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Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of hybrid target
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Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Dec 18, 2015

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Page 1: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Status of the experiment at KEKB for the hybrid targets

Junji Urakawa instead of T.TakahashiKEK

Positron Workshop Durham28 October 2009

First test of hybrid target

Page 2: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

R.Chehab/Posipol2008/Hiroshima, june 2008 2

POSITRON SOURCES USING CHANNELING FOR ILC & CLIC

THE BASIC SCHEME FOR ILC & CLIC

e-

Crystal Amorphous

e+, e-, e-

e+

“x” meters

Only the photons are impinging on the converter: that limits the energy deposition in the amorphous target. The yield is less than if the particles coming from the crystal were also impinging on the amorphous target

Radiator Converter

Page 3: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

R.Chehab/Posipol2008/Hiroshima, june 2008 3

POSITRON SOURCES USING CHANNELING FOR ILC & CLIC

PROPOSED POSITRON TARGET FOR CLIC

e-

Crystal Amorphous

e+, e-, g ge-

e+

2 m

(5 GeV)

W: 1.4 mm thick W: 10 mm thick

With an incident beam of 2.34 1012 e-/pulse, we expect 2.1 1012 e+/pulse at 270 MeV (pulse of 156 ns) Or 6.7 109 e+/bunch

PEDD can bewell below damage threshold for CLIC

Page 4: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

300Hz generation for ILC

Page 5: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Hybrid Target for the ILC

• KEKB LINAC– E(beam) : 8GeV– Bunch Charge: ~nC– Repetition : up to 50Hz (may limited by radiation safety )

Good place for the test (except for muti-bunch operation )

10 GeV

1 mm 8 mm

Page 6: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

experimental site KEKB LINAC

e+ source

Switch yard

Page 7: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Set up SiteLooking up from Down stream

Page 8: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

A TEST at KEKB LINAC1 To Demonstrate

• positron yield with the hybrid system• heat reduction by hybrid target

2. Detail investigation toward the positron source• momentum distribution,• angular distribution of e+

w/ a real beam (angular divergence, alignment) and crystal (mosicity),,,

JFY2009

JFY2010~

Page 9: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Status and Preliminary results of first beam test

September 21 – 23 2009

All results shown in the following slides are preliminary

Page 10: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Setup

8GeV e- 1mm W crystal

Sweeping Magnet0.96T 0.75m

amorphous W0.4 mm8 mm

Analyzing magnet5 ~ 20MeV

Page 11: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Around the magnet

15 hole in the lead shielding

s

All charged particles aredumped here when the Sweeping magnet ON

Shielding lead bricks

Page 12: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Data Acquisition Counting room Beam Area

PMe+

Beam current

Gate

ADC

e-

Goniometers to Align Crystal

e+ detector

motor Controller

Page 13: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

e+ of the least yield condition

Background conditions

Sweep mag

No Crystal

ANA. magset to 20 MeV

No Amorphous

e- Sweep mag

Crystal Woff Aligned

ANA. magset to 20 MeV

0.4mm Amorphous W

background

ADC counts

Signal is well separated from background evenwith thin converter

Page 14: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

posi

tron

yie

ld (a

rb. u

nit)

angle of crystal w.r.t. beam (mr)

rot. in vertical plain

esweep mag

0.4mm

Rocking curve

1

2

2.27 0.06

4.86 0.2

144.4 1.1const

2 2

2 21 22 2( )f Ae Be Const

Well fitted by two Gaussians Channeling + CB?

Narrower component is still x 4wider than the critical angle

Page 15: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

posi

tron

yie

ld (a

rb. u

nit)

angle of crystal w.r.t. beam (mr)

esweep mag

0.4mm

Rocking curve

1

2

2.07 0.04

5.3 0.2

141 1const

2 2

2 21 22 2( )f Ae Be Const

Page 16: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

data looks likes..

BG

Wa 0.4mmCr off aligned

amorphous 0.4mmCr aligned

amorpous 8mmCr aligned

amorphous 8mmCr not aligned

ADC counts

num

ber o

f cou

nts

/bin

Page 17: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

After BG substraction

Wa 0.4mmCr off aligned

amorphous 0.4mmCr aligned

amorpous 8mmCr aligned

amorphous 8mmCr not aligned

ADC counts

num

ber o

f cou

nts

/bin

1.9

1.2

Page 18: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

sweeping magnet OFF

No CrystalAmorpous8mm

amorpous 8mmCr aligned

amorphous 8mmCr not aligned

ADC counts

num

ber o

f cou

nts

/bin

1.07

Page 19: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Momentum dist.

P [MeV/C]

e+ y

ield

Page 20: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Data was taken under various conditonsCrystal amorphous Sweep mag Ana mag

NO NO on 20MeValigned 0.4mm on 20MeV

not alinged 0.4mm on 20MeVnot alinged NO on 20MeV

aligned 8mm on 20MeVnot alinged 8mm on 20MeVnot alinged NO on 20MeV

aligned NO on 20MeVoff NO on 20MeV

aligned 8mm off 20MeVnot alinged 8mm off 20MeV

aligned NO off 20MeVnot alinged NO off 20MeV

off 8mm off 20MeVNO NO off 20MeVon 8mm on 15MeV〃 8mm on 10MeV〃 8mm on 5MeV

Page 21: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Summray• Set up works !

– Very small backgound– DAQ seems good enough

• already have – many to be analyzed– worth to compare with simulation– some quantitative results in this workshop

• Hope temperature data in next run (Jan. 2010)

Page 22: Status of the experiment at KEKB for the hybrid targets Junji Urakawa instead of T.Takahashi KEK Positron Workshop Durham 28 October 2009 First test of.

Background conditions

Sweep mag

No Crystal

ANA. magset to 20 MeV

No Amorphous

e- Sweep mag

Crystaloff Aligned

ANA. magset to 20 MeV

No Amorphous

background e+ of the least yield condition

ADC counts

Signal is well separated from background evenwith NO converter