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An Introduction to the Ion-Optics of Magnet Spectrometers

An Introduction to the Ion-Optics of Magnet Spectrometers

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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

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