Nuclear Isomerism. Phil Walker. University of Surrey. on the occasion of the 70th birthday of Geirr Sletten

Size: px
Start display at page:

Download "Nuclear Isomerism. Phil Walker. University of Surrey. on the occasion of the 70th birthday of Geirr Sletten"

Transcription

1 Nuclear Isomerism Phil Walker University of Surrey on the occasion of the 70th birthday of Geirr Sletten

2 Nuclear Isomerism Phil Walker University of Surrey on the occasion of the 70th birthday of Geirr Sletten HAPPY BIRTHDAY GEIRR!!

3 What are isomers?

4 What are isomers? 1917: predicted by Soddy "different in their stability" 1921: uranium-x isomers observed by Hahn 1936: isomers explained as spin traps by von Weizsäcker excited nuclear states with long half-lives: > 1 ns

5 Why study isomers?

6 Why study isomers? At the limits of nuclear binding, isomers may be more stable than ground states.

7 Why study isomers? At the limits of nuclear binding, isomers may be more stable than ground states. 270 Ds α decay ms isomer at 1 MeV 0.1 ms ground state Hofmann et al., Eur. Phys. J. 10 (2001) 5 Xu et al., Phys. Rev. Lett. 92 (2004)

8 Why study isomers? At the limits of nuclear binding, isomers may be more stable than ground states. 270 Ds α decay ms isomer at 1 MeV 159 Re p decay µs isomer 0.1 ms ground state ground state unknown Hofmann et al., Eur. Phys. J. 10 (2001) 5 Xu et al., Phys. Rev. Lett. 92 (2004) Joss et al., Phys. Lett. B641 (2006) 34 Liu et al., Phys. Rev. C76 (2007)

9 Why study isomers? At the limits of nuclear binding, isomers may be more stable than ground states. KEY ROLE OF ANGULAR-MOMENTUM MAGNITUDE AND DIRECTION 270 Ds α decay ms isomer at 1 MeV 159 Re p decay µs isomer 0.1 ms ground state ground state unknown Hofmann et al., Eur. Phys. J. 10 (2001) 5 Xu et al., Phys. Rev. Lett. 92 (2004) Joss et al., Phys. Lett. B641 (2006) 34 Liu et al., Phys. Rev. C76 (2007)

10 A RECENT PHOTO

11 A USED TARGET

12 Chart of nuclides adapted from Lund web site

13 SLETTEN'S CHART

14 SLETTEN'S CHART

15 SLETTEN'S CHART

16 SLETTEN'S CHART

17 > 100 citations 1969

18 fission isomers 1969

19 1977 N ~ 82 isomers 16 NaI > 100 citations

20 1984 SATURN'S RINGS 14 NaI + 4 Ge(Li)

21 1984 SATURN'S RINGS 14 NaI + 4 Ge(Li)

22 1984 SATURN'S RINGS 14 NaI + 4 Ge(Li)

23 1985

24 10 NaI + 2 Ge(Li) (one suppressed) 1985

25 Os > 70 citations

26 1988 T 1/2 = 130 ns 6-quasiparticle isomer at 7 MeV bypassing 182-Os TESSA 3 (50 BGO + 12 Ge suppressed) with bunched beam of 36 S I beam current: on 5 ns off 200 ns time

27 counts gamma-ray coincidence spectrum 1988 bypassing ns 182-Os

28 isomer decay 1988

29 175-Hf 1990

30 9-quasiparticle isomer at 7.5 MeV ESSA 30 (30 Ge suppressed) recoil shadow τ > 10 ns 175 Hf 9-qp isomer 7455 kev bypassing 1990 bunched 48 Ca beam 7-qp 5-quasiparticle isomer at 3 MeV 3015 kev

31 175 Hf 175 Hf above 57/2 rotational bands based on 9-qp states Kondev et al., to be published Gammasphere 100 Ge suppressed "analysis of a number of high-seniority bands shows that they behave as if the nuclei rotate in the unpaired state" Frauendorf, Neergard, Sheikh, Walker, PRC61 (2000)

32 bypassing transitions nuclide K π bypassing quasiparticle intensity change 182 Os % Hf % Hf 57/2 >50 % W 35/2 95 % 5 1

33 bypassing transitions nuclide K π bypassing quasiparticle intensity change 182 Os % S 174 Hf % S 175 Hf 57/2 >50 % S 179 W 35/2 95 % S Do we understand the K-composition of S-bands? i.e. do we understand the orientation of the angular-momentum vector?

34 179-W 1983

35 W bypassing 14 NaI + 4 Ge(Li)

36 1983 bypassing 179-W

37 1983 bypassing 31/2 179-W

38 t-band K = 23/2 = bandhead spin W CAESAR: 6 Ge suppressed bunched and chopped beam Walker et al. PRL67 (1991) 433

39 W bands 174 W GAMMASPHERE bandhead? not an isomer K unknown [Tandel et al., Phys. Rev. C73 (2006) ]

40 174 W B(E2) ratios 2006 E2 transitions g s [Tandel et al., Phys. Rev. C73 (2006) ]

41 174 W B(E2) ratios 2007 K s = 8 ± 1 E2 transitions g s Walker, J. Phys. G34 (2007) 123

42 assume equal Q 0 s 2007 if K 1 = K 2, then c = 1, and R[B(E2)] s = R[B(E2)] g

43 174 W, K = 8 bandhead? 184 Os, K = 10 isomer bandhead 2007 full line: K = Ω <K s > 1 + Ω vs 2 for 2 i N 13/2 neutrons even-even nuclides K = Ω 1 Ω 2 Walker, J. Phys. G34 (2007) 123

44 174 W, K = 8 bandhead? 184 Os, K = 10 isomer bandhead 2007 full line: K = Ω <K s > 1 + Ω vs 2 for 2 i N 13/2 neutrons even-even nuclides high-k band crossings! K = Ω 1 Ω 2 Walker, J. Phys. G34 (2007) 123

