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Solution
ID: past-exam-of-the-short-options-paper-shared-by-prelims-and-parts-a-and-b-of-the-physics-course-of-the-university-of-oxford/2012/s19/1/c/solution
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Past exam of the short options paper shared by Prelims and Parts A and B of the physics course of the University of Oxford
/
2012
/
S19
/
1
/
c
/
Solution
by
Codex
0
2026-10-25
For
a
real
determinant
-one
map
, bounded generic repeated
transport
requires
eigenvalues
e
±
i
μ
, equivalently
∣
tr
M
∣
<
2
. Here both
planes
have
tr
M
=
2
−
L
1
L
2
/
f
2
, so
0
<
f
2
L
1
L
2
<
4
,
cos
μ
=
1
−
2
f
2
L
1
L
2
.
(1)
For positive drift
lengths
and
f
>
0
, this
means
f
>
L
1
L
2
/2
. The equalities are marginal and generally produce
a
Jordan-block
growth rather than stable
motion
. Moving the
reference
point changes the
map
by
a
similarity transformation
,
M
→
PM
P
−
1
, so the
eigenvalues
and full-
cell
phase advance are unchanged.
Write the
stable map
using the
Courant-Snyder parameters
, also called Twiss
parameters
:
M
=
(
cos
μ
+
α
sin
μ
−
γ
T
sin
μ
β
sin
μ
cos
μ
−
α
sin
μ
)
,
β
γ
T
−
α
2
=
1.
(2)
At the chosen
reference
point
β
=
M
12
/
sin
μ
,
α
=
(
M
11
−
M
22
)
/
(
2
sin
μ
)
, and
γ
T
=
−
M
21
/
sin
μ
. Repeated traversal gives
M
n
=
(
cos
n
μ
+
α
sin
n
μ
−
γ
T
sin
n
μ
β
sin
n
μ
cos
n
μ
−
α
sin
n
μ
)
.
(3)
If the full
ring
contains
N
c
identical
cells
, its one-turn phase is
N
c
μ
modulo
2
π
;
n
ring
turns use
n
N
c
μ
. The displayed
M
n
is for
n
repetitions of the specified
cell
.
Figure 1.
Stability and phase advance of the equal-strength
quadrupole
cell
. Both transverse
planes
have trace
2
minus
L
_
1
L
_
2
/
f
squared. The
strict
stable interval excludes the two marginal boundaries.
Details
.
Total
articles
:
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