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DESIR hall Stéphane Grévy CEN Bordeaux-Gradignan CS GANIL-SPIRAL2, 27/09/2013

DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

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Page 1: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

DESIR hall

Stéphane GrévyCEN Bordeaux-GradignanCS GANIL-SPIRAL2, 27/09/2013

Page 2: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

� Global optical design finished and presentedat EMIS2012, Japan. T. Kurtukian-Nieto et al., NIMB 2013, DOI: 10.1016/j.nimb.2013.07.066.

� Mechanical design and integration is almost ready.

� Dipoles already ordered. Delivery expected for May 2014. Expected field transversal homo-geneityof 10-5 over a zone of ± 150 mm around the

Status Report DESIR-HRS

geneityof 10 over a zone of ± 150 mm around thecentral beam trajectory. The design for the dipolesalso includes the possibility of easily changing magnetic edges to refine the minimization of aberrations.

� Manufacturing of other elements by CENBG.

� Expected working performance of the HRS considering misalignment and positioning precision of different elements : m/∆m =20,000 for a 3π mm mrad 60keV beam and energy spread ~eV.

� Due to the evolution of SPIRAL2 Project, a revaluation of the objectives at short- and mid-term will be done before the end of 2013 in coordination with the project leader and the SFRE team for operational consideration.

Page 3: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

DESIR beam lines

• 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m

• Inside hall (max.): fish-bone: L~40m

SP

IRA

L2 DESIR

entrance

S3

LIRATSPIRAL1

� Beam dynamics• Consolidated: first order• Inside hall: definition of optics will be done in

agreement with set-up and experiment requirements• Quadrupoles design is fixed• Deflectors design must be done• Errors calculation will restart soon

� Mechanical integration & transverse� Mechanical integration & transverse• Construction of a brick: quadrupoles

triplet+steerer by IPN, mounted downstream the GPIB at CENBG

• 2014: construction of a electrostatic deflector• Full integration of the S3 to DESIR transfer

beam line by 2014

Page 4: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

2- GPIB

3- Penning Trap

1- Ion SourcePIPERADE =

funded1.2 M€PIègede PEnningpour des noyaux RAdioactifsà DEsir

Purify (∆M/M~10-5 � isobaric separation)large samples (up to 106 pps) of exotic nucleiA

IM

� Ion Source + GPIB @ CENBGsimulations : design :

� Double Penning Trap @ CSNSM + MPIKsimulations : design :

� PIPERADE @ CENBG status: IS � running since march 2013, 25 nA

GPIB� mechanics ready, to be installed in june 2013

status : Penning � design under waymagnet� negociations with vendor under way

Page 5: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

Status of R&D at MLLTRAP Status of R&D at MLLTRAP

P.G. Thirolf, C. Weber, R. Meißner, P. Müller, S. S chulte-HeinemannLMU München

� R&D for in-trap ( αααα, conversion electron) decay spectroscopy:

(i) setup of ‘detector trap’ for α detection

- successful commissioning of home-built, UHV- and cryo-compatible Si strip detectors

Ileak < 200 pA/strip∆E/E ~ 21.7 keV 30x30 mm2

300 µm30 strips

- ongoing: characterization in magnetic field

(ii) tests with pixel detectors for electron detection (shake-off, conversion electrons)

- detector: RadEye® : developed for X-rays, suitable for (low-E) electrons ?

30 strips

- 512 x 1024 pixel: 48 x 48 µm2

- depletion depth 2 µm

- tunable electron source (0.1-6 keV) under construction) S. Schulte-Heinemann (2013)

J. Moazzami-Fallah, B.Sc. Thesis (2012), P. Müller, Ph.D. Thesis, in preparation.

Page 6: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

MultiMulti--Passage Spectrometer (MPS) Passage Spectrometer (MPS)

(A/q separator for charge-bred ions)

(benchmark ions: Xe52+, ε = 5 π mm mrad)

� R&D for MPS setup:

- ion-optical trajectory simulations (SIMION):

Xe 53+

B=1252 G

lens : +3700 Vfast-ramping (50 ms) 1.2 T dipole

top view

Charge separation:

recent publications:- C. Weber et al., Int. Jour. Mass Spectr., in print (2013), B. Blank et al., Int. Jour. Mass Spectr., in print (2013)- C. Weber et al., Nucl. Instr. Meth. B in print (2013), C. Weber et al., Hyp. Int., in preparation

� next to come: - design and manufacturing of steering mirrors and lenses- design and manufacturing of vacuum chamber

Xe 53+Xe 52+Xe 51+

lens: +2400 V

side view

Page 7: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

Multi Reflection Time-of-Flight Mass spectrometer

(MR ToF MS)