45 Summary Types of isomerism: shape isomers, spin traps, K isomers Technical developments: recoil shadow, beam pulsing, detector arrays K-forbidden transitions: importance of t-bands

46 Summary Types of isomerism: shape isomers, spin traps, K isomers Technical developments: recoil shadow, beam pulsing, detector arrays K-forbidden transitions: importance of t-bands KEY ROLE OF ANGULAR-MOMENTUM MAGNITUDE AND DIRECTION

47 Summary Types of isomerism: shape isomers, spin traps, K isomers Technical developments: recoil shadow, beam pulsing, detector arrays K-forbidden transitions: importance of t-bands KEY ROLE OF ANGULAR-MOMENTUM MAGNITUDE AND DIRECTION Thank you, Geirr, for many years of friendship and physics!

48 KEY ROLE OF ANGULAR-MOMENTUM MAGNITUDE AND DIRECTION "what I tell you three times is true" from Lewis Carroll, The Hunting of the Snark

49 Saturn's rings!!

50 K values at bandcrossings Walker, J. Phys. G34 (2007) 123

51 quotes [Narimatsu et al., Nucl. Phys. A601 (1996) 69] for 172 Hf (N = 100) [Cullen et al., Nucl. Phys.A638 (1998) 662] for 174 W (N = 100) [Tandel et al., Phys. Rev. C73 (2006) ]

52 172 Hf yrast band I i = Q 0 (eb) [Cullen et al., Nucl. Phys.A638 (1998) 662] ħω (MeV)

53 172 Hf yrast band I i = Q 0 (eb) ħω (MeV) corrected for K = [Cullen et al., Nucl. Phys.A638 (1998) 662]

54 Jain odd-n systematics [Jain et al., Rev. Mod. Phys. 62 (1990) 393]

55 TIDAL WAVES 182-Os isomer rotation

and shape coexistence

and shape coexistence Aspects University of nuclear of Surrey isomerism and shape coexistence - historical introduction - energy storage - enhanced stability - high-k isomers - neutron-rich A 190 isomers Phil Walker Isomer

More information

Nuclear isomers: stepping stones to the unknown

Nuclear isomers: stepping stones to the unknown Nuclear isomers: stepping stones to the unknown P.M. Walker Department of Physics, University of Surrey, Guildford GU2 7XH, UK Abstract. The utility of isomers for exploring the nuclear landscape is discussed,

More information

K-isomer decay rates. Phil Walker. - introduction - exploring the different degrees of freedom - exotic nuclei

K-isomer decay rates. Phil Walker. - introduction - exploring the different degrees of freedom - exotic nuclei K-isomer decay rates Phil Walker - introduction - exploring the different degrees of freedom - exotic nuclei Segre chart with isomers K isomers in deformed nuclei adapted from Walker and Dracoulis, Nature

More information

ISOMER BEAMS. P.M. WALKER Department of Physics, University of Surrey, Guildford GU2 7XH, UK

ISOMER BEAMS. P.M. WALKER Department of Physics, University of Surrey, Guildford GU2 7XH, UK International Journal of Modern Physics E c World Scientific Publishing Company ISOMER BEAMS P.M. WALKER Department of Physics, University of Surrey, Guildford GU2 7XH, UK p.@surrey.ac.uk Received (received

More information

arxiv:nucl-th/ v1 19 May 2004

arxiv:nucl-th/ v1 19 May 2004 1 arxiv:nucl-th/0405051v1 19 May 2004 Nuclear structure of 178 Hf related to the spin-16, 31-year isomer Yang Sun, a b Xian-Rong Zhou c, Gui-Lu Long, c En-Guang Zhao, d Philip M. Walker 1e a Department

More information

and 14 + isomers in 175,176 W

and 14 + isomers in 175,176 W 14 December 000 Physics Letters B 495 (000) 89 94 www.elsevier.nl/locate/npe g factors of the and 14 + isomers in 15,16 W M. Ionescu-Bujor a,, A. Iordachescu a,f.brandolini b,m.depoli c,n.mǎrginean a,c,

More information

High-spin isomers: structure and applications

High-spin isomers: structure and applications High-spin isomers: structure and applications P.M. Walker a a Department of Physics, University of Surrey, Guildford GU2 7XH, United Kingdom High-spin-isomer research is briefly reviewed, with attention

More information

Shape Effects in E2 Transition Rates from Z 76 High-Spin Isomers

Shape Effects in E2 Transition Rates from Z 76 High-Spin Isomers Bulg. J. Phys. 44 (2017) 427 433 Shape Effects in E2 Transition Rates from Z 76 High-Spin Isomers Department of Physics, University of Surrey, Guildford GU2 7XH, United Kingdom Received 30 September 2017

More information

K-hindered decay of a six-quasiparticle isomer in 176 Hf

K-hindered decay of a six-quasiparticle isomer in 176 Hf K-hindered decay of a six-quasiparticle isomer in 176 Hf G. Mukherjee 1, P. Chowdhury 1, F.G. Kondev 2, P.M. Walker 3, G.D. Dracoulis 4, R. D Alarcao 1, I. Shestakova 1, K. Abu Saleem 2, I. Ahmad 2, M.P.

