analysis of the energy gain measurements in tbts
DESCRIPTION
Analysis of the Energy Gain Measurements in TBTS. Oleksiy Kononenko 2 3/Mar/2011. Motivation. PRELIMINARY. New calibration + effective power increase. Javier Barranco. Energy Gain Measurements in TBTS. Analyzed acceleration measurements (events) in TBTS including the - PowerPoint PPT PresentationTRANSCRIPT
Analysis of the Energy Gain Measurements in TBTS
Oleksiy Kononenko23/Mar/2011
2
Motivation
PRELIMINARY
Javier Barranco
New calibration + effective power increase
3
Energy Gain Measurements in TBTSAnalyzed acceleration measurements (events) in TBTS including the corresponding timestamps are gathered by Javier Barranco Garcia here:
• http://elogbook.cern.ch/eLogbook/eLogbook.jsp?shiftId=1032364• http://elogbook.cern.ch/eLogbook/eLogbook.jsp?shiftId=1032385• http://elogbook.cern.ch/eLogbook/eLogbook.jsp?shiftId=1032677
Temperature, C Total Number of Events37 1750 655 560 11
4
One quarter of the TD24_tank (12WDSDVG1.8T) AS installed in TBTS
5
Results of the S-parameters HFSS Simulation
11.85 11.9 11.95 12 12.05
-40
-35
-30
-25
-20
-15
-10
-5
0
Frequency, GHz
dB
S11
S12
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Accelerating Voltage in TD24(Pin = 4W)
11.96 11.97 11.98 11.99 12 12.01 12.02 12.03 12.040
1000
2000
3000
4000
5000
6000
7000
Frequency,GHz
Vo
lta
ge
, V
abs(V+)
11.994 GHz
7
Layout of the Instrumentation for the CTF3 Two-beam Test-stand
Important input from Alexey Dubrovskiy: to use PPI0431 signal instead of the PSI0631 one and then take into account recirculation in PETS and waveguide network between PETS and AS. In this way more reliable input pulse is obtained for AS.
8
90 MW Pulse in CTF3 vs CLIC nominal (100 MV/m unloaded) pulse
0 50 100 150 200 250 300 3500
10
20
30
40
50
60
70
80
90
Time, ns
Po
we
r, M
W /
Ph
as
e,
de
g
CTF3,
CTF3, |P|CLIC nominal
9
Simulation of the Transmission
0 50 100 150 200 2500
5
10
15
20
25
30
35
Time, ns
Po
we
r, M
W
Simulation
Measurement
Ptrans(t) = conv (S12(t), sqrt(|P(t)|) * exp (i*(ω0*t+Δφ)) )
10
Simulation of the Energy Gain (no detuning)
0 10 20 30 40 50 60 70 80 90 1000
5
10
15
20
25
30
35
Peak Power, MWt
En
erg
y G
ain
, M
eV
CTF3, t=37CSimulation, f=0MHzSteady-state, f=0MHzCTF3, t=50CSimulation, f=0MHzCTF3, t=55CSimulation, f=0MHzCTF3, t=60CSimulation, f=0MHzSteady-state, f=0MHz
Vacc(t) = conv (RV(t), sqrt(|P(t)|) * exp (i*(ω0*t+Δφ(t))) )
11
Simulation of the Energy
0 10 20 30 40 50 60 70 80 90 1000
5
10
15
20
25
30
35
Peak Power, MWt
En
erg
y G
ain
, M
eV
CTF3, t=37CSimulation, f=9MHzSteady-state, f=9MHzCTF3, t=50CSimulation, f=6MHzSteady-state, f=6MHzCTF3, t=55CSimulation, f=5MHzSteady-state, f=5MHzCTF3, t=60CSimulation, f=4MHzSteady-state, f=4MHzSteady-state, f=0MHz
Vacc detuned (f) := Vacc (f - Δf), assuming that Δf=+10MHz at 30C and Δf = -1MHz/5C
12
Effect of the detuning in the comparison with the steady-state
0 50 100 150 200 250 300 350 400 4500
0.5
1
1.5
2
2.5
3
3.5x 10
7
Time, ns
Vo
lta
ge
, V
CTF3, df=0Steady-state, df=0CTF3, df=9MHzSteady-state, df=9MHz
Steady-state, df=9MHzCTF3, df=9MHz
13
Pulse-Surface Heating for 90MW CTF3 pulse vs CLIC nominal pulse
0 100 200 300 400 500 600 7000
5
10
15
20
25
30
35
40
45
Time, ns
T
, K
CLIC nominal, TCTF3, T
ΔT(t) = α * conv (1/sqrt(t), |P(t)|), normalization: ΔT (100ns, 100MV/m) = 28K
14
Conclusions
• Introducing detuning we’ve got rather good correlation between the simulations and measurements of the acceleration
• Pulse shape effect can also be clearly seen now, even though there is an interesting detuning effect
• There are still some calibration errors in the TBTS instrumentation
• Pulse-surface heating was comparable with the one for the CLIC nominal pulse