From GRETINA to GRETA

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August 17, 2006 The Future of γ-ray Spectroscopy 1 From GRETINA to GRETA I-Yang Lee Lawrence Berkeley National Laboratory Workshop on “The Future of Gamma-ray Spectroscopy” August 17 - 18, 2006, Tallahassee, FL

Transcript of From GRETINA to GRETA

August 17, 2006 The Future of γ-ray Spectroscopy 1

From GRETINA to GRETA

I-Yang Lee

Lawrence Berkeley National Laboratory

Workshop on “The Future of Gamma-ray Spectroscopy”August 17 - 18, 2006, Tallahassee, FL

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Outline

• Short history• Case for GRETA in 2007 LRP• Simulation of GRETA performance• Schedule and cost of GRETA• Plan for the white paper

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GRETA in1996 Long Range Plan

“It seems possible to develop a gamma-ray detector array which would have a resolving power about a thousand times that of any array currently existing or planned. Such a detector (called GRETA) would consist of a spherical shell of highly segmented, tapered hexagonal Gedetectors, each of which would be able to locate a scattering point in three dimensions to an accuracy between 1 mm and 1 cm. The gamma ray could then be reconstructed using the energy and position of the interactions.”

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GRETA in 2002 Long Range Plan

“4π Gamma-ray tracking array -The detection of gamma-ray emissions from excited nuclei plays a vital and ubiquitous role in nuclear science. The physics justification for a 4π tracking array that would build on the success of Gammasphere is extremely compelling, spanning a wide range of fundamental questions in nuclear structure, nuclear astrophysics, and weak interactions. This new array would be a national resource that could be used at several existing stable- and radioactive-beam facilities, as well as at RIA.”

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The science case for GRETA

1996 LRP

• 1994 Conceptual design study• 1998 Workshop on GRETA physics (LBNL)• 2000 Workshop on GRETA physics (MSU)• 2000 Proposal for a 3-crystal module cluster peer reviewed and funded• 2001 Workshop on Gamma-ray tracking detectors for nuclear science (Lowell)• 2002 Gamma Ray Tracking Coordination Committee review meeting (ANL)

⇒ “A National Plan for the Development of Gamma-Ray Tracking Detectors in Nuclear Science”

• 2003 NSAC facility review ranked GRETA 1 in science, and 1 in readiness• 2003 Proposal for GRETINA reviewed and received CD0 – mission need

2002 LRP

Workshops on Equipment for Radioactive Beam Facility

Experimental Equipment for an advanced ISOL facilityBerkeley, California, July 23-25, 1998

Workshop on the Experimental Equipment for RIAOak Ridge, Tennessee, March 18-22, 2003

RIA Facility WorkshopEast Lansing, Michigan , March 9-13, 2004

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Goal and plan for the 2007 LRP

Re-endorse the science of GRETASupport the completion of GRETA

Produce a white paper to make our caseas input to the LRP writing group

This goal and plan supported by bothGRETINA Advisory CommitteeGRETINA Management Committee

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The case for GRETA

• The science case for it remains strong.• It is a major initiative for our field.• It will be an essential part of the future

‘RIA’ facility. • It establishes a world-class capability in the

US in the meantime. • We have made great progress in the

construction of GRETINA.• We are asking to complete what we started.

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Simulation

• Reaction kinematics– Beam properties, target thickness.– Three types of reaction : fusion, fragmentation, and 2-

body reaction.– Particle velocity and gamma ray direction, Doppler

broadening.• GRETA efficiency and peak-to-total ratio

– GEANT simulation– Tracking efficiency

• Spectrum– Scale conditions of existing experimental results :

energy resolution, efficiency, peak-to-total, coincidence fold.

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GRETA SimulationFirst hit distribution

Φ sinθ

θ

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Doppler correction

0.00%

0.50%

1.00%

1.50%

2.00%

2.50%

3.00%

0 30 60 90 120 150 180

Lab Angle (degree)

Res

olut

ion

anglevelocity

46Ar → 45Ar, 70 MeV/amuβ= 0.37Δθ=1.0º

Δβ = 0.025

GRETINAAngular coverage

Φ sinθ

θ

θ coverage4 modules at 58º3 modules at 90º

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Energy resolution Example 1

• Proton knockout reaction 46Ar → 45Ar, 70 MeV/A• GRETINA angular coverage = 37º - 115º (4@ 58º, 3@90º)• Target to detector distance = 185 mm

GRETINA Energy Resolution Factors Value

(RMS) Resolution (FWHM %)

Beam position on target Δx, Δy 0.85 mm 0.192 Target position Δz 0.85 mm 0.375 Particle angle Δθx, Δθy 0.74 mr 0.069 GRETINA position Δx, Δy, Δz 1 mm 0.496 Particle momentum Δp/p 0.042 % 0.013 Target thickness 188 mg/cm2 0.084 TOTAL 0.641

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Experiment simulation 1

Gamma-ray energy (2keV/chan)

30Na from 32Al Beam

30Na from 30Mg Beam

340

370410250

175

190

150

140

340

370410

250

175

770430 (3+--2+)

Simulation SeGA Simulation GRETINA

48 Ca → 30Mg → 30Na

Gamma-gamma coincidence

(NSCL dataE. Rodriguez-Vieitez et al.)

