Yudai Ichikawa (Kyoto University/JAEA) 2013/07/26 RCNP 研究究会 「核子・ハイペロン多体系におけるクラスター現象」
卒業研究発表 『J-PARCでのハイペロン陽子散乱実...
Transcript of 卒業研究発表 『J-PARCでのハイペロン陽子散乱実...
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“ Development of a cylindrical tracking detectorwith multichannel
scintillation fibers and PPD readout ”
7th International Conference on New Developments In Photodetection
Yuya AkazawaTohoku University
for the J-PARC E40 collaboration
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2
Contents Motivation for development
– Requirements Construction of Cylindrical Fiber Tracker
– Fiber construction– PPD Read-out
Performance evaluation
– Response for cosmic ray and proton
– Linearity
– Energy resolution
Summary
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Liquid H2 target
BGO calorimeter
CFT
Σp scattering experimentΣp scattering experiment @J-PARC , Japan ⇒⇒ ΣN interactionMeasurement of dσ/dΩ of Σp scattering with high statistics
※ It is difficult to use Σ as a target or a beam ∵ lifetime (~10-10s) ⇒ need to produce Σ in a target
event identification by reconstructing kinematics
from θ and Ep'
of scattered protons
dEで粒子識別します
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π±
beam
K+
S±
①Production
Liquid H2 target
BGO calorimeter
CFT
①Production π± + p → Σ± + K+
Σp scattering experimentΣp scattering experiment @J-PARC , Japan ⇒⇒ ΣN interactionMeasurement of dσ/dΩ of Σp scattering with high statistics
※ It is difficult to use Σ as a target or a beam ∵ lifetime (~10-10s) ⇒ need to produce Σ in a target
event identification by reconstructing kinematics
from θ and Ep'
of scattered protons
p
dEで粒子識別します
NDIP2014 poster Honda Ryotaro
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π±
beam
K+
S±
①Production
②ScatteringLiquid H
2 target
BGO calorimeter
CFTCylindrical Fiber Tracker(CFT) ・ Trajectory ・ Energy deposit PID⇒
BGO calorimeter・Kinetic Energy
S±'①Production π± + p → Σ± + K+
②Scattering Σ± + p → Σ±' + p'
Σp scattering experimentΣp scattering experiment @J-PARC , Japan ⇒⇒ ΣN interactionMeasurement of dσ/dΩ of Σp scattering with high statistics
※ It is difficult to use Σ as a target or a beam ∵ lifetime (~10-10s) ⇒ need to produce Σ in a target
event identification by reconstructing kinematics
from θ and Ep'
p'of scattered protons
p
dEで粒子識別します
NDIP2014 poster Honda Ryotaro
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π±
beam
K+
S±
①Production
②ScatteringLiquid H
2 target
BGO calorimeter
CFTCylindrical Fiber Tracker(CFT) ・ Trajectory ・ Energy deposit PID⇒
BGO calorimeter・Kinetic Energy
S±'①Production π± + p → Σ± + K+
②Scattering Σ± + p → Σ±' + p'
Σp scattering experimentΣp scattering experiment @J-PARC , Japan ⇒⇒ ΣN interactionMeasurement of dσ/dΩ of Σp scattering with high statistics
※ It is difficult to use Σ as a target or a beam ∵ lifetime (~10-10s) ⇒ need to produce Σ in a target
event identification by reconstructing kinematics
from θ and Ep'
n
p±p'of scattered protons
p
dEで粒子識別します
NDIP2014 poster Honda Ryotaro
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Liquid H2 target
BGO calorimeter
CFTCylindrical Fiber Tracker(CFT) ・ Trajectory ・ Energy deposit PID⇒
BGO calorimeter・Kinetic Energy
①Production π± + p → Σ± + K+
②Scattering Σ± + p → Σ±' + p'
Σp scattering experimentΣp scattering experiment @J-PARC , Japan ⇒⇒ ΣN interactionMeasurement of dσ/dΩ of Σp scattering with high statistics
※ It is difficult to use Σ as a target or a beam ∵ lifetime (~10-10s) ⇒ need to produce Σ in a target
event identification by reconstructing kinematics
from θ and Ep'
of scattered protons
