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Hemispherical Deflection Analyzer (HDA)

_images/Hda-pe.jpg
_images/Hda3d.jpg

The Hemispherical Deflection Analyzer (HDA) consists of two concentric hemispherical electrodes held at different potentials. Charged particles of only a certain kinetic energy, called the pass energy, can pass through the electrodes at constant radius, so the system acts as a narrow band KE filter.

Cut-away of idealized HDA showing 1000 eV electron (red) and 900 and 1100 eV electrons (blue) flying through.

The HDA is an approximation of an idealized HDA, also called a spherical capacitor, consisting of two concentric spherical electrodes held at different potentials. The spherical capacitor has a simple analytic formulas for potential V and electric field E at radius r:

V(r) = -(k/r) + c E(r) = - \nabla V = -(k/r^2)

where

\begin{align*}
c & = (R_2 V(R_2) - R_1 V(R_1)) / (R_2 - R_1) k \\
  & = (V(R_2) - V(R_1)) * R_1 * R_2 / (R_2 - R_1)
\end{align*}

The pass energy w at R_0 is w = K(R_0) = q k / (2 R_0), for particle charge q.

Typical GEM files for ideal HDAs (spherical capacitors) are given below. Here, k = -200000, c = -2000, R0 = 100, K(R0) = 1000 eV, and V(R0) = 0. The inner and outer radii are R1 = 80 mm and R_2 = 120 mm.

Here is a typical 2D GEM file:

; sc2d.gem
pa_define(130,130,1,cylindrical,xy)
; outer electrode, R2
e(-333.3333) { fill { notin  { circle(0,0,119) } } }
; inner electrode, R1
e( 500.0000) { fill { within { circle(0,0,80) } } }

Here is a typical 3D GEM file:

; sc3d.gem
pa_define(130,130,130,planar,xyz)
; outer electrode, R2
e(-333.3333) { fill { notin  { sphere(0,0,0,119) } } }
; inner electrode, R1
e( 500.0000) { fill { within { sphere(0,0,0,80) } } }

Notice that the radius in the “notin” command is one grid unit less than R2 for improved accuracy.

Potential Energy (PE) surface of idealized HDA, showing 1000 eV electron (red) and 900 and 1100 eV electrons (blue) flying though.

See also

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