1
1.98GeV Damping ring Bunch compressor-2 8GeV Pre-Linac (S-band ) Experimental Hall 240GeV electron Main Linac (X-band) 240GeV positron Main Linac (X-band) Pre-damping ring 8GeV Pre-Linac ( S-band ) Bunch compressor-2 Positron target Polarized electron source 1.98GeV Linac ( S-band ) 1.98GeV Linac ( S-band ) 10GeV Linac ( S-band ) electron gun Bunch compressor-1 Bunch compressor-1 FEL facility 1.98GeV Damping ring Vertex Detector of CCD : YAG laser prober system for a measurement of spatial resolution at Niigata Univ.: Laser beam pulses of 2x2µm 2 spot size and 1064 nm wavelength are injected into CCD sensors to simulate the minimum ionizing particles. The incident position is controlled with a precision of 1µm. Calorimeter : A hadron calorimeter test module under assembling for test beam measurement at FNAL-MT6. The module is a sampling calorimeter composed of plastic scintillator and lead with hardware-compensating ratio. Tile/fiber scheme is used for optical readout. This module has achieved hadron energy resolution of 46.7%/E +0.9% with linearity better than 1% over energy range from 2GeV to 200GeV. Interaction Region : Study on an oscillation property of support system in a case of cantilever : A pair of final doublets must be aligned at sub-nano meter level during collisions at an interaction point. Central Drift Chamber : The so called "baby" chamber for beam-testing the performance of the mini-jet-cell of the current JLC central drift chamber design. The cell consists of 5 sense wires with a maximum drift length of 5cm and has been proved to provide an average spatial resolution better than 100 µm and 2-hit separation better than 2mm. µ + µ The Asian Committee for Future Accelerators (ACFA), considering the importance of the Electron-Positron Linear Collider Project and the potential of the Asian community to realize it, has initiated the Physics & Detector Study Group under ACFA in 1998. The charge of the group is to elucidate physics scenario and experimental feasibilities at the Linear Collider. An ACFA-JLC report will be completed in this summer, 2001, in order to summarize studies on the charge. Detector R&D An Accelerating Structure : View of a 1.8m- long X-band accelerating structure unit, which was assembled by using the diffusion bonding technique. Insert: Individual copper disks (61 mm diameter) that are high-precision machined at KEK for building the accelerating structure. A X-band klystron with periodic permanent magnet (PPM) focusing : This prototype produced 56 MW output power. A newer prototype, currently under testing, has recently produced 72 MW, 1.4 µsec at 25 Hz, nearly reaching the JLC design goal. C-band technologies are mature for the main linac. Performances of all RF componets have been verified for a 500 GeV collider. “C-band” linear collider as a backup option for JLC. Polarized Electron Source Accelerator R&D 0 20 40 60 80 100 0.0001 0.001 0.01 0.1 1 10 700 750 800 850 Polarization (%) Quantum Efficiency (%) Wavelength (nm) 0 0.5 1 0 2 4 6 8 10 2.55 µJ/bunch 0.90 µJ/bunch 0.27 µJ/bunch Current (A) Time (ns) Laser energy Polarization and quantum efficiency as a function of laser wavelength, measured for GaAs-GaAsP strained-layer super-lattice. Sub-nanosecond bunches measured for GaAs-GaAsP strained-layer super-lattice. JLC-PES collaboration (Nagoya Univ., KEK et.al ) Electron-positron Linear Collider at E cm =500GeV based on a X-band technology for e + e - , γγ , e - γ and e - e - experiments A B C X Y IP parameters Luminosity a (10 33 ) 8.79 8.20 7.49 14.6 24.9 Nominal luminosity b (10 33 ) 6.37 6.22 4.98 11.2 18.2 Repetition rate f rep (Hz) 150 150 Bunch charge N (10 10 ) 0.75 0.95 1.1 0.55 0.70 Bunches RF pulse n b 95 190 Bunch separation (ns) 2.8 1.4 Injected γε x γε y (10 -8 m-rad) 300 3 300 3 γε x at IP (10 -8 m-rad) 400 450 500 400 400 γε y at IP (10 -8 m-rad) 6 10 14 4 4 β x β y at IP (mm) 10 0.10 12 0.12 13 0.20 7 0.08 7 0.08 σ x σ y at IP (nm) 286 3.50 332 4.95 365 7.56 239 2.56 239 2.56 Bunch length σ z ( μ m) 90 120 145 80 80 Disruption parameters D x D y 0.094 7.67 0.117 7.86 0.135 6.53 0.088 8.19 0.112 10.4 Beamstrahlung parameter Υ 0.128 0.104 0.090 0.126 0.161 Pinch enhancement factor 1.38 1.32 1.50 1.30 1.37 Beamstrahlung δ B (%) 4.0 3.9 3.8 3.5 5.1 Photons per e e 1.07 1.18 1.27 0.94 1.18 Main Parameters at E cm =500GeV Main Parameters at E cm =500GeV KEK JLC High Energy Accerelator Research Organization

KEK JLC - Laboratori Nazionali di FrascatiKEK for building the accelerating structure. A X-band klystron with periodic permanent magnet (PPM) focusing : This prototype produced 56