dEで粒子識別します
π Beam
K+
S'n
pp'
S
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Liquid H2 target
BGO calorimeter
CFTCylindrical Fiber Tracker(CFT) ・ Trajectory ・ Energy deposit PID⇒
BGO calorimeter・Kinetic Energy
①Production π± + p → Σ± + K+
②Scattering Σ± + p → Σ±' + p'
Σp scattering experimentΣp scattering experiment @J-PARC , Japan ⇒⇒ ΣN interactionMeasurement of dσ/dΩ of Σp scattering with high statistics
※ It is difficult to use Σ as a target or a beam ∵ lifetime (~10-10s) ⇒ need to produce Σ in a target
event identification by reconstructing kinematics
from θ and Ep'
Measurement of energy deposit by CFTwith combination of scintillation fibers & MPPCs
of scattered protons
Main topic ~development of CFT~
dEで粒子識別します
π Beam
K+
S'n
pp'
S
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Requirements– Energy resolution
• 35% for 70MeV proton for 1 layer
– Angular resolution : σθ=0.77deg
– Surround the target• Cylindrical shape• Long active region ・・・ 400mm
– 2 types of fiber configurations ⇒⇒ Track finding 3 dimensionally
• Φ layers ( straight layer )• UV layers ( spiral layer )
ビーム軸をz軸と定義
get z position using “Φ”
Φ layer measure “Φ”
U・V layer
Cylindrical Fiber Tracker (CFT)
• Acceptance for scattering events
Energy deposit depends on the MMassass↓↓
Resolve proton and π
300mm
400mm
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Requirements– Energy resolution
• 35% for 70MeV proton for 1 layer
– Angular resolution : σθ=0.77deg
– Surround the target• Cylindrical shape• Long active region ・・・ 400mm
– 2 types of fiber configurations ⇒⇒ Track finding 3 dimensionally
• Φ layers ( straight layer )• UV layers ( spiral layer )
ビーム軸をz軸と定義
get z position using “Φ”
Φ layer measure “Φ”
U・V layer
Cylindrical Fiber Tracker (CFT)
• Acceptance for scattering events
Energy deposit depends on the MMassass↓↓
Resolve proton and π
・ Fiber construction➢ Special fiber configuration
・ Many channel operation ➢ Photon readout fiber by fiber
Prototype
Some challenges to overcomeSome challenges to overcome for development of CFTfor development of CFT
300mm
400mm
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CFT prototype
MPPC – S10362-11-050P HPK– MPPC size : 1×1mm2
– Pixel size : 50×50μm2 – 400 pixels/MPPC
r = 60
Scintillation Fiber – Kuraray SCSF-78M– Diameter:0.75mm
– MPPCs are operated and read-out by EASIROC boards
EASIROC boardsMPPCs are operated and read-out by
➢ 3layers2 straight layers + 1 spiral layer
➢ 1,100 fibers➢ Read fiber by fiber
400mmReadout frame
Reflector – ESR
EASIROC board – Specialized for
multi-MPPC readout – ADC, TDC
Read & operate
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12
Contents Motivation for development
– Requirements Construction of Cylindrical Fiber Tracker
– Fiber construction– PPD Read-out
Performance evaluation
– Response for cosmic ray and proton
– Linearity
– Energy resolution
Summary
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Construction of CFT prototype
Straight layer
Fiber fixing frame
Fixed to only frame hole Fiber was not glued each other
400 mm
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Construction of CFT prototype
Straight layerSpiral layerUU層層
Fiber fixing frame
Fixed to only frame hole Fiber was not glued each other
400 mm
400 mm
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Construction of CFT prototype
Straight layerSpiral layerUU層層
Fiber fixing frame
• Number of fiber : ~1100 channels
Fixed to only frame hole Fiber was not glued each other
400 mm
400 mm
400400mmmm
100100mmmm3 layers were combined. 3 layers were combined.
