Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via...

22
Nuclear Structure using Deep Inelastic and Transfer Reactions Partha Chowdhury University of Massachusetts Lowell

Transcript of Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via...

Page 1: Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via inelastic/transfer reactions • powerful technique complements fusion • accesses high

Nuclear Structure using

Deep Inelastic and Transfer Reactions

Partha Chowdhury University of Massachusetts Lowell

Page 2: Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via inelastic/transfer reactions • powerful technique complements fusion • accesses high

outline

Technique Physics Challenges Progress Status Outlook

Chowdhury ATLAS User Workshop May 15, 2014

Page 3: Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via inelastic/transfer reactions • powerful technique complements fusion • accesses high

N

Z J

the spectroscopic frontiers

A

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technique Complementarity : (in high-spin population with stable beam and target) -fusion-evaporation preferentially populates neutron- deficient nuclei -inelastic and transfer access stable to neutron-rich

Characteristics : -populates a wide variety of nuclei -Cross-sections competitive (or better) than fusion -complementary fragment provides identification

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Physics with inelastic/transfer reactions - Rich pioneering history at ATLAS - (narrow and personally biased recent examples here) - heavy and very heavy nuclei - A~180 region - yrast traps, K-isomers, limits of approximate symmetries, soft potentials, shape transitions - A~250 region - K-isomers, highest neutron orbitals, reduced pairing, higher order multipole shapes

Chowdhury ATLAS User Workshop May 15, 2014

Page 6: Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via inelastic/transfer reactions • powerful technique complements fusion • accesses high

•  Deep-inelastic collisions with pulsed 136Xe beams from ATLAS.

•  Various thick targets across four experiments (one more approved)

•  170Er, 174Yb, 175Lu, 176Lu, 185Re, 186W, 187Re and 192Os.

•  γ-γ-γ-time: 1/825 ns pulsing

•  γ-γ-clock: from 10/40µs up to 1/4s slow chopping.

Neutron-rich nuclei 170<A<190 : courtesy Greg Lane (ANU)

•  neutron-rich nuclei are only weakly populated •  huge backgrounds

•  many (many!) products •  intense target excitation

Requires Gammasphere and time correlations to pull them out.

• Focus on high-K isomers - purity of the K quantum number • Shape changes/transitions – triaxiality/hexadecapole • Astrophysical implications - 176Lu/180Ta, other fortuitous discoveries?

Chowdhury ATLAS User Workshop May 15, 2014

Page 7: Nuclear Structure using Deep Inelastic and Transfer Reactions · • nuclear structure via inelastic/transfer reactions • powerful technique complements fusion • accesses high

A~180 overview : courtesy Greg Lane (ANU)

New isomers/spectroscopy

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A~250 : connecting very heavy to superheavy Protons Neutrons

R.R. Chasman and I. Ahmad, Rev. Mod. Phys. 49, 833 (1977) Woods-Saxon

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complementary reaction mechanisms

209Bi (1450 MeV) on 248Cm 207Pb (1430 MeV) on 249Cf 208Pb (1430 MeV) on 244Pu

~15% above Coulomb barrier ATLAS + Gammasphere

backed targets

Inelastic and transfer reactions with radioactive targets Complement fusion-evaporation studies of Z>100 nuclei Follow same neutron orbitals into lower-Z isotones

Prior prompt spectroscopy in Cm, Pu using these techniques G. Hackman et. al., Phys. Rev. C 57, R1056 (1998) I. Wiedenhoever et al., PRL 83, 2143 (1999) K. Abu Saleem, Ph.D. thesis, Illinois Inst. of Tech. (2002)

Current program targets both prompt and

delayed spectroscopy

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Fusion Evaporation Deep Inelastic/Transfer N

