Future Neutrino Beam in J-PARC Tetsuro Sekiguchi IPNS, KEK 2013/11/12NNN2013, Kavli IPMU1.

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Presentation transcript:

Future Neutrino Beam in J-PARC Tetsuro Sekiguchi IPNS, KEK 2013/11/12NNN2013, Kavli IPMU1

Contents Introduction Upgrade Plan of J-PARC accelerator Upgrade Plan of Neutrino Facility Summary 2013/11/12NNN2013, Kavli IPMU2

J-PARC Materials and Life Science Experimental Facility (MLF) Hadron Experimental Facility Rapid Cycle Synchrotron (RCS) (3 GeV synchrotron) (25 Hz, 1MW) Linac (330m) Main Ring (MR) (30 GeV synchrotron) (0.75MW) 500 m Neutrino Experimental Facility 2013/11/12NNN2013, Kavli IPMU3

Neutrino Facility BeamDump PrimaryBeam-line ExtractionPoint MuonMonitors 110m 280m 295km To Kamioka Main Ring TargetHorns P  DecayVolume Near Neutrino Detectors 2013/11/12NNN2013, Kavli IPMU4

Neutrino Beamline Conventional neutrino beam – p + C   +   + +  Designed for T2K experiment – High intensity beam 750kW proton beam (30 GeV, 3.3x10 14 protons/pulse) – Off-axis beam (2~2.5 o ) Narrow band beam ~ 0.6 GeV – 1 st oscillation maximum 2013/11/12NNN2013, Kavli IPMU5  + ->  + +  decay  Target Horns Decay Pipe SK Oscillation Maximum

Secondary Beamline a 2013/11/12NNN2013, Kavli IPMU6 Target Station (target and horns inside He vessel) Decay volume Beam dump

Target Station 2013/11/12NNN2013, Kavli IPMU7 15.0m 10.6m Baffle Graphite Collimator Horn-1 Horn-2 Horn-3 Beam window Ti-alloy DV collimator Large flange, sealed with Al plates, t= 120mm 3 horns / a baffle are placed inside He vessel Apparatus on the beam-line highly irradiated after beam. Handled by remote-controlled crane. Service Pit OTR Target Beam

Target 2013/11/12NNN2013, Kavli IPMU8 Remote maintenance Remote maintenance 26mmx 910mm Ti-6Al-4V (0.3mmT) Graphite IG-430U He-gas cooling T~200K ~7MPa (Tensile strength 37MPa) 736 o C 30GeV-750kW (~20kW heat load) CFX analyses 9Nm 3 /min9Nm 3 /min(v=200m/s) Conductivity 140  20W/mK(rad. damage)

Magnetic Horns Aluminum alloy conductor (A6061-T6) – Double cylinder (inner: t3mm, outer: t10mm) – Tensile strength: 310MPa  95MPa after 5x10 8 cycle – 25MPa allowable stress (taking into account corrosion) – Safety factor ~ 2 320kA pulsed current (rated) – 2.1 T (max.) toroidal field – 2~3ms pulse width – 0.4Hz rep. rate  1 Hz for 750kW Water cooled – Total heat load: 750kW 15kJ (beam) + 10kJ (Joule) – Spraying water to inner conductor 2013/11/12NNN2013, Kavli IPMU9

Decay Volume & Beam Dump Decay Volume – 100m-long – Water cooled iron walls  4MW – 2~2.5 o OA angle for SK and HK Beam Dump – Graphite core – Water cooled  3MW 2013/11/12NNN2013, Kavli IPMU10 Designed for multi-MW beam since no access is possible after beam operation due to irradiation

Operation History 2013/11/12NNN2013, Kavli IPMU11 Delivered # of Protons Protons Per Pulse 1.43x10 20 pot until Mar.11,’ x10 20 pot Jun.9,’12 Rep=3.52s  50kW [6 bunches] 3.2s  3.04s  145kW 2.56s  190kW Mar.8, 2012 Run-1Run-2Run s  235kW Run x x x10 20 pot until May.8,’ x x x x10 7 Total # of pulses 1.2x10 14 ppp: world record of extracted protons/pulse for synchrotron No replacement of target and horns up to 1.2x10 7 pulses

