Recent advances in laser spectroscopy Iain Moore University of - - PowerPoint PPT Presentation

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Recent advances in laser spectroscopy Iain Moore University of - - PowerPoint PPT Presentation

Recent advances in laser spectroscopy Iain Moore University of Jyvskyl, Finland I.D. Moore, NUSTAR Week 2013, Helsinki, Finland Outline of talk A nuclear fingerprint in the atomic spectrum Collinear laser spectroscopy &


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SLIDE 1

Recent advances in laser spectroscopy

Iain Moore University of Jyväskylä, Finland

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 2
  • A nuclear fingerprint in the atomic spectrum
  • Collinear laser spectroscopy & extensions
  • Commissioning of the new IGISOL-4 facility
  • In-source and in-jet resonance ionization
  • Laser developments and a look to the future

Outline of talk

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 3

A nuclear fingerprint in the atomic spectrum

Sizes Spins Qs μ

Model Independent (measured) 20 μeV Isotope shift δ<r2> Isomer shift δ<r2> Hyperfine Splitting Model Dependent (inferred) Dynamic / static deformations Single / few particle configurations

Y+

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 4

40Zr

Radius of spherical nucleus of same volume Quadrupole deformation parameter

δ<r2>

z R θ

R = R0 ( 1 + β2 Y2,0 (θ,φ))

N=50 shell closure

Probing the deformation of nuclei

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 5

Between 1995 and 2010

(B. Cheal and K.T. Flanagan,

  • J. Phys. G 37 (2010) 113101)

Before 1995

(J. Billowes and P. Campbell,

  • J. Phys. G 21 (1995) 707)

Z N

Laser spectroscopy of radioisotopes - status

Z

Since 2010 Tl K (ISOLDE) Au Rb (TRIUMF) Cd (ISOLDE) Ac At

Recent work mostly by collinear laser spectroscopy Recent work mostly by in-source Resonance Ionization Spectroscopy (RIS)

Mn (JYFL/ISOLDE) Fr (TRIUMF – collinear) (ISOLDE – CRIS)

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 6

Workhorse: Collinear Laser Spectroscopy (CLS)

CW tunable laser beam (~1mW) Applied Doppler tuning voltage

PMT

Charge exchange (if required) Ion source Fast ion beam

ν ν0

Doppler broadened profile

rf cooler

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

  • W. Nörtershäuser et al., Phys. Rev. Lett. 102 (2009) 062503
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SLIDE 7

CLS on cooled and bunched beams

Ungated Gated (64-70 μs)

z

End plate potential Accumulate Release Reacceleration potential

Background suppression

50 ms/6 μs = ×104

Photon counts Ion counts

31Ga

  • E. Mané et al., PRC 84 (2011) 024303

Applied Doppler tuning voltage Background due to scattered light PMT Charge exchange

50 ms bunching

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 8

Tunable pulsed laser

Optical manipulation in the RFQ

  • J=0→J=1 gives μ, Q, δ<r2> but not I
  • Access to more accessible/efficient transitions
  • New elements to study (eg. Nb, Mn at JYFL)

IGISOL-3 layout

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

  • B. Cheal et al., Phys. Rev. Lett. 102 (2009) 222501
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SLIDE 9

Time of flight analysis

1+ ions 2+ ions

Cooler axis

(of single A,Z )

Multiple pulsed lasers (resonantly ionize 1+ → 2+)

Release Accumulate

Potential

(kicked away)

  • Ultra pure beam of single A and Z
  • No contaminant will have m/q selected by magnet

and m/(2q) selected by TOF (or other device)

Currently planned for 2014 at JYFL: Proposal B. Cheal

Ultra-pure beams: Ion Resonance Ionization

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 10

High frequency intensity modulation on bunched atom beams

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

Talk by A. Voss (JYFL/TRIUMF) @ 15:30 40 cm (~3µs transit time)

  • Intensity modulation of the laser light suppresses

hyperfine pumping in CLS of atoms

  • Demonstrated at TRIUMF on neutron deficient

206,205,204Fr

  • Immediately transferable to facilities, eg LaSpec
  • A. Voss et al., Phys. Rev. Lett. 111 (2013) 122501
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SLIDE 11

https://www.jyu.fi/fysiikka/en/research/accelerator/igisol

K=30 MeV cyclotron from K=130 MeV cyclotron

The new IGISOL-4 facility

Off-line ion sources: (discharge, carbon cluster…) Laser transport for optical manipulation/ IRIS Mass spectrometry & post-trap spectroscopy Collinear laser spectroscopy Laser ionization in-source/in-jet Decay spectroscopy

  • Fast extraction (~1 ms)
  • Chemically non-selective

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 12

104Mo

IGISOL-3 July 2008

104Mo

IGISOL-4 April 2013

Commissioning of the collinear beam line (2013)

Laser spectroscopy of neutron rich Mo fission fragments

(102-106,108Mo) F.C. Charlwood et al., Phys. Lett. B 674 (2009) 23

107Mo

IGISOL-4 April 2013

  • First “commissioning run”
  • Fission yields 2-3× higher than IG-3
  • 107Mo measured for the first time
  • Further optimisation planned

4d45s6D1/2 (11783 cm-1) → 4d45p6F1/2 (45853 cm-1) Penning traps Laser hut RFQ-buncher I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 13

