Pear-shaped nuclei measured via Coulomb excitation at REX- ISOLDE Liam P. Gaffney EuNPC2015 University of the West of Scotland, UK University of Liverpool,

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Pear-shaped nuclei measured via Coulomb excitation at REX- ISOLDE Liam P. Gaffney EuNPC2015 University of the West of Scotland, UK University of Liverpool, UK Peter Butler PhD Supervisor

Described by a multipole expansion in λ Multipole order: 2 λ 2 0 = monopole - breathing mode 2 1 = dipole - centre of mass shift 2 2 = quadrupole - axial deformation 2 3 = octupole - asymmetric deformation 2 4 = hexadecapole - pinching Nuclear Shapes Liam Gaffney - EuNPC2015 2

Reflection Asymmetry (Nuclei) Liam Gaffney - EuNPC Macroscopically... Nuclei take on a “pear” shape Reflection asymmetric β 3 -vibration Static β 3 -deformation Rigid β 3 -deformation... Signatures... Odd-even staggering, negative parity Parity doublets in odd-A nuclei Collective B(E3) transitions

224 Ra Reflection Asymmetry (Molecules) Liam Gaffney - EuNPC Asymmetric HCl molecule Rotational band – staggering of odd and even spin states F. Stephens, Jr., F Asaro and I. Perlman Phys. Rev. 96 (1954) 1568, 100 (1955) 1543

Reflection Asymmetry Liam Gaffney - EuNPC Microscopically driven... Intruder orbitals of opposite parity and ∆J, ∆L = 3 close to the Fermi level εFεF Enhancement of octupole part of nucleon-nucleon force... - Small energy gap - High sub-state density } Heaviest nuclei

Quantifying the pear-shape Liam Gaffney - EuNPC L.M. Robledo et al., Phys. Rev. C 81, (2010) RaRa Mean-field calculations reproduce behaviour of E1 transitions Two contributions to Q 1 : - Macroscopic of the order +0.1 fm - Microscopic of the order -0.1 fm Cancellation gives small B( E1 ) in 224 Ra

Quantifying the pear-shape Liam Gaffney - EuNPC Pros: - Less sensitive to single particle effects - Direct measure of octupole collectivity - Link to deformation via β 3 parameter Cons: - Difficult to access E3 transitions - Excited state decay dominated by E1/E2 B(E3) >~ 30 s.p.u. gives significant β 3

Coulomb Excitation Liam Gaffney - EuNPC Projectile (Z 1,A 1 ) Target (Z 2,A 2 ) b θ v Sommerfeld parameter: “Safe” Coulex: Dominated by E2 and E3 excitation near the Coulomb barrier

Octupole Collectivity Liam Gaffney - EuNPC Rn (Z=86)? Z = 34 Z = 56 Z = 88N = Ra

1.4 GeV p + primary target Hot W line (Ra) HRS REXTRAP + EBIS Post acceleration up to 3 MeV/u Miniball VADIS (Rn) GPS REX-ISOLDE, CERN Liam Gaffney - EuNPC

REX-ISOLDE Rn/ 224 Ra ~2.83 MeV/u Coulex target ~2 mg/cm 2

Miniball: Coulex set-up Liam Gaffney - EuNPC Particle ID in a Double- Sided Si Strip Detector. Event by event Doppler correction. 17˚ < θ lab < 54˚ Array of HPGe of 8 triple clusters 6-fold segmentation for positioning ε > 7% for 1.3MeV γ-rays N. Warr et al., EPJ 49 (2013)

Particle-gamma coincidences Prompt Random Normalisation = t prompt t random 224 Ra 120 Sn Liam Gaffney - EuNPC

60 Ni target - 2.1mg/cm2 120 Sn target - 2.0mg/cm2 224 Ra 60 Ni target - 2.1mg/cm2 120 Sn target - 2.3mg/cm2 220 Rn Spectra Rn and 224 Ra Liam Gaffney - EuNPC Heaviest short-lived ISOL beams to date

