Forward photon measurement and generic detector R&D Y. Kwon Yonsei Univ.

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Presentation transcript:

Forward photon measurement and generic detector R&D Y. Kwon Yonsei Univ.

Contents CGC-related  -physics at forward –Related to RHIC & LHC –Calculable from the 1 st principle. –To be addressed 5-10 years down the road. Relevant generic detector R&D –Si/W sandwich calorimeter –SiPM (Silicon photomultiplier) – 무엇보다 한국이 우수한 잠재력을 갖춘 영역에서

CGC-related  -physics at forward Application domain –Perturbative QCD :  QCD << p T, p T ~ Q s –High parton density at small x : bigger effect at forward/backward Parton kinematics –Projectile : large x (~valence quarks) –Target : Small x (~gluons  CGC) Study based on Jamal Jalilian-Marian’s work (PRD66(2002)014021, PRD66(2002)094014, PRD67(2003)074019, NPA753(2005)307)

Baseline prediction Forward hadron suppression –Jet quenching? –Parton coalescence model?

Direct  production in p+p  One of the best known QCD process… Hard photon : Higher order pQCD Soft photon : Initial/final radiation, Fragmentation function  Leading order diagram in perturbation theory Really? Motivation : Direct  production

A : Background field, Color Glass Condensate at small x Using reduction formalism, Baseline approach

in coordinate space and in the “singular” gauge. L. McLerran and R. Venugopalan, Phys. Rev. D59, (1999) U(z T ) : a unitary matrix containing the interactions between the quark and CGC.

 *(e + e - pair) measurement Motivation: Low p T : large  0,  background Internal conversion –Any source of real photons also emits virtual photons –Well known example:  Rate and m ee distribution calculable in QED (Kroll- Wada formula)  Hadron decays: m ee < M hadron  Essentially not such limit for point-like source.  0 Dalitz decay Improve signal-to-background ratio by measuring e + e - pairs with m ee > ~ M pion Compton

Extraction of  signal Interpret deviation from hadronic cocktail ( , , ,  ’,  ) as signal from virtual direct photons Extract fraction r with two-component fit Fit yields good  2 /NDF (13.8 / 10) Separately normalized to data at m ee < 30 MeV Fit range: 80 < m ee < 300 MeV

 Production vs  * production

Universality (DIS)

Dipole cross section Phenomenological models for the dipole cross sections… (baseline JIMWLK equations) Issues…

J. Jalilian-Marian, NPA753 (2005) p RHIC

Summary Forward  production at RHIC/LHC –Extension of pQCD possible –Extreme higher twist(large Q s ) and CGC. –Universality in dipole cross section (DIS & Forward  production) –Dipole cross section is not yet calculated from baseline JIMWLK equation, but models for it exist.

Generic detector R&D

6 inch fabrication line 17/32 한국의 잠재역량 8 inch fabrication line R&D environment 300 cm 2 ~ $ 500

FOCAL A compact sampling electromagnetic calorimeter – deals with large particle flux at forward – observes part of the energy deposited by particle for the optimized shower – measures key particles, e,  and  0, within small space – measures energy.

A compact EMCal, Si/W sandwich calorimeter 50 (GeV) electron 1 Moliere radius(~1.5cm)20 radiation length (4mm W~1 X 0 )

Silicon pad sensor Yonsei Nuclear Physics Lab.20 ground -

Preamp Injected signal Output signal

Cosmic muon test

24/32 KPS, Fall 2010 “A” Si/W calorimeter prototype

High sensitivity photon sensor (SiPM) ~ electrons for a photon in visible range

구조와 동작 V bias

Noise signal

24.5 (V) : Under breakdown

25.5 (V) : Breakdown ~18 (mV)

27.0 (V) : Over breakdown Cross talk? ~31 (mV)