ESEM, a positively biased detector is located above the sample, creating an electric field on the order of 105 V/m between the detector and sample surface. Secondary electrons leaving the sample are cascaded though the gas, amplifying the signal and creating positive ions. Because the electrons move very quickly through the gas, they do not accumulate in the specimen-to-detector gap. However, the velocity of the positive ions is limited by diffusion.

Download Full-text