~6 eV

(5-9 eV)

ground state first excited state higher excited states IP

E1

energy

0 eV E0

non-resonant ionization excitation of auto-ionizing states ionization of Rydberg-states extraction field or collisional ionization

Resonant laser ionization (spectroscopy)

σR: ~ 10-12 cm2 σΙ ~ 10-17 cm2 σΙ ~ 10-15 cm2 HOT CAVITY

  • ISOLDE, TRIUMF, GANIL,

ORNL, PNPI, ALTO, (SPES) GAS CELL

  • Leuven, JYFL, (PALIS)

SELECTIVITY & EFFICIENCY

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 14
  • Yu. Kudryavtsev et al., NIM B 267 (2009) 2908

Dual-chamber gas cell (Leuven/JYFL)

Laser beams Longitudinal

SPIG Ar/He from gas purifier

Ion Collector

Ionization chamber

Beam from Cyclotron Target Exit hole Ø 0.5 – 1 mm

17% 11% 2%

  • M. Reponen, I.D. Moore et al., NIMB (2013), doi:10.1016/j.nimb.2013.05.061

223Ra (τ1/2=11.4 d)

α-recoil source efficiencies Separation of stopping and laser ionization volume improves:

  • Laser ionization efficiency at

high cyclotron beam current

  • Increasing selectivity

(collection of non-neutral ions)

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

2013: 58Cu (τ½=3.2s)

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SLIDE 15

RIS in-source vs. collinear laser spectroscopy

Selective process Low lifetimes, low yields (<1 ion/s) High detection efficiency Poor resolution (100-1000× < CLS)

6-

68Cu

1+ 6- 722 β

β

  • I. Stefanescu et al., PRL 98 (2007) 122701

1+ (g.s.)

IN-SOURCE (RIS)

10000 15000 20000 25000 100 200 300 400 500 600 700 800

Counts Relative Frequency (MHz) 6- 1+

68Cu

  • P. Vingerhoets et al., PRC 82 (2010) 064311

COLLINEAR (FAST BEAMS)

High resolution Scanning voltage, not frequency Limited by detection method Beams of some 103 ions/s

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 16

Gas jet laser ionization – a tool for the future

  • a quest for PURE radioactive ion beams

→ (the Laser Ion Source ``Trap´´)

I.D. Moore et al., AIP Conf. Proc. 831 (2006) 511

2P3/2 2P1/2 2S1/2

Fj Fi

  • an optimal environment for spectroscopy

(reduced temperature and pressure)

F=J+I

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 17

0,00 0,03 0,06 0,09 0,12 1000 2000 3000 4000

  • 20
  • 10

10 20 100 200 300

Ion signal (arb. u.)

  • Ref. cell

Gas cell Gas jet (LIST)

ν - 915 423.95 (GHz)

First free jet ions in LIST geometry at JYFL

63Cu Vjet ~1040 m/s FWHM = 3.9(2) GHz FWHM = 6.7(3) GHz FWHM = 1.8(2) GHz

  • Employ special nozzles
  • Laser linewidth dominated

He, 180 mbar

I.D. Moore et al., NIMB (2013), doi:10.1016/j.nimb.2013.06.036

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 18

Collinear resonance ionization spectroscopy

Radioactive bunched ion beam from ISOLDE Stable beam from off line ion source Charge exchange cell Doppler tuning voltage applied PMT: fluorescence detection UHV interaction region MCP: ion detection Decay spectroscopy Si detectors Ge detectors Laser beam

202,203,204,205,207,211Fr 218,219, 220,221,229,231Fr

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

Talk by K. Flanagan (Manchester) @ 16:25

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SLIDE 19

Mode- matching telescope pulsed Nd-YAG pump laser

Attenuator fast piezo

Output to experiment (<20 MHz, 3W @10kHz)

TEM LaseLock digital

Injection-locked Ti:sa cavity

fast switched photodiode amplifier

  • ptical isolator

Ti:sa crystal

PSD

HV PD signal in

single mode fiber

Development of narrow-band pulsed Ti:sapphire lasers

Sirah Matisse TS cw-Ti:sa ~60 kHz linewidth

Glass plate

  • Similar developments at RIKEN/Nagoya and TRIUMF
  • RESIST Joint Research Activity for ENSAR 2

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

d = n λcw

1-150 mW

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SLIDE 20

Applications: high resolution spectroscopy

Spectroscopy of 229Th

1.5 GHz total width 3.5 GHz total width 1.5 GHz total width

Spectroscopy of 227Ac

6d7s2 J0=3/2 J1=3/2

227Ac

877.16 nm /2 = 438.58 nm 22 801.1 cm-1 424.7 nm 46347.0cm-1

  • V. Sonnenschein et al., J. Phys. B 45 (2012) 165005

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 21

Clusters and Halos Refractory Elements around Shell Closures Further away from stability Towards Superheavy Elements

Looking towards the future

A variety of techniques are used to probe the regions of interest New & future facilities

  • Becola (MSU)
  • TRIGASPEC (Mainz)
  • HELIOS@S3, GANIL
  • LaSpec at FAIR

I.D. Moore, NUSTAR Week 2013, Helsinki, Finland

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SLIDE 22

Thank you