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Page 1: KEK JLC - Laboratori Nazionali di FrascatiKEK for building the accelerating structure. A X-band klystron with periodic permanent magnet (PPM) focusing : This prototype produced 56

1.98GeVDamping ring

Bunch compressor-2

8GeV Pre-Linac (S-band )

Experimental Hall

240GeV electronMain Linac (X-band)

240GeV positronMain Linac (X-band)

Pre-damping ring

8GeV Pre-Linac ( S-band )Bunch compressor-2

Positron target

Polarized electron source

1.98GeV Linac ( S-band )

1.98GeV Linac( S-band )

10GeV Linac( S-band )

electron gun

Bunchcompressor-1

Bunchcompressor-1

FEL facility

1.98GeVDamping ring

Vertex Detector of CCD : YAG laser prober system for a measurement of spatial resolution at Niigata Univ.: Laser beam pulses of 2x2µm2 spot size and 1064 nm wavelength are injected into CCD sensors to simulate the minimum ionizing particles. The incident position is controlled with a precision of 1µm.

Calorimeter : A hadron calorimeter test module under assembling for test beam measurement at FNAL-MT6. The module is a sampling calorimeter composed of plastic scintillator and lead with hardware-compensating ratio. Tile/fiber scheme is used for optical readout. This module has achieved hadron energy resolution of 46.7%/√E +0.9% with linearity better than 1% over energy range from 2GeV to 200GeV.

Interaction Region : Study on an oscillation property of support system in a case of cantilever : A pair of final doublets must be aligned at sub-nano meter level during collisions at an interaction point.

Central Drift Chamber : The so called "baby" chamber for beam-testing the performance of the mini-jet-cell of the current JLC central drift chamber design. The cell consists of 5 sense wires with a maximum drift length of 5cm and has been proved to provide an average spatialresolution better than 100 µm and 2-hit separation better than 2mm.

µ +

µ −

The Asian Committee for Future Accelerators (ACFA), considering the importance of the Electron-Positron Linear Collider Project and the potential of the Asian community to realize it, has initiated the Physics & Detector Study Group under ACFA in 1998. The charge of the group is to elucidate physics scenario and experimental feasibilities at the Linear Collider. An ACFA-JLC report will be completed in this summer, 2001, in order to summarize studies on the charge.

Detector R&D

An Accelerating Structure : View of a 1.8m-long X-band accelerating structure unit, which was assembled by using the diffusion bonding technique. Insert: Individual copper disks (61 mm diameter) that are high-precision machined at KEK for building the accelerating structure.

A X-band klystron with periodic permanent magnet (PPM) focusing : This prototype produced 56 MW output power. A newer prototype, currently under testing, has recently produced 72 MW, 1.4 µsec at 25 Hz, nearly reaching the JLC design goal.

C-band technologies are mature for the main linac.Performances of all RF componets have been verified for a 500 GeV collider.

“C-band” linear collider as a backup option for JLC.

Polarized Electron Source

Accelerator R&D

0

20

40

60

80

100

0.0001

0.001

0.01

0.1

1

10

700 750 800 850

Pol

ariz

atio

n (%

)

Quantum

Efficiency (%

)

Wavelength (nm)

0

0.5

1

0 2 4 6 8 10

2.55 µJ/bunch0.90 µJ/bunch0.27 µJ/bunch

Cur

rent

(A

)

Time (ns)

Laser energy

Polarization and quantum efficiency as a function of laser wavelength, measured for GaAs-GaAsP strained-layer super-lattice.

Sub-nanosecond bunches measured for GaAs-GaAsP strained-layer super-lattice.

JLC-PES collaboration (Nagoya Univ., KEK et.al )

Electron-positron Linear Collider at Ecm=500GeV based on a X-bandtechnology for e+e-, γγ , e-γ and e-e- experiments

A B C X YIP parameters

Luminositya (1033) 8.79 8.20 7.49 14.6 24.9Nominal luminosityb (1033) 6.37 6.22 4.98 11.2 18.2Repetition rate frep (Hz) 150 150Bunch charge N (1010) 0.75 0.95 1.1 0.55 0.70Bunches/RF pulse nb 95 190Bunch separation (ns) 2.8 1.4Injected γεx/γεy (10-8m-rad) 300/3 300/3

γεx at IP (10-8m-rad) 400 450 500 400 400γεy at IP (10-8m-rad) 6 10 14 4 4βx/βy at IP (mm) 10/0.10 12/0.12 13/0.20 7/0.08 7/0.08σx/σy at IP (nm) 286/3.50 332/4.95 365/7.56 239/2.56 239/2.56Bunch length σz (μm) 90 120 145 80 80Disruption parameters Dx/Dy 0.094/7.67 0.117/7.86 0.135/6.53 0.088/8.19 0.112/10.4Beamstrahlung parameter Υ 0.128 0.104 0.090 0.126 0.161�Pinch enhancement factor 1.38 1.32 1.50 1.30 1.37Beamstrahlung δB (%) 4.0 3.9 3.8 3.5 5.1# Photons per e-/e+ 1.07 1.18 1.27 0.94 1.18

Main Parameters at Ecm=500GeVMain Parameters at Ecm=500GeV

KEK JLCHigh Energy Accerelator Research Organization