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PA
Collective Effects
mbtrack2
Commits
ed09e1a1
Commit
ed09e1a1
authored
11 months ago
by
Keon Hee KIM
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Add a reference for the fundamental theorem of beam loading
parent
c2c66db6
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master
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Faster CircularResistiveWall
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mbtrack2/impedance/resistive_wall.py
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14 additions, 8 deletions
mbtrack2/impedance/resistive_wall.py
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mbtrack2/impedance/resistive_wall.py
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ed09e1a1
...
...
@@ -45,7 +45,8 @@ class CircularResistiveWall(WakeField):
Resistive wall WakeField element for a circular beam pipe.
Impedance from approximated formulas from Eq. (2.77) of Chao book [1].
Wake function formulas from [2, 3].
Wake function formulas from [2, 3] and the fundamental theorem of
beam loading from [4].
Parameters
----------
...
...
@@ -67,7 +68,7 @@ class CircularResistiveWall(WakeField):
----------
[1] : Chao, A. W. (1993). Physics of collective beam instabilities in high
energy accelerators. Wiley.
[2] : Ivanyan, Mikayel I. and
Tsakanov, Vasili M
.
"
Analytical treatment of
[2] : Ivanyan, Mikayel I.
,
and
Vasili M. Tsakanov
.
"
Analytical treatment of
resistive wake potentials in round pipes.
"
Nuclear Instruments and Methods
in Physics Research Section A: Accelerators, Spectrometers, Detectors and
Associated Equipment 522, no. 3 (2004): 223-229.
...
...
@@ -75,6 +76,9 @@ class CircularResistiveWall(WakeField):
interbunch collective beam motions in storage rings.
"
Nuclear Instruments
and Methods in Physics Research Section A: Accelerators, Spectrometers,
Detectors and Associated Equipment 806 (2016): 221-230.
[4] : Zotter, Bruno W., and Semyon A. Kheifets (1998). Impedances and wakes
in high-energy particle accelerators. World Scientific.
"""
...
...
@@ -129,9 +133,9 @@ class CircularResistiveWall(WakeField):
The approxmiated expression is valid if the time is large compared
to the characteristic time t0.
Eq. (11) in [1] is completely
equivalent
to Eq. (22) in [2].
Eq. (11) in [1] is completely
identical
to Eq. (22) in [2].
The fundamental theorem
of beam loading is applied for the exact
The fundamental theorem of beam loading
[3]
is applied for the exact
expression of the longitudinal wake function: Wl(0) = Wl(0+)/2.
Parameters
...
...
@@ -148,7 +152,7 @@ class CircularResistiveWall(WakeField):
References
----------
[1] : Ivanyan, Mikayel I. and
Tsakanov, Vasili M
.
"
Analytical treatment of
[1] : Ivanyan, Mikayel I.
,
and
Vasili M. Tsakanov
.
"
Analytical treatment of
resistive wake potentials in round pipes.
"
Nuclear Instruments and Methods
in Physics Research Section A: Accelerators, Spectrometers, Detectors and
Associated Equipment 522, no. 3 (2004): 223-229.
...
...
@@ -156,6 +160,8 @@ class CircularResistiveWall(WakeField):
interbunch collective beam motions in storage rings.
"
Nuclear Instruments
and Methods in Physics Research Section A: Accelerators, Spectrometers,
Detectors and Associated Equipment 806 (2016): 221-230.
[3] : Zotter, Bruno W., and Semyon A. Kheifets (1998). Impedances and wakes
in high-energy particle accelerators. World Scientific.
"""
wl
=
np
.
zeros_like
(
time
)
idx1
=
time
<
0
...
...
@@ -179,7 +185,7 @@ class CircularResistiveWall(WakeField):
The approxmiated expression is valid if the time is large compared
to the characteristic time t0.
Eq. (11) in [1] is completely
equivalent
to Eq. (25) in [2].
Eq. (11) in [1] is completely
identical
to Eq. (25) in [2].
Corrected the typos in the last two terms in exact expression
(Eq. (11), of [1]).
...
...
@@ -193,11 +199,11 @@ class CircularResistiveWall(WakeField):
Returns
-------
wt : array of float
Transverse wake function in [V/C].
Transverse wake function in [V/C
/m
].
References
----------
[1] : Ivanyan, Mikayel I. and
Tsakanov, Vasili M
.
"
Analytical treatment of
[1] : Ivanyan, Mikayel I.
,
and
Vasili M. Tsakanov
.
"
Analytical treatment of
resistive wake potentials in round pipes.
"
Nuclear Instruments and Methods
in Physics Research Section A: Accelerators, Spectrometers, Detectors and
Associated Equipment 522, no. 3 (2004): 223-229.
...
...
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