Contents Introduction Upgrade Plan of J-PARC accelerator Upgrade Plan of Neutrino Facility Summary 2013/11/12NNN2013, Kavli IPMU12

Linac Upgrade New accelerating structure, ACS, will be installed to increase the extracted beam energy from 181MeV to 400MeV (JFY2013) Front-end part (IS+RFQ) will be replaced to increase peak current from 30mA to 50mA (JFY2014) 2013/11/12NNN2013, Kavli IPMU13 RF antenna Collab. w/ SNS

MR Upgrade 2013/11/12NNN2013, Kavli IPMU14 Number of protons/pulse is limited by beam loss due to space charge effect – ~450kW is estimated upper limit with current apparatus. To achieve 750kW – Higher beam energy than 30GeV Too high power consumption P 50GeV =4xP 30GeV – Higher rep. rate than 0.4Hz 1.3sec cycle with 2.0x10 14 protons/pulse We choose higher rep. rate scenario for 750kW

MR Upgrade 2013/11/12NNN2013, Kavli IPMU15 2kW  3.5kW

MR Upgrade Timeline 2013/11/12NNN2013, Kavli IPMU16 750kW 400kW 300kW 200kW 150kW

Contents Introduction Upgrade Plan of J-PARC accelerator Upgrade Plan of Neutrino Facility Summary 2013/11/12NNN2013, Kavli IPMU17

Acceptable Beam Power Acceptance of each component for high power beam – Target Mechanical: 0.75MW Cooling: 0.75MW – Horn Cooling for conductors: 1.85MW Cooling for striplines: 0.4MW Hydrogen production: 0.3MW Power supply: 0.4Hz, 250kA – He vessel, Decay Volume & Beam Dump Cooling: 4MW(HV&DV), 3MW(BD) – Facility Water disposal: 0.5MW Radio-active air: 0.5MW 2013/11/12NNN2013, Kavli IPMU18

Hydrogen Production in Horn H 2 production by water radiolysis (2H 2 O  2H 2 +O 2 ) – H 2 production rate: 40L/day – H 2 must be removed.  H 2 recombination (2H 2 +O 2  2H 2 O) 2013/11/12NNN2013, Kavli IPMU19 Buffer tank Pump Suction pump He vessel Height ~8m Service PitMachine Room H2OH2O He He gas line H2H2 Beam

Hydrogen Production in Horn H 2 recombination + forced circulation outside He vessel – H 2 density after 1 week 220kW beam 1.6% near horn, 1.0% in tank – ~1.5% expected w/o recomb.  H 2 inside horn not removed. Forced circulation inside horn is really necessary. 2013/11/12NNN2013, Kavli IPMU20 Buffer tank Pump Suction pump He vessel Height ~8m Service PitMachine Room H2OH2O He He gas line H2H2 Beam diffusion H 2 : 1.6% O 2 : 0.7% H 2 : 1.0% O 2 : 0.03% Acceptable beam power ~300kW Catalyst canister (Catalyst = Alumina pellet with 0.5%Pd )

Hydrogen Production in Horn Forced circulation inside horns – New horns have forced circulation lines H 2 density will be below 1% even with higher power beam New horn will be installed in FY /11/12NNN2013, Kavli IPMU21 Buffer tank Pump Suction pump He vessel Height ~8m Service PitMachine Room H2OH2O He He gas line H2H2 Beam Forced circulation Acceptable beam power should be checked with beam

Horn Power Supply New power supply production for 1Hz operation, – Designed for 320kA operation – Energy recovery (~50% of stored energy recycled) – Low input load One horn is operated with a power supply Low impedance striplines are also developed Production is on going  Operation from fall in /11/12NNN2013, Kavli IPMU22 PS (K2K) PS(New) 5.5 kV4.1 kV PS(New) 5.8 kV PS (New) 4.3 kV kA, 320 kA, 1Hz

