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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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Transport <strong>of</strong> 6-dim 6<br />

σ Matrix<br />

Consider <strong>the</strong> 6-dim. ray vec<strong>to</strong>r in TRANSPORT: X = (x, Θ, y, Φ, l, dp/p)<br />

Ray X 0 from location 0 is transported by a 6 x 6 Matrix R <strong>to</strong> location 1 by: X 1 = RX 0<br />

(7)<br />

Note: R maybe a matrix representing a complex system (3) is : R = R n R n-1 …R 0<br />

Ellipsoid in Matrix notation (6), generized <strong>to</strong> e.g. 6-dim. using σ Matrix: X 0<br />

T<br />

σ 0<br />

−1<br />

X 0 = 1<br />

Inserting Unity Matrix I = RR -1 in equ. (6) it follows X 0<br />

T<br />

(R T R T-1 ) σ 0<br />

−1<br />

(R -1 R) X 0 = 1<br />

from which we derive (RX 0 ) T (Rσ 0 R T ) -1 (RX 0 ) = 1<br />

(6)<br />

(8)<br />

The equation <strong>of</strong> <strong>the</strong> new ellipsoid after transformation becomes X 1<br />

T<br />

σ 1<br />

−1<br />

X 1 = 1<br />

(9)<br />

where σ 1 = Rσ 0 R T (10)<br />

Conclusion: Knowing <strong>the</strong> TRANSPORT matrix R that transports one<br />

ray through an ion-optical system using (7) we can now also transport<br />

<strong>the</strong> phase space ellipse describing <strong>the</strong> initial beam using (10)

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