Status of Hybrid target R&D at KEK-LINAC T.Takahashi Hiroshima University March 2011 ALPG11 Eugene...
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Transcript of Status of Hybrid target R&D at KEK-LINAC T.Takahashi Hiroshima University March 2011 ALPG11 Eugene...
Status of Hybrid target R&D at KEK-LINAC
T.TakahashiHiroshima University
March 2011ALPG11 Eugene
Collaborators:V. Strakhovenko O. Dadoun, R. Chehab, A.Variola, L. Rinolfi, O. Dadoun,T.Kamitani, T.Suwada, T.Omori, J.Urakawa,K.Furukawa, K.Umemori,M.Satoh,T.Sugimura,S.Kawada, T.Akagi, Y. Uesugi
Hybrid target for positron source
• Chehab, Variola, Strakhovenko Scheme for LC positron sources
Experimental study for further development
e-e+, e-, g g
e-
e+
experimental site KEKB LINAC
Switch yard
8 GeV e-~ nc/bunchupto 25Hz single bunch
Setup
8GeV e- 1mm W crystal
Sweeping Magnet0.96T 0.75m
amorphous W8 mm18 mm
Analyzing magnet5 ~ 30MeV
pictures
e- 8GeV
W Crystal on the goniometer
Sweeping magnet
pictures
movable stage
amorphoustargets
thermocoupolesattached back end
The data• Hybrid
• Conventional
e 8GeV sweep mag
1mm W Crystal on axis (aligned to the beam) off axis (not aligned to the beam)
e 8GeV
amorphous W 1.75, 3.5, 5.25, 8, 18mm
temperatureat the end of the targets by thermocouplesand infrared camera
positrons fromthe targetmomentumanalyzed
g
posit
ron
yiel
d (a
rb. u
nit)
angle of crystal w.r.t. beam (mr)
rot. in vertical plain
esweep mag
8 mm
Rocking curve
1
2
3.4 0.117.7 0.4
1 2
2 22 21 2
( )f A B Const
same for horizontal rotation
Preliminary
factor 3 enhancement
it was 1.2 in 2009 Sep datawe found the detector was saturated in previous exp.
e+ yield
amorphous thickness [mm]
e+ d
etec
ted
[a.u
]P=20MeV
simulation and data normalized at 8mmneed to correct acceptance for precise analysis
0 2 4 6 8 10 12 14 16 180
5
10
15
ConventionalSimulationHybrid ON axisSimulationHybrid OFF axis
Temperature measurement w/ thermocouples
back plane of amorphous target thermocouple
approximately 1mm x 1mm
to fast data loggerread temperature each 10ms
bunch by bunch temperature variationPEDD information by thermocouple
temperature at equilibriumtotal energy deposit
Example ofTemperature Measurement
0 2 4 6 8 10 12 14 16 18 20 22 24 26 28 30202530354045505560
Temperature of the 8mm amorphous target for the hybrid case
Time from Beam On (Minutes)
Tem
pera
ture
(deg
ree
Celsi
us)
Base temp. 23.3℃
DT~32℃
Preliminary
T vs total energy deposit
hybrid on axis
conventional
18mm
8mm
T at equilibrium has information for total energy deposit except for 18mm hybrid
target is thicker than shower max
hybrid off axis
T at
equ
ilibr
ium
(deg
)
bunch by bunch temperature rise
• bunch repetition 1Hz
combine all bunches to for statistics
~ 60 pulses for one data set
time , base T. adjustment
1sec
0 1 0 2( )/ ( )/0( ) (1 )sin(2 ( ))
t t t tT t T ae eb f t
Beam profile on amorphous
sx=2.0mmsy=2.3 mm
beam profilescrystal amorphous
3.2m
sx=2.0mmsy=2.3 mm
sx=0.42mmsy=1.54mm
beam divergencex~ 0.5mry~ 0.24mr PEDD estimation
bunch by bunch temp.• dT provides a measure of PEDD
hybrid on axis
conventional
hybrid off axis
Simulation
Measured
summary• we took systematic data for hybrid target R&D
– yield from various target thickness– momentum 5, 10, 20 MeV– energy deposit/temperature
• at equilibrium • single bunch variation• beam profile
• Correction for detector acceptance – hopefully next a couple of months
Evaluation of the hybrid scheme as a positron source
Data analysis Done
supplements
momentum dependence
e+ momentum[MeV]
e+ d
etec
ted
[a.u
.] hybrid on axis conventional
0 5 10 15 200
5
10
0 5 10 15 200
5
10
18mm
8mm
5.25mm
3.5mm
1.75mm
Beam profile on the cryltal
sx=0.42mmsy=1.54mm
adjust time and base line
Time
Tem
p
Time
Tem
p.
variation base temp. for 1 min.
clock difference
just overlay 50 pulses
Channeling Radiation e-
Crystals: converter from high energy electrons to low energy photons
photon energy (MeV)
#g crystal#g amorphous
relative intensity of phtons fromcrystal and amorphous tungsten
KEKB LINAC• KEKB LINAC
• E(beam) : 8GeV Bunch Charge: ~nC
• Ideal for R&D for hybrid target
Experiences with crystal targets for KEKB