Cherenkov Detectors for b Physics Sacha Kopp University of Texas at Austin cos C = 1/(n ) CC...

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Cherenkov Detectors for b Physics Sacha Kopp University of Texas at Austin cos C = 1/(n) C “radiator” “photo-detector”
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Page 1: Cherenkov Detectors for b Physics Sacha Kopp University of Texas at Austin cos  C = 1/(n  ) CC “radiator” “photo-detector”

Cherenkov Detectors for b Physics

Sacha Kopp

University of Texas at Austin

cosC = 1/(n)

C“radiator”

“photo-detector”

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Good Ol’ Days of Cherenkov Counters

ThresholdCounter

Velocity Selector

“Fitch Counter”

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Ring-Imaging Cherenkov Detectors (RICH)

• First detectors: DELPHI “RICH” at LEP SLD “CRID” at SLC

• Both TMAE-based TPC’s, dual radiator

Original proposal in J. Séguinot & T. Ypsilantis, Nucl. Instr. Meth. 142, 377 (1977)

figures from J. Séguinot CERN-89-12

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BaBar “Detector of Internally-Reflected Cherenkov-light (DIRC)”

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DIRC Principle ee

t ~ 300 nsabout collision time

t ~ 8 nsabout collision timefigures from J. Schwiening, Nucl. Instr. Meth. A502, 67 (2003)

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BaBar DIRC Performance

figures from B. Ratcliff, RICH2004 Conference

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Belle DetectorSC solenoid 1.5T

CsI(Tl) 16X0

TOF counter

8GeV e -

Si vtx. det.3 lyr. DSSD

μ/KL detection14/15 lyr. RPC+Fe

Tracking + dE/dxsmall cell + He/C2H5

3.5GeV e +

Aerogel Cherenkov cnt.n=1.015~1.030

AK=0.101±0.025±0.005

3.9

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Particle Identification at Belle

slide taken from Blair Ratcliff, RICH 2004 Conference

p/K/π separation is based on Likelihood ratio:

LR(K)=L(K)+L(π)

L(K)

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CLEO-IIIRICH

Detector

• Fit inside existing CsI calorimeter (102 cm ID)

• Limit to 13% X0

• Needed <20 cm depth 0.0

0.2

0.4

0.6

0.8

1.0

0.0 0.5 1.0 1.5 2.0 2.5 3.0

eKp

Che

renk

ov A

ngle

(ra

d)

Momentum (GeV/c)

C = 12.8 mrad in LiF

• Coverage for daughters of B mesons produced at rest: pmax ~ 2.65 GeV/c

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Photon Detectors

Charged Particle

Cherenkov Photon

Nitrogen Expansion Volume

Carbon Fiber Support Tube

LiF Crystal

LiF + TEA Detector

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0

20

40

60

80

100

2 4 6 8 10 12

Wavelength (nm)

Tra

nsm

issi

on

orQ

uant

um E

ffic

ienc

y (%

)

Photon Energy (eV)

LiF

CaF2

He+TEA

CH4+TEA

C* (6.42)C* (7.48)

C*(7.94)

N* (8.30)

620 310 207 155 124 103

ROYGBIV

O2

H2O

• Alkali-halide crystals low dispersion (n/ = 0.0023 nm-1): cosC = 1/n() Can fabricate with good transparency, large sizes (after many yrs’ effort)

• Sole example in world: previous effort by Sauli @ FNAL E605, npe ~ 1-2

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• Images are conic intersections distorted and truncated by refractive effects.

• Total internal reflection for trk < 6° sawtooth radiatorAlso reduces chromatic aberrations

Radiator Optics

Image in photon detectors:

charged track

Sawtooth image in detectors:

primary arcssecondary arcs (+1 reflection)

charged track

emerging

internally reflected radiator

photon detector

charged track charged track

reflected emerging

4mm

Planar radiator Sawtooth radiator

A. Efimov and S. Stone, Nucl. Instr. Meth. A371, 79 (1996)

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Anode Wires

1 mm

e-CH +TEA gas4CaF Window2

4.5 mm

Window Frame

Cathode Pads

• Multiwire chamber 20246 cm2

• CH4 + TEA gas (no blinds/cloisons)

