TY - GEN
T1 - Opimization of electrostatic phase plate for biological specimens in transmission electron microscopy
AU - Li, Wen Ping
AU - Han, Li
PY - 2010
Y1 - 2010
N2 - The inner and outer diameter of electrostatic phase plate di, dm and do limit the number of electrons passing through and then affect the high-resolution information in the phase contrast image. The current density contours at the upper surface of the phase plate is first used to determine di, dm and do. The current density contours and trajectory of un-scattered electrons under a real objective lens model were simulated by traditional aberration integrated method. The current density contours of scattered electrons were obtained by solving the Newton-Lorentz equation of motion. In building the motion equation in a practical field, second order finite element method and Hermite function interpolation are applied to get the axial field and its arbitrary order. The motion equations were solved by fifth-order Runge-Kutta algorithm and the performance of scattered electrons was given for a 200kV TEM. From our simulation, di should be larger than 6.4nm, dm should be possible enough to be fabricated and do be larger than 32 μ m.
AB - The inner and outer diameter of electrostatic phase plate di, dm and do limit the number of electrons passing through and then affect the high-resolution information in the phase contrast image. The current density contours at the upper surface of the phase plate is first used to determine di, dm and do. The current density contours and trajectory of un-scattered electrons under a real objective lens model were simulated by traditional aberration integrated method. The current density contours of scattered electrons were obtained by solving the Newton-Lorentz equation of motion. In building the motion equation in a practical field, second order finite element method and Hermite function interpolation are applied to get the axial field and its arbitrary order. The motion equations were solved by fifth-order Runge-Kutta algorithm and the performance of scattered electrons was given for a 200kV TEM. From our simulation, di should be larger than 6.4nm, dm should be possible enough to be fabricated and do be larger than 32 μ m.
KW - Current density contours
KW - Electron trajectory
KW - Hermite function interpolation
KW - Phase plate
UR - https://www.scopus.com/pages/publications/77953304296
U2 - 10.1109/ICBECS.2010.5462475
DO - 10.1109/ICBECS.2010.5462475
M3 - 会议稿件
AN - SCOPUS:77953304296
SN - 9781424453153
T3 - 2010 International Conference on Biomedical Engineering and Computer Science, ICBECS 2010
BT - 2010 International Conference on Biomedical Engineering and Computer Science, ICBECS 2010
T2 - 2010 International Conference on Biomedical Engineering and Computer Science, ICBECS 2010
Y2 - 23 April 2010 through 25 April 2010
ER -