More information

Isomers in Heavy Deformed Nuclei

Isomers in Heavy Deformed Nuclei Isomers in Heavy Deformed Nuclei P. Chowdhury* Department of Physics, University of Massachusetts Lowell, Lowell MA 01854, USA. *email: partha_chowdhury@uml.edu The talk provides an overview of K-isomer

More information

Spectroscopy of fission fragments using prompt-delayed coincidence technique

Spectroscopy of fission fragments using prompt-delayed coincidence technique PRAMANA c Indian Academy of Sciences Vol. 85, No. journal of September 5 physics pp. 95 Spectroscopy of fission fragments using prompt-delayed coincidence technique RPALIT and S BISWAS Department of Nuclear

More information

Nuclear Isomers: What we learn from Tin to Tin

Nuclear Isomers: What we learn from Tin to Tin INDIAN INSTITUTE OF TECHNOLOGY ROORKEE Nuclear Isomers: What we learn from Tin to Tin Ashok Kumar Jain Bhoomika Maheshwari Department of Physics Outline Nuclear Isomers The longest chain of Sn isotopes

More information

Quadrupole moment of the K π = 14 + isomer in 176 W

Quadrupole moment of the K π = 14 + isomer in 176 W Physics Letters B 541 (00) 19 6 www.elsevier.com/locate/npe Quadrupole moment of the K π = 14 + isomer in 176 W M. Ionescu-Bujor a, A. Iordachescu a,f.brandolini b,m.depoli c,n.mǎrginean a,c, D. Bucurescu

More information

High-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes

High-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes High-spin studies and nuclear structure in three semi-magic regions of the nuclide chart High-seniority states in Sn isotopes Outline: Alain Astier, CSNSM Orsay, France Motivations Experimental conditions

More information

arxiv:nucl-th/ v1 14 Nov 2005

arxiv:nucl-th/ v1 14 Nov 2005 Nuclear isomers: structures and applications Yang Sun, Michael Wiescher, Ani Aprahamian and Jacob Fisker Department of Physics and Joint Institute for Nuclear Astrophysics, University of Notre Dame, Notre

More information

Evidence for K mixing in 178 Hf

Evidence for K mixing in 178 Hf Hyperfine Interactions 107 (1997) 141^147 141 Evidence for K mixing in 178 Hf C.B. Collins The University of Texas at Dallas, Center for Quantum Electronics, PO Box 830688, Richardson, TX 75083-0688, USA

More information

Gamma-ray spectroscopy I

Gamma-ray spectroscopy I Gamma-ray spectroscopy I Andreas Görgen DAPNIA/SPhN, CEA Saclay F-91191 Gif-sur-Yvette France agoergen@cea.fr Lectures presented at the IoP Nuclear Physics Summer School September 4 17, 2005 Chester, UK

More information

Search for very long-lived isomers in the hafnium-tungsten region

Search for very long-lived isomers in the hafnium-tungsten region Search for very long-lived isomers in the hafnium-tungsten region Zs. Podolyák, 1 P. M. Walker, 1 D. M. Cullen, 2 G. D. Dracoulis, 3 P. Fallon, 4 B. Fairchild, 4 K. Hauschild, 5 A. O. Macchiavelli, 4 D.

More information

Recent results from digital INGA at BARC TIFR Pelletron Linac Facility and future plans

Recent results from digital INGA at BARC TIFR Pelletron Linac Facility and future plans PRAMANA c Indian Academy of Sciences Vol. 83, No. 5 journal of November 214 physics pp. 719 728 Recent results from digital INGA at BARC TIFR Pelletron Linac Facility and future plans RPALIT Tata Institute

More information

Symmetries and collective Nuclear excitations PRESENT AND FUTURE EXOTICS IN NUCLEAR PHYSICS In honor of Geirr Sletten at his 70 th birthday

Symmetries and collective Nuclear excitations PRESENT AND FUTURE EXOTICS IN NUCLEAR PHYSICS In honor of Geirr Sletten at his 70 th birthday Symmetries and collective Nuclear excitations PRESENT AND FUTURE EXOTICS IN NUCLEAR PYSICS In honor of Geirr Sletten at his 70 th birthday Stefan Frauendorf, Y. Gu, Daniel Almehed Department of Physics

More information

Gamma spectroscopy in the fermium region at SHIP

Gamma spectroscopy in the fermium region at SHIP Nuclear Structure Physics with Advanced Gamma- Detector Arrays, Padova June 10-12, 2013 Gamma spectroscopy in the fermium region at SHIP Stanislav Antalic Comenius University, Bratislava Collaboration

More information

A Comparison between Channel Selections in Heavy Ion Reactions

A Comparison between Channel Selections in Heavy Ion Reactions Brazilian Journal of Physics, vol. 39, no. 1, March, 2009 55 A Comparison between Channel Selections in Heavy Ion Reactions S. Mohammadi Physics Department, Payame Noor University, Mashad 91735, IRAN (Received

More information

High-spin states in 90 Ru and the projected shell model description

High-spin states in 90 Ru and the projected shell model description PHYSICAL REVIEW C 69, 064319 (2004) High-spin states in 90 Ru and the projected shell model description D. Bucurescu, 1 N. Mărginean, 2,1 C. Rossi Alvarez, 3 Y. Sun, 4,5 C. A. Ur, 3,1 L. C. Mihăilescu,

More information

Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy.

Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy. Probing neutron-rich isotopes around doubly closed-shell 132 Sn and doubly mid-shell 170 Dy by combined β-γ and isomer spectroscopy Hiroshi Watanabe Outline Prospects for decay spectroscopy of neutron-rich

More information

Projected shell model analysis of tilted rotation

Projected shell model analysis of tilted rotation PHYSICAL REVIEW C VOLUME 57, NUMBER 1 JANUARY 1998 Projected shell model analysis of tilted rotation J. A. Sheikh, 1.2 Y. Sun, 3,4,5 and P. M. Walker 1 1 Department of Physics, University of Surrey, Surrey,

More information

Exploring the Structure of Cold and Warm Nuclei Using Particle Accelerators in India

Exploring the Structure of Cold and Warm Nuclei Using Particle Accelerators in India Exploring the Structure of Cold and Warm Nuclei Using Particle Accelerators in India GOPAL MUKHERJEE VARIABLE ENERGY CYCLOTRON CENTRE, KOLKATA ABSTRACT The Indian National Gamma Array (INGA) and the VECC

