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マイクロメッシュを用いた 高増幅率型 μ-PIC の開発 Development of m -PIC using micro mesh. 神戸大学 越智 敦彦、桂華 智裕. 1. Introduction 2. Test operation of prototype 3. Simulation studies. Kobe Univ. Atsuhiko Ochi, Tomohiro Keika. 3 rd MPGD workshop @ Saga Univ. 26/Jan/2007. Introduction. Mesh. 400 m m. - PowerPoint PPT Presentation
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マイクロメッシュを用いた高増幅率型 μ-PIC の開発
Development of -PICusing micro mesh
1. Introduction2. Test operation of prototype3. Simulation studies
神戸大学 越智 敦彦、桂華 智裕Kobe Univ. Atsuhiko Ochi, Tomohiro Keika
3rd MPGD workshop @ Saga Univ. 26/Jan/2007
400m
Mesh
Introduction
• Micro pixel chamber (-PIC)– Position resolution ( - 100m)– Timing resolution ( < 100ns)– High rate capability
( > 107c/sec/mm2)
• With micro mesh– Higher gain in stable
operation (>104)
Effect using micro mesh
• Higher Electric field around the anode– Vertical direction against
detection flat– Without increase of e-field
near cathode edge Higher gas gain will
be attained safely• 104-5
• Reduction of positive ion distribution across detection volume
Applications
• Replacement of -PIC with GEM– Real time imaging device for
• X-ray• Gamma-ray• Charged particle• Neutron• etc.
• TPC– Low ion diffuse
Prototype test• Micro mesh was mounted on -PIC
– Supported by plastic film / nylon wire• Support structure is future tasks
– Distance between -PIC and wire• About 300m
– Micro mesh is connected to HV controller
• Operation gas– Ar:C2H6 = 90:10
0.5mm
Micro scope picturesfor same place(different focus point)
Micro mesh mounted on -PIC by hand.Size of -PIC = 3cm x 3cm.Efficient area using mesh = 2mm x 3cm
Test parameters
• Only signal pulses (gain) were measured– Gain dependency on
• Anode voltage (=Va)• Mesh voltage (=Vm)• Drift voltage (=Vd)
10 m
10 m100m
Drift Plane
Cathode
Anode 信号
Vd
Va
MeshVm
0
2000
4000
6000
8000
10000
12000
14000
16000
420 430 440 450 460 470 480 490 500
no meshVm=0VVm=-50VVm=-100VVm=-150V
Gain curve (Va, Vm dependence)
• Vd-Vm = 100V (Vd=2kV for no mesh plot)• Gas: Ar(90%)+C2H5(10%)• Source: Fe55 (5.9kV)
Va [V]
Gain
Collection efficiency problem
• Collection efficiencies for electrons– Depend on Vd-Vm … smaller is better
Without MeshWith mesh (Vm=0V)
Va=450V Va=450V
Vd [-V] Vd [-V]
Gain Gain
Current status of development
• Came up with the new idea -PIC with micro mesh
• Prototypes were made and tested– Gas multiplicity of it is more than 3 times– Gain of 2 x 104 were attained
• With prototype mesh (distance is about 300m)
– More studies are needed for tuning up the parameters
• Simulation studies Keika will talk
Optimization of parameters for μ-PIC with micro mesh
2007.1.26-27 MPGD workshop
@Saga Univ.
Kobe Univ.M2 Tomohiro Keika神戸大学 桂華 智裕
マイクロメッシュ μ-PIC の最適動作パラメーターの探索
Simulation Study
Parameters
•Height of micro mesh
•Mesh Voltage (Vm)
•Drift Voltage (Vd)
( Anode Voltage is fixed )We optimize the height of micro mesh using a simulation.
AnodeCathode
micromesh
Height
Optimization for detector parameters
•Structure
•Operation voltage3D simulation
About simulation softwareMaxwell3D
Garfield
3D field simulator made by Ansoft Co. America
•Make a 3D structure geometry•Calculate electromagnetic field using a finite element method (FEM) (Supported by Cosmic Ray Group at Kyoto Univ.)
2D・ 3D field simulator made by CERN
•Feed maps made by Maxwell3D to Garfield
•Calculate electromagnetic field , gas gain and so on.
Geometry drawing
We compare the three patterns.
Micro mesh100μm
200μm
500μm
or
or
Height of micro mesh
Cathode
Anode
Polyimide
Height
100μm200μm500μm
Effect using micro mesh
No micro mesh (Va=450V)
Micro mesh 100μm (Va=450V,Vm=-100V)
Micro mesh
Color display of electric field
AnodeAnode
Comparison of the results by Maxwell3D and by observed value
How to calculate gas gain•Calculated using the first Townsend coefficient•Collection-efficiency•No space-charge effect, ion-electron recombination
Focus: increasing or decreasing trend of the results
( Va=450V,Vd=-5000V )→It is the comparative data.
4102.2
Gas gain of μ-PIC without micro mesh is
Supply voltage to micro mesh
赤:Mesh100um
青:Mesh200um
緑:Mesh500um
Gai
n
4102.2
Select these parameters to compare the electric field near micro mesh.
条件: Va=450V,Vm-Vd=100V
Dependences of gas gain on Anode Voltage and Height of micro mesh
Dependences of gas gain on Anode Voltage and Height of micro
mesh
赤:メッシュ 100um
Vm=0V,Vd=-100V
青:メッシュ 200um
Vm=-100V,Vd=-200V
緑:メッシュ 500um
Vm=-300V,Vd=-400VDistance from the subtrate to micro mesh
100μm
200μm
500μm
Ele
ctri
c fi
eld
We had better lower the electric field near micro mesh to prevent electric discharge.
Collection efficiencyTerminal points of electron on the electrode plane or micro mesh.
Vm=0V Vm=-200V
Anode:37%
No-Anode:3.6%
Mesh:60%
Anode:37%
No-Anode:21%Mesh:41%
Study for the optimization using a 3D simulation.
(Qualitative interpretation)Gain dependency on voltage of mesh Vm increase Collection efficiency decrease
Estimation of electric field near the micro mesh Most desirable fields were obtained in wider (500um) case In typical case, gain using micro mesh is quite greater than symple u-PIC. simple u-PIC (Va=450V, Vd=-5000V(10mm) ) : 2.2 x 104
with micro mesh (Va=450V, Vm=-400V, Distance=500um) : 2.0 x 105
Results
Gas gain get more increasedBut
Gain rise
Future prospects
• How to hold the mesh on detector?– How to keep the flatness of the mesh?– Wire or leg?– Insulations are attached with micro mesh or -PIC?
• Optimization of geometries and operation voltage?– Collection efficiency ↑ and gas gain ↑– To get consistency of simulation and measurement
• 2 dimensional readout and larger detection area– With amplifiers and data acquisition system
• We have to get the budget for this project !!!– There is no budget about this project yet !!
• We need more than 5M JPY to make new design of -PIC