Φ1+U+Φ2Φ1+U+Φ2
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Readout ~photon sensor~• Number of fiber : 1100 channel• Photon sensor
: MPPC fiber by fiber A circuit mounting 32 MPPCs
Readout frame
Edge of fibers
64mm
30m
m
1×1mm2
6mm間隔 100μm精度ゴムシート 0.8mm
MPPC
• Contact between fiber and MPPC– by connecting PCB and readout
frame
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Readout ~photon sensor~• Number of fiber : 1100 channel• Photon sensor
: MPPC fiber by fiber A circuit mounting 32 MPPCs
Readout frame
Edge of fibers
spacer(rubber sheet)
0.8mm
attach
64mm
30m
m
1×1mm2
6mm間隔 100μm精度ゴムシート 0.8mm
Readout frame
MPPC
fiber
MPPC
• Contact between fiber and MPPC– by connecting PCB and readout
framecontact
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Ref EASIROC chip : proceedings of NDIP 2011 Omega/IN2P3EASIROC board : R. Honda PD12
Readout ~photon sensor~• Number of fiber : 1100 channel• Photon sensor
: MPPC fiber by fiber A circuit mounting 32 MPPCs
Readout frame
Edge of fibers
spacer(rubber sheet)
0.8mm
attach
64mm
30m
m
1×1mm2
6mm間隔 100μm精度ゴムシート 0.8mm
Readout frame
MPPC
fiber
MPPC
EASIROC board
• Contact between fiber and MPPC– by connecting PCB and readout
framecontact
ADC , TDC , bias adjustment etc...
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MPPC operation
• For uniformity of MPPCs– Each MPPC's gain was adjusted
by changing bias voltage.
– 1,100 MPPCs were adjusted.
• Operation voltage– Over Voltage ≈ 1.4V
ADC [ch]
pedestal
1 photon
2 photon
MPPC output
– Fittingしてない絵
EASIROC20mV/bit, 0~4.5Vfor each channel
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y[m
m] Measurement of cosmic ray
• Mean value = 19 p.e. – sufficient to distinguish hit
Photon Num oftypical fiber
p.e.
p.e.
Fiber No.
Light yield was almost uniform.
Uniformity for all fibersDistribution of p.e. for cosmic ray
Uniformity for all fibers
coun
t
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Contents Motivation for development
– Requirements Construction of Cylindrical Fiber Tracker
– Fiber construction– PPD Read-out
Performance evaluation
– Response for cosmic ray and proton
– Linearity
– Energy resolution
Summary
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Performance evaluationMeasurement of energy deposit
➢ Linearity ➢ Between energy deposit and light yield
➢ Energy resolution➢ Require σ/Mean = 35% for 70MeV proton for 1 layer
in order to resolve proton and pion with 4σ
Σ decay product
π±
beam
K+
S±S±'
n
p±p'
pcosmic ray
MIP particle
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Test experiment in CYRIC
Behavior for proton
θp beam
CFT
CH2target
– Angular resolution
Performance evaluation for protonΔE-E relation PID⇒
⇒⇒ angular resolution was acceptable
・ pp scattering experiment– 80MeV proton beam from
cyclotron @CYRIC in Tohoku Univ.σ
E(BGO) =1.2%
for 80MeV p beam
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Test experiment in CYRIC
Behavior for proton
θp beam
CFT
CH2target
energy deposit:dEScattering angle : θ
kinetic energy:E
– Angular resolution
Performance evaluation for protonΔE-E relation PID⇒
⇒⇒ angular resolution was acceptable
・ pp scattering experiment– 80MeV proton beam from
cyclotron @CYRIC in Tohoku Univ.
– Ep is selected by θ
σE(BGO)
=1.2% for 80MeV p beam
Kin
etic
en
erg
y E
[M
eV
]
Scattering angle θ [degree]
response for proton 20~70 MeV
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Linearity of light yield• Separating angles corresponds to select Ep.selecting θ
SimulationEstimated energy deposit
Experimental datap.e.
comparecompare
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Linearity of light yield
Estimated energy deposit [MeV]
MPPC covering area to fiber : 400pixel*(covering ratio) ≒ 180pixel
1mm
0.75mm
dete
cted
p.e
.
cosmic ray
Response function
Nout = Neff*{1- exp(-B*dE/Neff)}
Neff = effective pixel number of MPPC
= 197 pixels
• dE from proton is higher than that of MIP
• Separating angles corresponds to select Ep.selecting θ
SimulationEstimated energy deposit
Experimental datap.e.
comparecompare
※ For each layer
PreliminaryPreliminary
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Linearity of light yield
Estimated energy deposit [MeV]
MPPC covering area to fiber : 400pixel*(covering ratio) ≒ 180pixel
1mm
0.75mm
dete
cted
p.e
.
cosmic ray
Response function
Nout = Neff*{1- exp(-B*dE/Neff)}
Neff = effective pixel number of MPPC
= 197 pixels
• dE from proton is higher than that of MIP
• Separating angles corresponds to select Ep.selecting θ
How much does non-linearity affect to energy resolution ?