More information

Identification of yrast high-k isomers in 177 Lu and characterisation of 177m Lu

Identification of yrast high-k isomers in 177 Lu and characterisation of 177m Lu Physics Letters B 584 (2004) 22 30 www.elsevier.com/locate/physletb Identification of yrast high-k isomers in 177 Lu and characterisation of 177m Lu G.D. Dracoulis a, F.G. Kondev b,g.j.lane a,a.p.byrne

More information

Lifetime Measurement in 103,104 Rh with RDDS Method in Inverse Kinematics: A Test for Nuclear Chirality. Suzuki Tomokazu

Lifetime Measurement in 103,104 Rh with RDDS Method in Inverse Kinematics: A Test for Nuclear Chirality. Suzuki Tomokazu Lifetime Measurement in 3,4 with RDDS Method in Inverse Kinematics: A Test for Nuclear Chirality Suzuki Tomokazu Research Center for Nuclear Physics, Osaka University T. Koike, G. Rainovski,3,T.Ahn 3,M.Carpenter

More information

Some Aspects of Nuclear Isomers and Excited State Lifetimes

Some Aspects of Nuclear Isomers and Excited State Lifetimes Some Aspects of Nuclear Isomers and Excited State Lifetimes Lecture 2: at the Joint ICTP-IAEA Workshop on Nuclear Data : Experiment, Theory and Evaluation Miramare, Trieste, Italy, August 2016 Paddy Regan

More information

Conversion Electron Spectroscopy in Transfermium Nuclei

Conversion Electron Spectroscopy in Transfermium Nuclei Conversion Electron Spectroscopy in Transfermium Nuclei R.-D. Herzberg University of iverpool, iverpool, 69 7ZE, UK Abstract Conversion electron spectroscopy is an essential tool for the spectroscopy of

More information

Highly deformed Bands in 175 Hf

Highly deformed Bands in 175 Hf PHYSICAL REVIEW C 70, 054314 (2004) Highly deformed Bands in 175 Hf D. T. Scholes, 1 D. M. Cullen, 1 F. G. Kondev, 2 R. V. F. Janssens, 3 M. P. Carpenter, 3 D. J. Hartley, 4, * M. K. Djongolov, 5 G. Sletten,

More information

New theoretical insights on the physics of compound nuclei from laser-nucleus reactions

New theoretical insights on the physics of compound nuclei from laser-nucleus reactions New theoretical insights on the physics of compound nuclei from laser-nucleus reactions Adriana Pálffy Max Planck Institute for Nuclear Physics, Heidelberg, Germany Laser-Driven Radiation Sources for Nuclear

More information

Radioactivity at the limits of nuclear existence

Radioactivity at the limits of nuclear existence Radioactivity at the limits of nuclear existence Zenon Janas Institute of Experimental Physics University of Warsaw Chart of nuclei - stable - β + - β - - α - fission - p p and 2p radioactivty proton radioactivity

More information

Some (more) High(ish)-Spin Nuclear Structure. Lecture 2 Low-energy Collective Modes and Electromagnetic Decays in Nuclei

Some (more) High(ish)-Spin Nuclear Structure. Lecture 2 Low-energy Collective Modes and Electromagnetic Decays in Nuclei Some (more) High(ish)-Spin Nuclear Structure Lecture 2 Low-energy Collective Modes and Electromagnetic Decays in Nuclei Paddy Regan Department of Physics Univesity of Surrey Guildford, UK p.regan@surrey.ac.uk

More information

Collective Excitations in Exotic Nuclei

Collective Excitations in Exotic Nuclei Collective Excitations in Exotic Nuclei David Radford (ORNL) RIA Summer School, August 2002 I Nuclear Excitations: Single particle motion vs. Collective motion Collective Modes: Rotations and Vibrations

More information

Low-spin structure of 210 Bi

Low-spin structure of 210 Bi Low-spin structure of 21 Bi investigated in cold-neutron capture reaction on 29 Bi Natalia Cieplicka, S. Leoni, B. Fornal INFN, Sezione di Milano 5th orkshop on Nuclear Level Density and Gamma Strength,

More information

Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation August Experimental Nuclear Physics: Part 2

Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation August Experimental Nuclear Physics: Part 2 2358-11 Joint ICTP-IAEA Workshop on Nuclear Structure Decay Data: Theory and Evaluation 6-17 August 2012 Experimental Nuclear Physics: Part 2 E. Ricard McCutchan Brookhaven National Lab. USA Experimental

More information

Electromagnetic modulation of monochromatic neutrino beams

Electromagnetic modulation of monochromatic neutrino beams Journal of Physics: Conference Series PAPER OPEN ACCESS Electromagnetic modulation of monochromatic neutrino beams To cite this article: A L Barabanov and O A Titov 2016 J. Phys.: Conf. Ser. 675 012009

More information

GRETINA at ATLAS. (and GRETA Too!!) C.J. (Kim) Lister Gretina / Greta Pre-Town Meeting F.S.U. August th 2006

GRETINA at ATLAS. (and GRETA Too!!) C.J. (Kim) Lister Gretina / Greta Pre-Town Meeting F.S.U. August th 2006 GRETINA at ATLAS (and GRETA Too!!) C.J. (Kim) Lister Gretina / Greta Pre-Town Meeting F.S.U. August 17-18 th 2006 Overview Philosophy Where is our field of nuclear structure going? What role does gamma-ray

More information

Yrast and near-yrast excitations up to high spin in Cd 52

Yrast and near-yrast excitations up to high spin in Cd 52 PHYSICAL REVIEW C, VOLUME 61, 044311 Yrast and near-yrast excitations up to high spin in 100 48 Cd 52 R. M. Clark, 1 J. N. Wilson, 2, * D. Appelbe, 3 M. P. Carpenter, 4 C. J. Chiara, 5 M. Cromaz, 1 M.