• Total 15 m2 of chambers

• <8% “dead area”

• No observed aging of components from corrosive TEA

• Cathode pad readout (80% coupling)

• Achieve effective gain ~ 105

Photon Detector MWPCs

S.K. & Georg Viehhauser

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Single Photo-electron Detection• Assume:

electronics = 400 e

chamber gain ~ 40,000

• Charged ptcles ionize ~ 62 e-/cm in CH4

• Single ’s: large statistical fluctuations.• Gain limit g~105 due to feedback

(R.Arnold et al, Nucl. Instr. Meth. A270, 255 (1980).

originally seen by H. Schlumbohm, Z. Phys. 151, 563 (1958)

• Analog readout of signal accurate clustering in RICH identification of charged

particles

4

/1dze

ggz

= e4/g

= 96%

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Readout Electronics

• VA_RICH chip variation of chip used for Si tracking detectors (input Cdet)

daisy-chain multiple chips into one VME controller input protection (protect against chamber sparking) dynamic range 650,000 e

Marina Artuso

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Electronics Performance

• 230,400 channels in CLEO RICH onboard sparsification.

• Coherent noise subtraction was an improvement, also adopted for CsI incoh ~ 2.6 ADC counts ~ 400e

Marina Artuso & Silvia Schuh

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• Parasitic µ beam (> 100 GeV).

• 2 MWPCs as track reference

• Demonstrated npe~12 expected for CLEO-III

Sawtooth works as expected given clarity measurements.

RICH Beam Test

E866 beam dump

MWPC1MWPC2

Trigger counters

Vetocounter

1.5 m

RICHconcrete

N = 13.5N = 13.5

=4.8 mr =4.8 mr

CC

NN

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photo of beam testBeamline

Elliot Lipeles

Ray Mountain

Silvia Schuh

Alex Efimov

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Beam Test Events Planar

Sawtooth

M. Artuso et al Nucl. Instrum. Meth. A441, 374 (2000)

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Yuri Maravin

Jeff Cherwinka

Rachid Ayad

Rachid Ayad

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AlexSmith

RayMountain

GeorgViehhauser

SilviaShuh

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Ray Mountain

Jeff Cherwinka

Georg Viehhauser

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First CLEO-III Data

ee ee taken from T. Skwarnicki, BCP Conference, Taipei, Dec. ‘99

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CLEO-III RICH Performance

M. Artuso et al, Nucl. Instrum. Meth. A554: 147-194 (2005)

BDK

BD

Beam Constrained Mass (GeV/c)

A. Bornheim et al, Phys. Rev. D68:052002 (2003)

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LHCb Layout

b Exp’ts at Hadron Machines

CERN LHC Proposed for FNAL Tevatron

• Purpose is to collect large samples to over-constrain Unitarity Triangle and search for New Physics.

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Particle ID in Forward b Experiments

Gas

C4F8O

n=1.00138

LiquidC5F12

n=1.24

(proximity focused)(mirror-focused)

(mirror-focused)BTeV RICH

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-20,000 V

-19,890 V

-15,800 V

ground

Vacuum-based Photodetectors

0pe 1pe

2pe

3pe

BTeV HPD readout with VA_RICH

87 mm

125 mm

e-

+60 VSilicondiode

HPD: DEP PP0380AT

figures from T. Skwarnicki, presentation at DOE review of BTeV

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MAPMTs

Beam(120 GeV p)

Glassmirror

Gas tank:C4F8O

and Argon

Beam Test of BTeV RICH

figures from T. Skwarnicki, presentation at DOE review of BTeVJ.C. Wang

R. MountainS. Blusk

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Looking Back• The CLEO-III/c RICH detector works well

• We all made it through a challenging project working beyond edge of demonstrated technology rising/falling of semiconductor industry learning curve in chambers, crystals, gas systems, electronics, … near-miss not choosing CsI or other photocathode

• I would like to express my gratitude and admiration for my coworkers at Syracuse, and those that followed to make the RICH a success.

• All of us grateful for the job Sheldon did supporting our research encouraging “discussion” spreading infectious enthusiasm maintaining focus providing “guidance” to young turks

• I wish Sheldon & Syracuse group many years of productive research