Difference: RobAinsworthHOMInteraction (1 vs. 4)

Revision 406 Jun 2012 - TomCraneAdmin

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META TOPICPARENT	name="RobAinsworthStudies"

Monopole Mode Excitation

Line: 47 to 47

dU_n = q(\Re(V_n)\cos(\omega_n dt) - \Im(V_n)\sin(\omega_n dt)) - \frac{1}{2}\Delta V_{q,n} %ENDLATEX%

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META TOPICMOVED	by="RobAinsworth" date="1329310256" from="Public.RobAinsworthHOMDynamicsStudies" to="Public.RobAinsworthHOMInteraction"

Revision 316 Apr 2012 - webmanip_5foldt2nt_2esh

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META TOPICMOVED	by="RobertAinsworth" date="1329310256" from="Public.RobAinsworthHOMDynamicsStudies" to="Public.RobAinsworthHOMInteraction"

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META TOPICMOVED	by="RobAinsworth" date="1329310256" from="Public.RobAinsworthHOMDynamicsStudies" to="Public.RobAinsworthHOMInteraction"

Revision 216 Feb 2012 - TomCrane1

Line: 1 to 1

META TOPICPARENT	name="RobAinsworthStudies"

Monopole Mode Excitation

Line: 47 to 47

dU_n = q(\Re(V_n)\cos(\omega_n dt) - \Im(V_n)\sin(\omega_n dt)) - \frac{1}{2}\Delta V_{q,n} %ENDLATEX%

Added:

>
>

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META TOPICMOVED	by="RobertAinsworth" date="1329310256" from="Public.RobAinsworthHOMDynamicsStudies" to="Public.RobAinsworthHOMInteraction"

Revision 116 Feb 2012 - TomCrane1

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Added:

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META TOPICPARENT	name="RobAinsworthStudies"

Monopole Mode Excitation

The voltage induced by a point-charge, , according to the fundamental theorem of beam loading given by

$\Delta V_{q,n} = - q \frac{\omega_n}{2}(R/Q)_n (\beta)$

(1)

where $\omega_n$ is the angular frequency of mode, $n$ , $\beta$ is the velocity of the particle as a fraction of the speed of light and $(R/Q)_n (\beta)$ is given by

$(R/Q)_n (\beta) = \frac{\left| \int_{-\infty}^{\infty}E_{z,n}(r=0,z)e^{i\omega_n \frac{z}{\beta c}}dz\right|^2}{\omega_n U_n}$

(2)

where $U_n$ is the stored energy in the mode and $E_{z,n}(r = 0,z)$ the electric field along the beam axis. Due to losses, the amplitude of the voltage will decay according to

$V_n(t) = \Delta V_{q,n}e^{-t/T_{d,n}}e^{i\omega_n t}$

(3)

where $T_{d,n} = 2Q_{L,n}/\omega_n$ is the voltage decay time constant with $Q_{L,n}$ as the loaded quality factor of the complete system and is the inverse sum of all the subsystems

$\; \frac{1}{Q_L} = \frac{1}{Q_{ex}} + \frac{1}{Q_0}.$

(4)

For a superconducting cavity, the natural $Q_0$ is of the order of $10^{10}$ meaning that that $Q_L$ is dominated by $Q_{ex}$ and so the approximation that $Q_L \approx Q_{ex}$ is made.

In pulsed operation the voltage after one pulse with bunches and no HOM voltage present before the arrival of the first bunch, is given by

$V_{p,n} = \Delta V_{q,n} \sum^N_{k=1} e^{-kT_b/T_{d,n}+ik\omega_nT_b} = \Delta V_{q,n} \frac{1-e^{-NT_b/T_{d,n}+iN\omega_nT_b}}{1-e^{-T_b/T_{d,n}+i\omega_nT_b}}$

(5)

where $T_b$ is the time between bunches. After $m$ pulses with pulse period $T_p$ , the voltage present in the cavity is given by:

$V^m_{p,n} = \Delta V_{q,n} \frac{1-e^{-NT_b/T_{d,n}+iN\omega_nT_b}}{1-e^{-T_b/T_{d,n}+i\omega_nT_b}} \frac{1-e^{-mT_p/T_{d,n}+im\omega_nT_p}}{1-e^{-T_p/T_{d,n}+i\omega_nT_p}}$

(6)

Monopole Mode Interaction

$dU_n = q(\Re(V_n)\cos(\omega_n dt) - \Im(V_n)\sin(\omega_n dt)) - \frac{1}{2}\Delta V_{q,n}$

(7)

|*META TOPICMOVED*|by="RobertAinsworth" date="1329310256" from="Public.RobAinsworthHOMDynamicsStudies" to="Public.RobAinsworthHOMInteraction"|
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