More information

Chapter 6. Summary and Conclusions

Chapter 6. Summary and Conclusions Chapter 6 Summary and Conclusions The basic aim of the present thesis was to understand the interplay between single particle and collective degrees of freedom and underlying nuclear phenomenon in mass

More information

Review of Metastable States in Heavy Nuclei

Review of Metastable States in Heavy Nuclei Review of Metastable States in Heavy Nuclei G. D. Dracoulis Department of Nuclear Physics, R.S.P.E. Australian National University, Canberra, A.C.T. 0200, Australia P. M. Walker Department of Physics,

More information

Investigation of Pygmy Dipole Resonance in neutron rich exotic nuclei

Investigation of Pygmy Dipole Resonance in neutron rich exotic nuclei Investigation of Pygmy Dipole Resonance in neutron rich exotic nuclei R.Avigo 1,2, O.Wieland 1, A.Bracco 1,2, F.Camera 1,2 on behalf of the AGATA and DALI2 collaborations 1 INFN, sezione di Milano 2 Università

More information

What do we know experimentally about the N=149, N=151 and N=153 isotones?

What do we know experimentally about the N=149, N=151 and N=153 isotones? What do we know experimentally about the N=149, N=151 and N=153 isotones? - Introduction - Experimental review - Issues & questions - Conclusions A. Lopez-Martens Region of interest 118 117 1.8 ms 11.65

More information

High Spin States in Nuclei: Exotic Quantal Rotation III. Umesh Garg. University of Notre Dame. Supported in part by the National Science Foundation

High Spin States in Nuclei: Exotic Quantal Rotation III. Umesh Garg. University of Notre Dame. Supported in part by the National Science Foundation High Spin States in Nuclei: Exotic Quantal Rotation III Umesh Garg University of Notre Dame Supported in part by the National Science Foundation CNSSS17 August 23-29, 2017 u normal collective rotation

More information

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics Nuclear Physics and Astrophysics PHY-302 Dr. E. Rizvi Lecture 13 - Gamma Radiation Material For This Lecture Gamma decay: Definition Quantum interpretation Uses of gamma spectroscopy 2 Turn to γ decay

More information

Nuclear and Radiation Physics

Nuclear and Radiation Physics 501503742 Nuclear and Radiation Physics Why nuclear physics? Why radiation physics? Why in Jordan? Interdisciplinary. Applied? 1 Subjects to be covered Nuclear properties. Nuclear forces. Nuclear matter.

More information

Sunday Monday Thursday. Friday

Sunday Monday Thursday. Friday Nuclear Structure III experiment Sunday Monday Thursday Low-lying excited states Collectivity and the single-particle degrees of freedom Collectivity studied in Coulomb excitation Direct reactions to study

More information

New data on β decay of exotic nuclei close to 100 Sn:

New data on β decay of exotic nuclei close to 100 Sn: New data on β decay of exotic nuclei close to 1 Sn: 94 Ag and 1 In C. Plettner 1, I. Mukha 1, J. Döring 1, L. Batist 2, H. Grawe 1, A. Blazhev 1,3, C. R. Hoffman 4, Z. Janas 5, R. Kirchner 1, M. La Commara

More information

DSAM lifetime measurements for the chiral bands in 194 Tl

DSAM lifetime measurements for the chiral bands in 194 Tl Journal of Physics: Conference Series PAPER OPEN ACCESS DSAM lifetime measurements for the chiral bands in 194 Tl To cite this article: P L Masiteng et al 2016 J. Phys.: Conf. Ser. 724 012028 Related content

More information

Discovery of highly excited long-lived isomers in neutron-rich hafnium and tantalum isotopes through direct mass measurements

Discovery of highly excited long-lived isomers in neutron-rich hafnium and tantalum isotopes through direct mass measurements Discovery of highly excited long-lived isomers in neutron-rich hafnium and tantalum isotopes through direct mass measurements M.W. Reed, 1, I.J. Cullen, 1 P.M. Walker, 1 Yu.A. Litvinov, 2, 3 K. Blaum,

More information

Coherent and incoherent nuclear pion photoproduction

Coherent and incoherent nuclear pion photoproduction Coherent and incoherent nuclear pion photoproduction Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Gordon Conference on photonuclear reactions, August 2008

More information

RFSS: Lecture 6 Gamma Decay

RFSS: Lecture 6 Gamma Decay RFSS: Lecture 6 Gamma Decay Readings: Modern Nuclear Chemistry, Chap. 9; Nuclear and Radiochemistry, Chapter 3 Energetics Decay Types Transition Probabilities Internal Conversion Angular Correlations Moessbauer

More information

Collective rotation and vibration in neutron-rich 180,182 Hf nuclei

Collective rotation and vibration in neutron-rich 180,182 Hf nuclei Collective rotation and vibration in neutron-rich 180,182 Hf nuclei E. Ngijoi-Yogo, S. K. Tandel, G. Mukherjee, I. Shestakova, and P. Chowdhury Department of Physics, University of Massachusetts Lowell,

More information

Fission fragment mass distributions via prompt γ -ray spectroscopy

Fission fragment mass distributions via prompt γ -ray spectroscopy PRAMANA c Indian Academy of Sciences Vol. 85, No. 3 journal of September 2015 physics pp. 379 384 Fission fragment mass distributions via prompt γ -ray spectroscopy L S DANU, D C BISWAS, B K NAYAK and

More information

What do we measure, and how do we measure it?