Z

N ≥ 150 Nuclei

x

x x x x x x x

the highest neutron orbitals

x x

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Total Projection

Au

Cou

lex

Au

X-r

ays

Au

Cou

lex

Total Projection

388

keV

33

3 ke

V

249Cf decay transitions

388

keV

X-ray double gate

244Pu ~1 nCi

249Cf ~25 µCi

249Cf gsb

spectroscopic challenges : radioactive targets

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208Pb + 249Cf and Gammasphere

100 150 200 250 300 350 400 450 5000.0

2.0x106

4.0x106

6.0x106

8.0x106

1.0x107

388

keV

, 245 C

m

115 keV Cf X-ray

Energy (keV)

Cou

nts

Total Projection

279

keV

, Au

Cou

lex

100 150 200 250 300 350 400 450 5000.0

5.0x103

1.0x104

1.5x104

2.0x104

2.5x104

388

keV

, 245 C

m

115 keV Cf X-ray gated Projection

Energy (keV)

Cou

nts

100 150 200 250 300 350 400 450 500

0.0

5.0x102

1.0x103

1.5x103

388

keV

, 245 C

m

115/115 keV Cf X-ray gated Projection

Cou

nts

Energy (keV)

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Acknowledgments: John Greene and Irshad Ahmad for target prep and ANL in-house collaborators for ensuring beam was hitting target

spectroscopic challenges : radioactive targets

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S.K. Tandel et al., Phys. Rev. C 82, 041301 (R ) (2010)

X-γ and cross-coincidences with binary reaction partner High-spin studies at the highest oscillator shells

odd-A Cm (Z=96) and Cf (Z=98) 209Bi + 248Cm, 207Pb+ 249Cf

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Bands built on single-particle orbitals (N=151)

Single-particle orbitals H. Makii et al., PRC 76, 081301(R) (2007)

S.S. Hota (Ph.D. thesis, 2012)

to be published

S.K. Tandel et al., PRC 82, 041301

(R ) (2010)

Rotational Bands

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emerging systematics: N=151

πi13/2 and νj15/2 align at comparable frequencies

νj15/2 alignments blocked and unblocked

Experiments say protons align first

Cranking calculations say neutrons align first!

Inclusion of β6 deformation is important

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Bands built on ground state and excited states

Configurations from M1/E2 branching ratios

comprehensive data now available for N=150-154

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reduced neutron pairing

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orbitals from above the N=184 shell gap?

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154

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2009 evolving landscape : A~250 region

Chowdhury ATLAS User Workshop May 15, 2014

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evolving landscape : A~250 region 2013

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•  nuclear structure via inelastic/transfer reactions •  powerful technique complements fusion •  accesses high spins in neutron-rich nuclei •  radioactive targets and heavy beams for A~250 studies •  K-Isomer physics (not focused on here) •  emerging systematics of highest neutron orbitals •  competing nucleon alignments •  higher order multipole deformation •  reduced neutron pairing at the N=152 gap •  orbitals from above the N=184 spherical gap?

status summary

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•  data on odd-proton nuclei sorely lacking •  (both for inelastic/transfer as well as fusion) •  A~250 proton transfer yields much lower than in A~180 •  explore limits of radioactive target experiments •  heavy radioactive beams ?? •  N~150 factory ???

near future outlook

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S. S. Hota.1, P. Chowdhury1, T.L. Khoo2, M.P. Carpenter2, R.V.F. Janssens2, I. Ahmad2, J. Greene2, S.K. Tandel1,3,

D. Seweryniak2, S. Zhu2, P. Bertone2, C.J. Chiara2,4, A. Y. Deo1, N. D’Olympia1, C. J. Guess1, G. Henning2, C.R. Hoffman2,

E. G. Jackson1, F.G. Kondev2, S. Lakshmi1, T. Lauritsen2, C.J. Lister1, E.A. McCutchan, V. S. Prasher1, Y. Qiu1,

U. Shirwadkar1, I. Stefanescu2

1University of Massachusetts Lowell 2Argonne National Laboratory

3Centre for Excellence in Basic Sciences

4University of Maryland

Collaborators for A~250 experiments

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