Laser spectroscopy of actinides at the IGISOL facility, JYFL Iain - - PowerPoint PPT Presentation

laser spectroscopy of actinides at the igisol facility
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Laser spectroscopy of actinides at the IGISOL facility, JYFL Iain - - PowerPoint PPT Presentation

Laser spectroscopy of actinides at the IGISOL facility, JYFL Iain Moore University of Jyvskyl, Finland Outline Motivation for heavy element studies Laser ionization and spectroscopy of plutonium Comparison of RIS vs. collinear


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SLIDE 1

Laser spectroscopy of actinides at the IGISOL facility, JYFL

Iain Moore

University of Jyväskylä, Finland

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SLIDE 2

Outline

  • Motivation for heavy element studies
  • Laser ionization and spectroscopy of

plutonium

  • Comparison of RIS vs. collinear spec
  • Laser ionization of thorium – towards

the nuclear clock

  • Outlook

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 3

History: towards heavy & rare isotopes

  • Uranium is heaviest ISOL target
  • Need fusion reactions in HI collisions
  • Low production cross sections
  • Lack of stable isotopes – lack of
  • ptical transitions

In the 1950s, physicists and chemists expected it would be possible to deduce many properties of an element from a detailed knowledge of electronic

  • configurations. Transuranium elements (Np to Fm) could be bred in small

amounts in reactors, or from nuclear fallout. Huge spectrographs built: tens of thousands of atomic emission lines observed for each

  • actinide. Sample sizes 0.1 mg. Quite good info

available up to Es (Z=99)

30 m Argonne Paschen-Runge spectrometer

Tomkins & Fred, Spectr. Chem. Acta 6 (1954) 139

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 4
  • spin/parity known (without brackets!!)
  • even-even nuclei: 0+
  • source: NNDC (Tuli, Wallet cards)

100Fm 102No 98Cf 104Rf 96Cm 94Pu 92U 90Th 88Ra

Courtesy of Piet Van Duppen

Ground state nuclear structure

  • spin/parity

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 5

N.J. Stone, Nuclear Data Services, IAEA (2014)

100Fm 102No 98Cf 104Rf 96Cm 94Pu 92U 90Th 88Ra

…and for the magnetic moments?

  • M. Sewtz et al., Phys Rev Lett 90 (2003) 163002
  • H. Backe et al., Hyp. Int. 162 (2005) 3

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 6

Sizes Spins Shapes Magnetic

properties

frequency shifts

Nuclear properties

level splittings

Laser spectroscopy: a window to the nucleus

Laser frequency

I.D. Moore, Mustar Week 2016, York, UK

244Pu+ 242Pu+ 240Pu+ 239Pu+

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SLIDE 7

An overview of optical measurements for heavy nuclei

Md No

  • P. Campbell, I.D. Moore, and M.

Pearson, PPNP 86 (2016) 127 (UPDATED)

I.D. Moore, Mustar Week 2016, York, UK

Charting a new territory….

Laser spectroscopy of nobelium

  • B. Cheal
  • M. Laatiaoui et al., doi:10.1038/nature19345
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SLIDE 8

Resonance ionization spectroscopy (RIS)

20 mW 3 mW

Po (Z=84)

  • D. Fink et al., PRX 5 (2015) 011018

 Selective process  Short lifetimes, low yields (<1 ion/s)  High detection efficiency  Poor resolution (line broadening) F=J+I

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 9

High-resolution RIS of Pu at Mainz

I.D. Moore, Mustar Week 2016, York, UK

388 nm transition

  • V. Sonnenschein, PhD thesis, University of Jyväskylä (2015)

Atomic HF spectra: 238-242,244Pu Transition ``B´´: 5f67s2 7F1 → 5f67s7p

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SLIDE 10

In-gas laser ionization of Pu at JYFL

238-242,244Pu on tantalum substrate

(~1μm Ti on top): T~1000-1200°C

244Pu ~1016 atoms 239Pu ~2×1014 238Pu ~8×1012

I.D. Moore, Mustar Week 2016, York, UK

  • I. Pohjalainen, I.M. et al., NIMB 376 (2016) 233
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SLIDE 11