What do we measure, and how do we measure it? What do we measure, and how do we measure it? Production of transactinides Isolation of nuclei of interest Instrumentation and measurements K. Hauschild Production of Transactinides N-capture + β-decay

More information

Nuclear Shape Dynamics at Different Energy Scales

Nuclear Shape Dynamics at Different Energy Scales Bulg. J. Phys. 44 (207) 434 442 Nuclear Shape Dynamics at Different Energy Scales N. Minkov Institute of Nuclear Research and Nuclear Energy, Bulgarian Academy of Sciences, Tzarigrad Road 72, BG-784 Sofia,

More information

Shape coexistence in light Krypton isotopes

Shape coexistence in light Krypton isotopes Shape coexistence in light Krypton isotopes Introduction : Shape coexistence Safe Coulomb excitation of RIBs RDDS Lifetime measurement Results and conclusions Andreas Görgen DAPNIA / Service de Physique

More information

Montecarlo simulation of the decay of warm superdeformed nuclei

Montecarlo simulation of the decay of warm superdeformed nuclei Montecarlo simulation of the decay of warm superdeformed nuclei E. Vigezzi INFN Milano Understanding the dynamics in the SD well: probing γ strength functions, energy barriers, level densities, residual

More information

Mean field studies of odd mass nuclei and quasiparticle excitations. Luis M. Robledo Universidad Autónoma de Madrid Spain

Mean field studies of odd mass nuclei and quasiparticle excitations. Luis M. Robledo Universidad Autónoma de Madrid Spain Mean field studies of odd mass nuclei and quasiparticle excitations Luis M. Robledo Universidad Autónoma de Madrid Spain Odd nuclei and multiquasiparticle excitations(motivation) Nuclei with odd number

More information

Approved for Public Release Distribution Unlimited f\ FQtf- öl" J & \

Approved for Public Release Distribution Unlimited f\ FQtf- öl J & \ SPCH8-4-017 REPORT Item 0002 for the contract Investigation ofk-mixing in Nuclei with Isomeric States Supported by Contract No. F61708-98-W0027 Submitted by Acad. Prof. Dr. Ioan-Iovitz Popescu Principal

More information

Study of multi-nucleon transfer reactions with light nuclei

Study of multi-nucleon transfer reactions with light nuclei Study of multi-nucleon transfer reactions with light nuclei G. Benzoni, D. Montanari, A. Bracco,N.Blasi, F. Camera, F.C.L. Crespi,A.Corsi,S.Leoni, B. Million, R. Nicolini, O. Wieland, A. Zalite,F.Zocca,

More information

Particle excitations and rotational modes in nuclei with A 70-90

Particle excitations and rotational modes in nuclei with A 70-90 . 4 5 7 / 5-6 4 7 4 5 5 -, 4. 1 I J E J K J B H A H K @ = @ H A F D O I E Particle excitations and rotational modes in nuclei with A 7-9 In nuclei of the mass region with A 7-9 both protons and neutrons

More information

Structure of the Low-Lying States in the Odd-Mass Nuclei with Z 100

Structure of the Low-Lying States in the Odd-Mass Nuclei with Z 100 Structure of the Low-Lying States in the Odd-Mass Nuclei with Z 100 R.V.Jolos, L.A.Malov, N.Yu.Shirikova and A.V.Sushkov JINR, Dubna, June 15-19 Introduction In recent years an experimental program has

More information

Antimagnetic Rotation in Cd isotopes

Antimagnetic Rotation in Cd isotopes Proceedings of the DAE Symp. on Nucl. Phys. 56 (2011) 3 Antimagnetic Rotation in Cd isotopes S.Chattopadhyay,* and S. Roy Saha Institute of Nuclear Physics, Kolkata - 700064, INDIA. * email: Sukalyan.chattopadhyay@saha.ac.in

More information

Studying the nuclear pairing force through. Zack Elledge and Dr. Gregory Christian

Studying the nuclear pairing force through. Zack Elledge and Dr. Gregory Christian Studying the nuclear pairing force through 18 O( 26 Mg, 28 Mg) 16 O Zack Elledge and Dr. Gregory Christian Weizsaecker Formula Binding energy based off of volume and surface terms (strong force), coulomb

More information

The 46g BGO bolometer

The 46g BGO bolometer Nature, 3 The g BGO bolometer 1 Photograph of the heat [g BGO] and light [Ge; =5 mm] bolometers: see Fig. 1c for description Current events: Amplification gains: 8, (heat channel) &, (light channel). The

More information

arxiv: v3 [nucl-ex] 12 Jan 2012

arxiv: v3 [nucl-ex] 12 Jan 2012 Fast-timing measurements in 95,96 Mo arxiv:2.539v3 [nucl-ex] 2 Jan 202 S Kisyov, S Lalkovski, N Mǎrginean 2, D Bucurescu 2, L Atanasova 3, D Balabanski 3, Gh Cata-Danil 2, I Cata-Danil 2, D Deleanu 2,

More information

Gamma-ray spectroscopy II

Gamma-ray spectroscopy II Gamma-ray spectroscopy II Andreas Görgen DAPNIA/SPhN, CEA Saclay F-91191 Gif-sur-Yvette France agoergen@cea.fr Lectures presented at the IoP Nuclear Physics Summer School September 4 17, 2005 Chester,

More information

Photopion photoproduction and neutron radii

Photopion photoproduction and neutron radii Photopion photoproduction and neutron radii Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Jefferson Lab PREX workshop, August 2008 Talk Outline Nuclear (π

More information

Spectroscopy of 252No to Investigate its K-isomer

Spectroscopy of 252No to Investigate its K-isomer Spectroscopy of to Investigate its K-isomer Edward Parr Motivation in Superheavies PROTONS Single Particle Energy (MeV) Single Particle Energy (MeV) NEUTRONS Next shell gaps predicted for Superheavy spherical

