An Introduction to the Ion-Optics of Magnet Spectrometers
An Introduction to the Ion-Optics of Magnet Spectrometers
An Introduction to the Ion-Optics of Magnet Spectrometers
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
The 2-dimensional 2<br />
case ( x, Θ )<br />
Ellipse Area = π(det σ) 1/2<br />
Emittance ε = (det σ) 1/2 is constant<br />
for fixed energy & conservative<br />
forces (Liouville’s Theorem)<br />
Note: ε shrinks (increases) with<br />
acceleration (deceleration);<br />
Dissipative forces: ε increases in<br />
gases; electron, s<strong>to</strong>chastic, laser<br />
cooling<br />
σ = ⎛σ 11 σ 21 ⎫<br />
⎝σ 21 σ 22 ⎭<br />
σ −1 = 1/ε 2 ⎛σ 22 −σ 21 ⎫<br />
⎝−σ 21 σ 11 ⎭<br />
Exercise 1:<br />
Show that:<br />
2 dimensional cut x-Θ is shown<br />
Real, pos. definite<br />
symmetric σ Matrix<br />
σσ −1 = ⎛1 0 ⎫<br />
⎝ 0 1⎭<br />
Inverse Matrix<br />
= I (Unity Matrix)<br />
2-dim. Coord. vec<strong>to</strong>rs<br />
(point in phase space)<br />
X =<br />
⎛x ⎫<br />
X T = (x Θ)<br />
⎝Θ⎭<br />
Ellipse in Matrix notation:<br />
X T σ −1 X = 1<br />
(6)<br />
Exercise 2: Show that Matrix notation<br />
is equivalent <strong>to</strong> known Ellipse equation:<br />
σ 22 x 2 −2σ 21 x Θ + σ 11 Θ 2 = ε 2