SimulationEstimated energy deposit
Experimental datap.e.
comparecompare
※ For each layer
PreliminaryPreliminary
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Energy resolution
Estimated energy deposit [MeV]
Ene
rgy
reso
lutio
n [%
]
• Resolution was worse than simulation. <-- to be calibrated for each channel• Energy resolution of CFT = 28%28% for 70MeV proton (dE = 0.7MeV)
satisfied our requirement (35% for 70MeV)
Energy resolution of one layer
PreliminaryPreliminary • Simulation – Cylinder Shape of fiber– Fluctuation of Photon
number– MPPC Saturation
suggests that resolution will become worse at high dE region.
SimulationData
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summary We plan to perform Σp scattering experiment at J-PARC
CFT(Cylindrical Fiber Tracker) will measure the trajectory and the energy deposit
Construction –– a Prototype consists of 3 layers• Scintillation Fiber + MPPC• 2 straight layers +1 spiral layer ≈ 1,100 fibers• MPPCs which read each fiber were operated by EASIROC board
Performance evaluation • Measured cosmic ray and pp scattering
– Cosmic-ray ・・・ Mean detected photon number = 19 p.e.• Linearity ・・・ MPPC saturated in high energy deposit region.• Effective pixel number of MPPC = 197pixels
⇔ consistent with fiber covering area• Energy resolution
– worse than that of simulation ← to be improved
– σ/Mean = 28% for 70MeV proton(dE=4.7MeV)
satisfied our requirement
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Back up
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To improve the energy resolution
Estimated energy deposit [MeV]
dete
cted
p.e
.
cosmic ray
1mm
0.75mm
• Calibration method– Response function
➢ Layer by layer (now)contain the effect of the deviation of MPPC' gain
➢ ⇒⇒ fiber by fiber Energy resolution should be improved.
• Expand MPPC effective area– Inserting a spacer between fiber and MPPC– MPPC saturation will become weaker.
• etc... fiber
MPPC
fiber
Spacer
MPPC
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32
A design of actual type Actual detectors
The design have almost finished
Just now constructing
CFT BGO
CFT+BGO
・BGO calorimeter ・・・
24 BGO(30×25×400mm3) will be placed cylindrically
・CFT ・・・
4 Φ layers,4 U・V layers ~5,000 fibers
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x[mm]
y[m
m]
Φ1U
Φ2
Efficiency• Efficiency for Φ layer
(actual hit) / (expected by other 3 hit track)Φ1-①
Φ1-③
Φ2-①
Φ2-③
actual hit
expected byother 3 hit
?
・ Number of photon is sufficient・ Position dependence
⇒ suggest that there were some space between some fibers
efficiency = 87%Position dependence of efficiency– Each fiber position
– to be improved
{
Φ=0
Φ
Φ
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h
Linearity of light yield
Estimated dE for pp scat.
•
Detected p.e.
en
erg
y d
ep
osi
t [M
eV
]
• Linearity between energy deposit(simulation) and p.e.(actually detected)
energy deposit [MeV]
de
tect
ed
p.e
.
Comparevia scattering angle
cosmic ray
considering air gap (0.8mm) between fiber edge and MPPC
• 176 pixel
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angular resolution
Target peak13.7mm(σ)13.7mm(σ)
・estimated from σvertex
=13.7mm13.7mm
σΔθ
=1.0°
・Ideal resolution (Geant4)σ
Δθ=0.77° , σ
vertex=9.4mm
vertex
proton beam
Prototype nearly realized the simulated performance ⇒ to be better by improving position precision
Vertex (beam line) [mm]
Ep'calc (pC scattering)
Ep'calc (pp)
Ep'
mea
sure
(BG
O+
CF
T)
[MeV
] Angular distribution of Ep'
Scattering angle [degree]
CH2target(200μm t)
Trajectory was reconstructed by CFT ----> vertex ( beam line × trajectory)