More information

Status & Future for In-Beam Spectrometers for Tagging at JYFL

Status & Future for In-Beam Spectrometers for Tagging at JYFL Status & Future for In-Beam Spectrometers for Tagging at JYFL Department of Physics, Finland Task 1 - Improvement of RDT method (Jyväskylä) Extend the method from α-decay tagging to β-γ tagging, for the

More information

HEIDI WATKINS. Plunger Measurements of Shape Coexistence in the Neutron Deficient 174 Pt Nuclei

HEIDI WATKINS. Plunger Measurements of Shape Coexistence in the Neutron Deficient 174 Pt Nuclei Plunger Measurements of Shape Coexistence in the Neutron Deficient 174 Pt Nuclei HEIDI WATKINS 2009 IoP NUCLEAR PHYSICS CONFERENCE UNIVERSITY OF BIRMINGHAM OVERVIEW Physics Motivation. Shape Coexistence

More information

Spectroscopy of 74 Ge: from soft to rigid triaxiality

Spectroscopy of 74 Ge: from soft to rigid triaxiality Spectroscopy of 7 Ge: from soft to rigid triaxiality J. J. Sun a, Z. Shi b, X. Q. Li a,, H. Hua a,, C. Xu a, Q. B. Chen a, S. Q. Zhang a, C. Y. Song b, J. Meng a, X. G. Wu c, S. P. Hu c, H. Q. Zhang c,

More information

p(p,e + ν)d reaction determines the lifetime of the sun

p(p,e + ν)d reaction determines the lifetime of the sun 2013.12.25 Contents Basic properties of nuclear systems Different aspects in different time scales Symmetry breaking in finite time scale Rapidly rotating nuclei Superdeformation and new type of symmetry

More information

Report on Nuclear Spectroscopy at JYFL

Report on Nuclear Spectroscopy at JYFL Report on on Report Nuclear Spectroscopy Spectroscopy Nuclear at JYFL JYFL at In-beam & Decay Spectroscopy (Daresbury, Liverpool, Manchester, Paisley, Surrey, York) Collinear Laser Spectroscopy (Birmingham,

More information

More Energetics of Alpha Decay The energy released in decay, Q, is determined by the difference in mass of the parent nucleus and the decay products, which include the daughter nucleus and the particle.

More information

Bogdan Fornal. Institute of Nuclear Physics, Polish Academy of Sciences Krakow, Poland. PARIS Workshop, October 14-16, 2009, Kraków, Poland

Bogdan Fornal. Institute of Nuclear Physics, Polish Academy of Sciences Krakow, Poland. PARIS Workshop, October 14-16, 2009, Kraków, Poland Bogdan Fornal Institute of Nuclear Physics, Polish Academy of Sciences Krakow, Poland PARIS Workshop, October 14-16, 2009, Kraków, Poland V ( r ) = V WS ( r ) + V ls R 2 0 1 r dv ( r) dr L ˆ S ˆ appearence

More information

Role of Hexadecupole Deformation in the Shape Evolution of Neutron-rich Nd Isotopes

Role of Hexadecupole Deformation in the Shape Evolution of Neutron-rich Nd Isotopes Role of Hexadecupole Deformation in the Shape Evolution of Neutron-rich Nd Isotopes Center for Nuclear Study, the University of Tokyo Rin Yokoyama INPC 2016 at Adelaide, Australia Sep. 13, 2016 Sep. 13,

More information

Physics of neutron-rich nuclei

Physics of neutron-rich nuclei Physics of neutron-rich nuclei Nuclear Physics: developed for stable nuclei (until the mid 1980 s) saturation, radii, binding energy, magic numbers and independent particle. Physics of neutron-rich nuclei

More information

Isospin symmetry breaking in mirror nuclei. Experimental and theoretical methods

Isospin symmetry breaking in mirror nuclei. Experimental and theoretical methods Isospin symmetry breaking in mirror nuclei Experimental and theoretical methods Silvia M. Lenzi Dipartimento di Fisica dell Università and INFN, Padova, Italy 2. Experimental techniques for mirror spectroscopy

More information

International Nuclear Physics Conference Adelaide, Australia September 13, 2016

International Nuclear Physics Conference Adelaide, Australia September 13, 2016 International Nuclear Physics Conference Adelaide, Australia September 13, 2016 This work was performed under the auspices of the U.S. Department of Energy by under contract DE-AC52-07NA27344. Lawrence

More information

Gamma-ray spectroscopy

Gamma-ray spectroscopy Gamma-ray spectroscopy Alison Bruce University of Brighton Aim is to give an overview for non-specialists but also some details that specialists might find useful. Contents: Basic gamma-ray properties,

More information

Experimental Nuclear Structure Part II

Experimental Nuclear Structure Part II Experimental Nuclear Structure Part II Filip G. Kondev kondev@anl.gov Workshop on Nuclear Structure and Decay Data: Theory and Evaluation, Trieste, Italy February 20 th March 3 rd, 2006 Argonne National

More information

EXPERIMENTAL METHODS

EXPERIMENTAL METHODS S. H. Liu, 1 J. H. Hamilton, 1 A. V. Ramayya, 1 A. Covello, 2 A. Gargano, 2 N. Itaco, 2 Y. X. Luo, 1,3 J. O. Rasmussen, 3 S. J. Zhu, 4 J. K. Hwang, 1 A.V.Daniel, 1,5 G.M.Ter-Akopian, 5 Y. Oganessian 5,

More information

Compound and heavy-ion reactions

Compound and heavy-ion reactions Compound and heavy-ion reactions Introduction to Nuclear Science Simon Fraser University Spring 2011 NUCS 342 March 23, 2011 NUCS 342 (Lecture 24) March 23, 2011 1 / 32 Outline 1 Density of states in a

