Switching the chirality of a ferroelectric vortex in designed nanostructures by a homogeneous electric field

2017 ◽  
Vol 96 (13) ◽  
Author(s):  
Le Van Lich ◽  
Takahiro Shimada ◽  
Jie Wang ◽  
Van-Hai Dinh ◽  
Tinh Quoc Bui ◽  
...  
Keyword(s):  
Electric Field ◽  
Homogeneous Electric Field ◽  
Ferroelectric Vortex

Contour-clamped homogeneous electric field electrophoresis of Staphylococcus aureus

2006 ◽  
Vol 1 (6) ◽  
pp. 3028-3033 ◽  
Author(s):  
Frances G O'Brien ◽  
Edet E Udo ◽  
Warren B Grubb
Keyword(s):  
Staphylococcus Aureus ◽  
Electric Field ◽  
Homogeneous Electric Field

scholarly journals Experimental Study on Power Frequency Breakdown Characteristics of C4F7N/CO2 Gas Mixture Under Quasi-Homogeneous Electric Field

IEEE Access ◽  
2019 ◽  
Vol 7 ◽  
pp. 19100-19108 ◽  
Author(s):  
Xiaoxing Zhang ◽  
Qi Chen ◽  
Ji Zhang ◽  
Yi Li ◽  
Song Xiao ◽  
...  
Keyword(s):  
Experimental Study ◽  
Electric Field ◽  
Gas Mixture ◽  
Homogeneous Electric Field ◽  
Co2 Gas ◽  
Power Frequency

Ein Level-Crossing-Experiment im angeregten (5p1/2 5d5/2)J=2-Term des Sn I zur Untersuchung der Energieverschiebungen im elektrischen Feld / Level-Crossing Experiment in the Excited (5p1/25d5/2)J=2-State of the Sn I for the Investigation of the Energy Shifts in an Electric Field

1970 ◽  
Vol 25 (5) ◽  
pp. 608-611
Author(s):  
P. Zimmermann
Keyword(s):  
Magnetic Field ◽  
Electric Field ◽  
Stark Effect ◽  
Second Order ◽  
Wave Functions ◽  
Zero Field ◽  
Homogeneous Electric Field ◽  
Level Crossing ◽  
Crossing Experiment ◽  
The Magnetic Field

Observing the change of the Hanle effect under the influence of a homogeneous electric field E the Stark effect of the (5p1/25d5/2)j=2-state in Sn I was studied. Due to the tensorial part β Jz2E2 in the Hamiltonian of the second order Stark effect the signal of the zero field crossing (M ∓ 2, M′ = 0 β ≷ 0 ) is shifted to the magnetic field H with gJμBH=2 | β | E2. From these shifts for different electric field strengths the value of the Stark parameter|β| = 0.21(2) MHz/(kV/cm)2 · gJ/1.13was deduced. A theoretical value of ß using Coulomb wave functions is discussed.

On the Senftleben-Beenakker Electric Effect in Gaseous Ammonia

1971 ◽  
Vol 26 (6) ◽  
pp. 952-964 ◽  
Author(s):  
A.C. Levi ◽  
G.E. Tommei
Keyword(s):  
Electric Field ◽  
Field Dependence ◽  
Gaseous Ammonia ◽  
Homogeneous Electric Field ◽  
Distribution Matrix ◽  
Electric Effect ◽  
Low Pressures ◽  
Infinite Set

Abstract The viscosity of gaseous ammonia in the presence of a static homogeneous electric field is calculated using the Waldmann-Snider equation. Special attention is paid to the field dependence of the effect which is strongly influenced by molecular inversion. The latter causes a coupling of tensors of different rank in J in the expansion of the distribution matrix, thereby leading to an infinite set of equations which is solved numerically by a limiting procedure. The effect has a complicated dependence on pressure p and field E but to a good approximation turns out to depend on E/p a t pressures high with respect to an inversion pressure (about 5 atm for NH3, 300 torr for ND3) and, in agreement with the experiments, on E2/p at low pressures.

Sign in / Sign up

Export Citation Format

Share Document