Disposal of Radio-active Water Maintenance scenario – Be7: 53GBq/10 20 pot  removed by ion-exchanger (99.9%) – Tritium: 24GBq/10 20 pot  dilution & disposal Present capacity – 80 dilution cycles/year (3 working days/cycle) – Acceptable beam power is ~500kW 2013/11/12NNN2013, Kavli IPMU23 Remove 99.9 % of 7 Be 80times /year Accessible during beam No access during beam Regulation Be7 < 30Bq/cc H3 < 42Bq/cc

Disposal of Radio-active Water Upgrade of water disposal system – New building for water disposal system is planned. – 240m 3 DP tank (320m 3 in total)  2MW acceptable 2013/11/12NNN2013, Kavli IPMU24 Remove 99.9 % of 7 Be 80times /year Accessible during beam No access during beam Regulation Be7 < 30Bq/cc H3 < 42Bq/cc New DP tank 240m 3 New facility building

Radio-active Air 2013/11/12NNN2013, Kavli IPMU25 Helium compressor Cooling water system Machine room Service pit Ground floor Concrete shields Storage area Building Chimney stack Exhaust system Radiation monitor for exhaust air Target Horns Helium vessel Short-lifetime radio-activity like Ar41(  ~2h) produced in underground area

Radio-active Air 2013/11/12NNN2013, Kavli IPMU26 Helium compressor Cooling water system Machine room Service pit Ground floor Concrete shields Storage area Building Chimney stack Regulation by law: < 0.5 mBq/cc Exhaust system Radiation monitor for exhaust air Target Horns Go out through exhaust line Leakage of radioactive air from underground area through gaps Helium vessel

Air Tightness Improvement 2013/11/12NNN2013, Kavli IPMU27 Caulking between concrete shields Lay the air-tight sheet Lay the protection sheet under air-tight sheet Air-tight sheet (made of the same material for balloon) Protection sheet (over air-tight sheet)

Radio-active Air 2013/11/12NNN2013, Kavli IPMU28 Helium compressor Cooling water system Machine room Service pit Ground floor Concrete shields Storage area Building Chimney stack Regulation by law: < 0.5 mBq/cc Caulking + Air-tight sheet Exhaust system Radiation monitor for exhaust air Target Horns Now : ~ kW Go out through exhaust line Leak rate reduced, but leakage happens through the edge of sheet. Helium vessel Acceptable beam power ~500kW

Radio-active Air 2013/11/12NNN2013, Kavli IPMU29 Helium compressor Cooling water system Machine room Service pit Ground floor Concrete shields Storage area Building Chimney stack Regulation by law: < 0.5 mBq/cc Caulking + Air-tight sheet Exhaust system Radiation monitor for exhaust air Target Horns Go out through exhaust line Helium vessel Add air-tight lamination (made of steel and air-tight material) under concrete shields Acceptable beam power > 1MW (should be confirmed with actual setup)

Acceptable Beam Power Acceptance of each component for high power beam – Target Mechanical: 0.75MW Cooling: 0.75MW – Horn Cooling for conductors: 1.85MW Cooling for striplines: 0.4MW  0.75MW (2014~) Hydrogen production: 0.3MW  > 1MW (2014~) Power supply: 0.4Hz, 250kA  1Hz, 320kA (2014~) – He vessel, Decay Volume & Beam Dump Cooling: 4MW(HV&DV), 3MW(BD) – Facility Water disposal: 0.5MW  2MW (2016 or 2017~) Radio-active air: 0.5MW  > 1MW (2014~) 2013/11/12NNN2013, Kavli IPMU30 Graphite material is supposed to withstand up to ~1.5MW, when optimization of design including beam size, horn shape, cooling, etc is done.

Summary J-PARC neutrino beamline is designed for 750kW beam J-PARC accelerator aims to achieve 750kW beam with 1Hz operation. There are some devices which limit acceptable beam power. Several upgrades are planed to accept 750kW beam. 2013/11/12NNN2013, Kavli IPMU31