More information

5 th ASRC International Workshop, 14 th -16 th March 2012

5 th ASRC International Workshop, 14 th -16 th March 2012 Fission Fragment Fragment Spectroscopy with Large Arrays and STEFF A.G. Smith, J. Dare, A. Pollitt, E. Murray The University of Manchester W. Urban, T. Soldner ILL Grenoble I. Tsekhanovich, J. Marrantz

More information

Probing shell evolution with large scale shell model calculations

Probing shell evolution with large scale shell model calculations Probing shell evolution with large scale shell model calculations Yutaka Utsuno Advanced Science Research Center, Japan Atomic Energy Agency Center for Nuclear Study, University of Tokyo Nuclear structure

More information

Gamma Spectroscopy of 207 Tl 126 Populated in Deep-Inelastic Collisions

Gamma Spectroscopy of 207 Tl 126 Populated in Deep-Inelastic Collisions Gamma Spectroscopy of 207 Tl 126 Populated in Deep-Inelastic Collisions Emma Wilson Submitted for the degree of Doctor of Philosophy Department of Physics Faculty of Engineering and Physical Sciences University

More information

Search for the chiral doublet bands in 78 Br. Speaker: C. Liu Supervisor: Prof. S. Y. Wang Shandong University, Weihai

Search for the chiral doublet bands in 78 Br. Speaker: C. Liu Supervisor: Prof. S. Y. Wang Shandong University, Weihai Search for the chiral doublet bands in 78 Br Speaker: C. Liu Supervisor: Prof. S. Y. Wang Shandong University, Weihai Contents 1 2 3 4 Introduction Experiment Details Result and Discussions Conclusion

More information

Types of radiation resulting from radioactive decay can be summarized in a simple chart. Only X-rays, Auger electrons and internal conversion

Types of radiation resulting from radioactive decay can be summarized in a simple chart. Only X-rays, Auger electrons and internal conversion General information Nuclei are composed of combinations of nucleons (protons and neutrons); certain combinations of these nucleons (i.e., certain nuclides) possess a high degree of stability while others

More information

2007 Fall Nuc Med Physics Lectures

2007 Fall Nuc Med Physics Lectures 2007 Fall Nuc Med Physics Lectures Tuesdays, 9:30am, NN203 Date Title Lecturer 9/4/07 Introduction to Nuclear Physics RS 9/11/07 Decay of radioactivity RS 9/18/07 Interactions with matter RM 9/25/07 Radiation

More information

Antimagnetic rotation in 108,110 In with tilted axis cranking relativistic mean-field approach *

Antimagnetic rotation in 108,110 In with tilted axis cranking relativistic mean-field approach * Antimagnetic rotation in 108,110 In with tilted axis cranking relativistic mean-field approach * Wu-Ji Sun( ) Hai-Dan Xu( ) Jian Li( ) 1) Yong-Hao Liu( ) Ke-Yan Ma( ) Dong Yang( ) Jing-Bing Lu( ) Ying-Jun

More information

Towards 78 Ni: In-beam γ-ray spectroscopy of the exotic nuclei close to N=50

Towards 78 Ni: In-beam γ-ray spectroscopy of the exotic nuclei close to N=50 Towards 78 Ni: In-beam γ-ray spectroscopy of the exotic nuclei close to N= IPN Orsay: D. Verney, M. Niikura, F. Aziez, S. Franchoo, F. Ibrahim, F. Le Blanc, I. Matea, I. Stefan CSNSM Orsay: A. Korichi

More information

Research at FSU, using RESOLUT facility Development of and research with two new detector-systems

Research at FSU, using RESOLUT facility Development of and research with two new detector-systems Nuclear Astrophysics and Structure Research with Radioactive Beams Research at FSU, using RESOLUT facility Development of and research with two new detector-systems ResoNeut: Low-energy neutron detector-array

More information

Projected total energy surface description for axial shape asymmetry in 172 W

Projected total energy surface description for axial shape asymmetry in 172 W . Article. SCIENCE CHINA Physics, Mechanics & Astronomy November 014 Vol. 57 No. 11: 054 059 doi: 10.1007/s11433-014-557-4 Projected total energy surface description for axial shape asymmetry in 17 W TU

More information

Band Structure of nuclei in Deformed HartreeFock and Angular Momentum Projection theory. C. R. Praharaj Institute of Physics Bhubaneswar.

Band Structure of nuclei in Deformed HartreeFock and Angular Momentum Projection theory. C. R. Praharaj Institute of Physics Bhubaneswar. Band Structure of nuclei in Deformed HartreeFock and Angular Momentum Projection theory C. R. Praharaj Institute of Physics. India INT Workshop Nov 2007 1 Outline of talk Motivation Formalism HF calculation

More information

Magnetic rotation past, present and future

Magnetic rotation past, present and future PRAMANA c Indian Academy of Sciences Vol. 75, No. 1 journal of July 2010 physics pp. 51 62 Magnetic rotation past, present and future A K JAIN and DEEPIKA CHOUDHURY Department of Physics, Indian Institute

More information

X-ray superburst ~10 42 ergs Annual solar output ~10 41 ergs. Cumming et al., Astrophys. J. Lett. 559, L127 (2001) (2)

X-ray superburst ~10 42 ergs Annual solar output ~10 41 ergs. Cumming et al., Astrophys. J. Lett. 559, L127 (2001) (2) Neutron stars, remnant cores following supernova explosions, are highly interesting astrophysical environments In particular, accreting neutron stars presents a unique environment for nuclear reactions

More information

The two-step (and multiple-step) γ cascade method as a tool for studying γ-ray strength functions. Milan Krtička

The two-step (and multiple-step) γ cascade method as a tool for studying γ-ray strength functions. Milan Krtička The two-step (and multiple-step) γ cascade method as a tool for studying γ-ray strength functions Milan Krtička Outline The method of two-step γ-cascades following thermal neutron capture (setup at Rez

More information