Layout of IGISOL-4 experimental area

Collinear laser beamline (Manchester/Liverpool) JYFLTRAP Penning trap mass spectrometer RF cooler-buncher (+optical manipulation) Cone trap

(Manchester)

Atom trap/BEC (UCL)

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 12

I.D. Moore, Mustar Week 2016, York, UK

Collinear spectroscopy of Pu+ at IGISOL

30-60kV

PMT

30-60kV PMT

5f67s2 8F1/2 → 5f57s2 6P1/2 (363 nm)

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SLIDE 13

Extraction of nuclear information

Calibration of atomic factors:

  • F385nm = -7.1(7) GHz/fm2
  • F388nm = -22.8(23) GHz/fm2
  • F363nm = +7.9(6) GHz/fm2

King plots of isotope shifts vs. δ<r2>

  • A. Voss et al., to be submitted to PRA (2016)

δ<r2> from optical and X-rays from muonic atoms Discrepancy seen between techniques – under discussion (complete error budget)

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 14

Christoph Düllman, JGU Mainz

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SLIDE 15

229mTh

ΔE ≈ 7.6 eV τ ≈ 25 mins?

3/2 [631] 5/2 [633]

229Th and the low-lying isomeric state

Impact

  • Nuclear clock
  • Gamma ray laser
  • Qubit
  • Test of fundamental

constants

  • NEET

ΔE ≈ 6.3 – 18.3 eV

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 16

Laser ionization of thorium at JYFL

I.D. Moore, Mustar Week 2016, York, UK

a) Identify and characterize the 229Th isomer transition b) Implement key components to operate a nuclear clock

OBJECTIVES:

232Th ~1015 atoms

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SLIDE 17

Characterizing the ionization scheme

26878.16 cm-1 38956.96 cm-1 AI 50980.96 cm-1 0 cm-1 IP 50867 cm-1 6d2 7s2 3F2

831.67 nm 827.987 nm 372.049 nm

  • Y. Liu and D. Stracener, NIMB 376 (2016) 233

λ1

Isat=1065(276) mW/cm2

λ1

Isat=4003(637) mW/cm2

λ2 λ3

I.D. Moore, Mustar Week 2016, York, UK

  • I. Pohjalainen et al., manuscript under preparation
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SLIDE 18

Mass separator scans (Th with Ti/Zr coatings)

232Th on tantalum

substrate (~1μm Ti on top): T~1800-2000°C

Laser on Laser off

I.D. Moore, Mustar Week 2016, York, UK

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SLIDE 19

Populating the isomer via 233U α decay

I.D. Moore, Mustar Week 2016, York, UK

  • 200 kBq 233UF4 evaporated onto 20 mm ɸ steel
  • ~10000 229Th α-recoil ions/s leaving source
  • α-recoil ions stopped in ultra-pure He gas
  • charge exchange forms 229Th3+

229Th3+?

A/q=76.3

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SLIDE 20

I.D. Moore, Laser 2016 Workshop, Poznan, 16 May 2016

Summary + Outlook

  • New programme of high-resolution laser spectroscopy on

actinide elements (ng of material)

  • HR-RIS and collinear laser spectroscopy on Pu isotopes:

comparison of techniques; extraction of HF factors and changes in mean-square charge radii; heaviest element using CLS to date

  • Preparations towards 239Pu ”target” – α-recoil source with 100%

branching ratio into 235mU isomeric state

  • Awaiting 229Th samples from Vienna – ground state hyperfine

template

  • 233U source from Munich – production of 229mTh isomer
  • On-line production – 232Th(p,p3n)229g,mTh at 50 MeV
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SLIDE 21

Thanks to all collaborators

  • n these projects

& for your attention 