• Cutting edge technique for exotic isotopes with short T1/2mass resolving power > 105

mass measurement relative accuracy 10-6

Typical trapping time ~10mssee R. Wolf’s presentation

MR ToF MS project at GANIL/SPIRAL 2: mass separation and mass measurements for present and future low energy

experiments at LIRAT, S3, and DESIRCan be combined with PIPERADE at DESIR

Collaboration between GANIL, LPC Caen and Greifswald university

Page 8: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

Principle: mass separation by time-of-flight of ion bunchestrapped between two mirrors

Multi Reflection Time -of -Flight Mass spectrometer (MR ToF MS)

see R. Wolf’s presentationSeveral geometries benchmarked

Starting from ISOLTRAP’s simplified geometry~1m

Page 9: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

StatusConceptual design study from first SIMION and SIMBUCA

simulationsSimulated resolving power >105 achieved

Simulated space charge effects above 5 103 ions/bunch

BUT experimentally seen at Greifswald: space charge effect could bedealt with up to 104-105 ions/bunch

Multi Reflection Time-of-Flight Mass spectrometer (MR ToF MS)

Master thesis B. Kansal

dealt with up to 10 -10 ions/bunch

Some key components ordered

Indicative time plan2014: Detailed design, construction

2015-…: Commissionning at LIRAT and S3

PhD thesis P. Chauveau

Page 10: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

Hyperfine splitting

ground state

excited state

λ1scan resonant excitation step

422.7 nm

ionization potential

continuum

non-resonant ionization 1064 nm

λ2

Key results from commissioning experiments:• 9 new isotopes and 5 new isomeric states

studied, n-def down to 202Fr, n-rich up to 231Fr.

• Experimental efficiency of 1:100 measured for 202Fr based on an independent yield measurement.

����count resonantly produced ions: • highly efficient and background-free• current resolution ~ 1 GHz

(to be improved to < 100 MHz)

CRIS: Collinear Resonance Ionization Spectroscopy on Fr isotopes at ISOLDE

422.7 nm measurement.

• Factor of 1000 improvement in efficiency over previous attempt to demonstrate CRIS.

• A factor of 10 6 increase in sensitivity compared to previous laser spectroscopy measurements on 207-213Fr.

• Non-resonant ionization efficiency (leading to background counts) of less than 1:100000 thanks to UHV (to be improved)

• First demonstration of laser assisted nuclear decay spectroscopy on ultra-pure isomeric beam(K. Lynch et al., Hyp. Int. 216 (2013) 95

202gFr

202mFr

K. Flanagan et al., Phys. Rev. Lett., submitted

Page 11: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

First on-line laser spectroscopy experiment at the new IGISOL facility

104MoIGISOL 3July 2008

104MoIGISOL 4April 2013

107MoIGISOL 4April 2013

• First “commissioning run”• Already seeing improvements• 107Mo now measured• similar set-up under preparation for DESIR

Page 12: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

Decay γγγγ-ray Total Absorption Spectrometer (DTAS)accurate measurement of ββββ-strength distributions

J.L. Tain et al., IFIC-U.Surrey-CIEMAT-JYFL-GSI-PNPI

� 18x 15x15x25cm3 NaI(Tl) modules � Pb-SS shielding + support table for JYFL/DESIR ready

Total absorption 22Na spectrum� Working on gain

stabilization system: light-source + light-splitter + reference-detector

1-to-20 fiber-bundlesplitter

� Commissioning at JYFL 2013/2014

� Electronics + DACQ ready

Page 13: DESIR presentation 2013 · 2014. 10. 23. · DESIR beam lines • 3 lines: SPIRAL2/S3/LIRAT up to DESIR: L=117m • Inside hall (max.): fish-bone: L~40m SPIRAL2 DESIR entrance S3

D. Testov (PhD work) and Orsay-Dubna collaboration

Direct ββββ-delayed neutron emission measurement

of 82,83,84Ga with TETRA at ALTO

84GaT1/2=0.085s

84GeT1/2=0.954 s

84AsT1/2=4.2 s

83GeT1/2= 1.85 s

83AsT1/2=13.4 s

β-n

β-n

β

β

β

Pn(84Ge)=10.2(9) B.Pfeiffer et al. Prog. Nucl. Energy 41, 39 (2002)others: 10.8(6) , 9.5(20) , 9(3)

Pn(84Ga)=(49.8±4)%

TETRA detector at BEDO setup: - 4π neutron detector with 90 3He counters at 7 atm- measured eff. 63±5% (on line)- 4π beta detector- 1 Ge detector- movable tape

n

γ γ