results with a cvd diamond at the k2k beam-line
DESCRIPTION
Results with a CVD diamond at the K2K beam-line. RD42 collaboration meeting May 14 th 2004. Contents 1.Introduction 2.Set up 3.Results 4.Summary. Jun Kubota(Kyoto Univ.). Japan. Member. Kyoto Univ. J.Kubota, K.Nishikawa, T.Nakaya, M.Yokoyama. KEK. J.Kameda(now, ICRR). Canada. - PowerPoint PPT PresentationTRANSCRIPT
May 14th 2004 RD42 collaboration meeting 1
Results with a CVD diamond at Results with a CVD diamond at the K2K beam-linethe K2K beam-line
Jun Kubota(Kyoto Univ.)
RD42 collaboration meetingMay 14th 2004
ContentsContents1.Introduction1.Introduction2.Set up2.Set up3.Results3.Results4.Summary4.Summary
May 14th 2004 RD42 collaboration meeting 2
Kyoto Univ.
J.Kubota, K.Nishikawa, T.Nakaya, M.Yokoyama
J.Kameda(now, ICRR)
KEK
TRIUMF
Toronto Univ.
Japan
Canada
P.Kitching, A.Konaka
J.F.Martin, W.Trischuk(RD42)
Member
May 14th 2004 RD42 collaboration meeting 3
1.Introduction1.1 J-PARC neutrino oscillation experiment(T2K)
~1GeV beam
J-PARC50GeV PS
Super-K: 22.5 kt
Plan to start in 2009
Discovery of oscillationPrecision measurement of oscillation parameter
eμ νν
μμ νν
May 14th 2004 RD42 collaboration meeting 4
In a long baseline neutrino oscillation experiment,it’s necessary to monitor the direction, the profile andthe intensity of the neutrino beam.
1.2 motivation
The neutrino beam can be monitored on spill-by-spill basison spill-by-spill basisby measuring the secondary muons coming from pion decay
A muon monitor is needed
(In K2K, silicon pad detectors and ion chamber are usedas muon monitors)
protonTarget
May 14th 2004 RD42 collaboration meeting 5
1.2 motivation(cont.)
In T2K long baseline neutrino oscillation experiment,the muon beam intensity is expected to be 1000 times more than K2K
/yearμ/cm10 211 /yearμ/cm10 214In K2K, about In T2K, about
Radiation hardnessRadiation hardness for silicon detectorswill become a problem
Test whether a diamond detector is useful as a muon monitor- A diamond detector is installed to K2K muon monitor
May 14th 2004 RD42 collaboration meeting 6
1.3 diamond detector
•Developed by RD42
•2 diamonds bought from Ohio State
Univ.-One packaged at Toronto, sent to KEK
-Second one still at Toronto
•Characteristic-Size 0.95cm 0.95cm
-Thickness 500
μm
Capacitance 9.1pF(as capacitor)
May 14th 2004 RD42 collaboration meeting 7
2 Set up2.1 The position of the diamond detector
K2K neutrino beam line
200 m
silicon detectors ion chamber
3.5m
Beam dumpTarget
p
12GeVPS
K2K muon monitor
Muon intensity @ beam center ; ~Beam has 9 bunches for 1.1 , every 2.2sec
24μ/spill/cm10μsec
May 14th 2004 RD42 collaboration meeting 8
2.1 The position of the diamond detector(cont.)
35cm
Beam center
diamond detectorsilicon detectorsion chamber
silicon detectors
We install the diamond detectoraround the beam center
The signal from the silicon detector is used as a referenceWe don’t know the absolute muon flux
Inside of K2K muon monitor
May 14th 2004 RD42 collaboration meeting 9
HV supply
Diamond detector 9.1pF
capacitor 2200pF(to keep bias voltage)
about 20m
50 resistance
read out
w/o Amp
Time constant…about 0.46nsecOperate at the bias voltage of 650V
2.2 Circuit
May 14th 2004 RD42 collaboration meeting 10
Beam spill has 9bunches for 1.1μsec
3mV
1.1micro-sec
2.3 Raw signal from the diamond detector
9 bunches are clearly observed, but,signal also has overshoot
overshoot
May 14th 2004 RD42 collaboration meeting 11
3.Results
The relation of the collected charge v.s the electric fieldThe charge collection distancePhysical value defined by RD42
Measured item
May 14th 2004 RD42 collaboration meeting 12
0.2
Electric field(V/ m)μ
1.0V/ mμ
1.0 1.2 1.40 0.4 0.6 0.8
0.02
0.05
0.070.06
0.04
0.01
0.03
0
3.1 The relation of the collected charge v.s the electric field
diam
ond/
sili
con
Above 1.0V/
almost flatμm
In RD42 measurement(NIM.A514(2003)79),reach plateau
1.0V/μ m
consistentconsistent
May 14th 2004 RD42 collaboration meeting 13
Beam center
3.2 The charge collection distance
13.8pC(56.69ADC count)silicon detector160pC(656.1ADC count)average of two silicon detectors
measured ratio(diamond/silicon) 13.8pC/160pC… 8.6%
pedestal signal
@ m(650V)Measurement of the collected chargeMeasurement of the collected charge 1.3V/μ
May 14th 2004 RD42 collaboration meeting 14
3.2 The charge collection distance(cont.)
Thickness of depletion layerAssumption… the collection efficiency;100%
The charge collection distance( )μm
The charge collection distance116.5 μm Possibly underestimate (>20%)
due to overshoot(shown by signal photograph)
measuredratio
μmsilicon
diamond
22000e/300
36e/2
22
2cm
cm(0.95)
300
μm μm
8.6%
Ratio(diamond/silicon)Ratio(diamond/silicon)Generated charge for a mip
Size
May 14th 2004 RD42 collaboration meeting 15
SummaryWith a diamond detector, the signal of muon flux( ) was observed at K2K muon monitor
The relation of the collected charge v.s the electric fieldabove 1.0V/ , almost flatThe charge collection distance116.5 …possibly underestimate (>20%) due to overshoot (shown by signal photograph)-agree with the expectation(typical collection distance should be around 120 )
24μ/spill/cm10
μm
In T2K, we can conclude a diamond detector is usefula diamond detector is usefulas a muon monitoras a muon monitor
μm
μm