n-rich nuclei from secondary fragmentation reactions

4 × efficiency1/5 × Doppler width

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Experiment simulation 2

238U + 170Er 5.7 MeV/uGS + CHICO3 ·109 p/s (0.5 pna), 0.5 mg/cm2

3 days, γ−γ−γ

1n transfer 169Er

SimulationGS + CHICO

Simulation 170Er + 238U 5.7 MeV/u

GRETINA + SuperCHICO1n 3 ·109

GRETINA + SuperCHICO3n 3 ·109

GRETA + SuperCHICO6n 3 ·109

C.Y. Wu et al., PRC 70, 014313 (2004)

n-rich nuclei from transfer reactions

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Experiment simulation 3

Simulation GRETA, ε =0.25

4-fold, I=10-5

Simulation GS, ε =0.09

Simulation GS, ε =0.09

3-fold, I=10-4

3-fold, I=10-3

64Ni ( 48Ca, 4n) 108Cd, GammasphereA. Görgen et al., PRC 65, 027302 (2002)

v/c=0.04

High-spin states from fusion reactions

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GRETINA

A gamma-ray tracking array covering 1π solid angle.

28 36-fold segmented Ge crystals in 7 cryostats

All signals (1036 channels) are digitized at 100 MHz.

On-line analysis performs signal decomposition and tracking to give position, energy, and scattering sequence of interactions.

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Features of GRETINA

• Better position Resolution – 2 mm vs. 20 mm– High recoil velocity experiments

• Compactness – 1 π solid angle is comparable or better than Gammasphere in efficiency– Use with auxiliary detectors, recoil separators etc.

• Higher efficiency for high energy gamma rays– Giant resonances studies

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Possible installation sites

ANL FMA

NSCL S800

LBNL Cave 4C

ORNL RMS

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GRETINA milestones

Critical DecisionsCD0 : Mission need Aug. 2003

CD1 : Preliminary Baseline Range Feb. 2004

CD2A/CD3A : Start Constructionlong lead time items (Ge) June 2005

CD2B/CD3B : Start Construction July 2007

CD4 : Start of Operation Sept. 2010

CD0: Approve mission needCD1: Approve preliminary baseline range CD2: Approve performance baseline rangeCD3: Approve start of construction CD4: Approve start of operation

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ScheduleWBS Task Name

1 GRETINA1.1 Mechanical1.1.2 Design1.1.3 Production1.2 Detector Module1.2.1 Purchasing1.2.2 Test/Characterize Module 11.2.3 Test/Characterize Rest of Modules1.3 Electronics 1.3.2 Prototype 1.3.3 Production1.4 Computing Systems1.4.2 Prototype1.4.3 Production1.5 System Assembly1.5.1 Prototype 1.5.2 Production1.6 Project Management1.7 Environment and Safety1.12 Level 1 Milestones: Critical Decisions CD1 CD2A/3A CD2B/3B CD4

Complete test proc. and apparatusAward module contract

Complete mechanical subsystem

Complete test DSP moduleStart production DSP module

Award computer farm contract

Ready for prototype assemblyReady for final assembly

CD0

3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 32003 2004 2005 2006 2007 2008 2009 2010 2011

Phase A complete

Complete detector purchase

Complete design/draw. support structure

Complete acceptance mod. 1

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Detector schedule

Number of detectorsCalendar year

order receive

2005 1

2006 1

2007 4

2008 2 3

2009 3

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GRETA costAdditional cost beyond GRETINA

Redirected effort not includedCost ContingencyItem

$k rate $k Mechanical 1,000 25% 250Detector 23,000 15% 3,450Electronics 2,142 25% 536Computing 830 30% 249Assembly 200 25% 50Management 2,000 15% 300Environment and Safety 150 20% 30Total 29,322 17% 4865With contingency 34,187 With escalation 42,391

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GRETA Detector Schedule

0

5

10

15

20

25

30

35

2006 2007 2008 2009 2010 2011 2012 2013 2014 2015 2016

Calendar YearN

umbe

r of d

etec

tor

GRETINAGRETATotal

0

5

10

15

20

25

30

35

2006 2007 2008 2009 2010 2011 2012 2013 2014 2015

Calendar Year

Num

ber o

f det

ecto

r

GRETINAGRETATotal

Start 20102π 20124π 2016

Start 20082π 20114π 2014

Plan A Plan B

GRETA schedule will most likely be determined by fundingprofile and/or detector production capability

August 17, 2006 The Future of γ-ray Spectroscopy 23EC – NUPECC Meeting 9.3.06 J. Gerl GSI

2001 2003 2005 2007 2009 2011 2013 2015 2017

Preparatory phaseInvest: 6.5 M€Effort: 120 FTE

Well structured organization based on LoIs and MoUs

AGATA Cost and schedule

Construction phaseInvest: 50 M€Effort: 100 FTE

OperationCost: < 1 M€

TMR

I3 EURONS

EC FP7

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Outline of white paper

• Executive summary• Introduction• Science case• Technical feasibility• Cost estimates• Conclusion

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Schedule of white paper

• 8/17, finalize outline of science case, writing assignments.

• 10/2, complete first draft, send for review• 10/16, receive comments on first draft• 10/23, complete second draft, send for review by

‘outside’ reviewer, discussion at DNP meeting• 11/13, receive comments.• 12/4, Complete final version, start copy

production• January 07, Chicago town meeting

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Summary

• GRETINA is under construction, and is planned to be completed in 2010.

• Goal of this workshop is to produce a white paper for the 2007 long range plan process.• Refine and strengthen the science case• Obtain support to start the next step of GRETA

construction in 2008