Analysis Ra Gosia Liam Gaffney - EuNPC free matrix elements + 6 normalisation factors “Experiment”Number and type of data Multi-nucleon transfer[1,2] 226 Ra( 58 Ni, 60 Ni) 224 Ra 232 Th( 136 Xe, 128 Te) 224 Ra Alpha, alpha-prime[3] 226 Ra(α,α’2n) 224 Ra Alpha(beta)-decay[4] 228 Th( 224 Fr) → α(β) Branching ratios (1 -, 3 -, 5 -, 7 -, 2 + γ ) -- 5 Delayed-coincidence [5,6]Lifetimes (2 +, 4 + ) -- 2 Cd/Sn high CoM range 23.9˚ < θ lab < 40.3˚ γ-ray yield Ni high CoM range 23.1˚ < θ lab < 39.9˚ γ-ray yield Cd/Sn low CoM range 40.3˚ < θ lab < 54.3˚ γ-ray yield Ni low CoM range 39.3˚ < θ lab < 53.2˚ γ-ray yield -- 7 Total55 data points [1] Poynter et al., Phys. Lett. B 232, 447 (1989) [2] J.F.C. Cocks et al., Nucl. Phys. A 645, 61 (1999) [3] Marten-Tölle et al., Z. Phys. A 336, 27 (1990) [4] W. Kurcewicz, et al., Nucl. Phys. A 289 (1977) [5] W.R. Neal and H.W. Kraner, Phys. Rev. 137, B1164 (1965) [6] H. Ton et al., Nucl. Phys. A 155, 235 (1970)  2 total = 27

Results Ra Liam Gaffney - EuNPC Consistent with rotational model Unstretched E3 matrix elements are non- zero. Coupled with level energy data, we observe a static octupole deformation in 224 Ra

Results Rn Liam Gaffney - EuNPC Consistent with rotational model. No information on unstretched E3. Much larger data set required to determine if vanishes. δE and Δix implies a coupling of an octupole phonon to the even-spin rotational band. Dynamic collectivity in 220 Rn Fit: 34 data points -> 21 free parameters January 2015: 146 Nd, 148 Sm, 152 Gd measure with MINORCA (Miniball at Orsay)

Static or dynamic pear-shape? Liam Gaffney - EuNPC Octupole phonon coupled to even-spin rotational band. Even-spin band O Odd-spin band J.F.C. Cocks et al., Nucl. Phys. A 645, 61 (1999) Odd-spin states aligned to intrinsic rotational structure of the even-spin band.

Statically deformed or vibrational? Liam Gaffney - EuNPC Octupole vibrational Our data Radioactive beams

Q1Q1 Q2Q2 Q3Q3 Comparison to theory Liam Gaffney - EuNPC Cluster model [1] - Misses small Q1 - Q 2 is consistently too low - Q 3 trend not observed Mean field, HFB with D1S or D1M [2] - Predicts cancelation of Q 1 - Differences in Q 3 predictions More (good) mean-field models on the market Important Q 2 -Q 3 coupling [3] [3] Robledo & Butler (2013). Phys. Rev. C, R [1] Shneidman, et al. (2003). Phys. Rev. C, 67(1) [2] Robledo & Bertsch (2011). Phys. Rev. C, 84(5) nd place to ICECube

Electric Dipole Moment (EDM) Liam Gaffney - EuNPC A static atomic EDM implies CP-violation or equivalently T-violation Schiff theorem: neutral atomic system of point particles in electric field readjusts itself to give zero E field at all charges. BUT: finite size of nucleus and shape of charge distribution can break the symmetry TRIUMF (S929) 221,223 Rn Radium EDM ANL 225 Ra KVI (+atomic sensitivity) Ra Atomic EDM proportional to Schiff moment - Experiments are taking advantage of this in North America and right here in Groningen! 

Octupole enhanced EDM Liam Gaffney - EuNPC Current Limit: |d( 199 Hg)| < 3.1x e cm [1] [2] W. C. Griffith et al. Phys. Rev. Lett. 102, (2009) Schiff moment 224 Ra Energy splitting of parity doublets [1] J. Dobaczewski, & J. Engel, Phys. Rev. Lett., 94, (2005) [3] M. Pospelov & A. Ritz, Annals of Physics, 318, 119 (2005) 225 Ra ∆E = 55 keV 221 Rn ∆E = ?? keV Sensitivity increase of ~1000 for octupole deformed nuclei + experimental improvements [1]

Preliminary Coulex of 221 Rn Liam Gaffney - EuNPC K X rays 201 keV 224 keV 273 keV 290 keV - doublet Large x-ray excess implies strongly converted, low-energy transitions which are not observed SPEDE - e - detector for MINIBALL Experiment to be re-run to define level scheme Complementary β-decay experiment in the pipeline ISOLDE) Courtesy of George O’Neill, PhD student University of Liverpool

Summary and outlook Liam Gaffney - EuNPC Demonstrated sensitivity and ability to measure E3 matrix elements with Radioactive Ion Beams (RIBs). B(E3; 3 -  0 + ) measured for the first time in Rn’s and only second measurement in Ra’s, both to ~10% precision. Proposal for measurements in 222,226,228 Ra and Ba region at HIE-ISOLDE (starting next year). Plus odd-mass nuclei ( 221 Rn), in progress Odd-mass nuclei key to atomic EDM measurements. Nuclear structure input vital; beginning to appear.

Collaborators Liam Gaffney - EuNPC T.E. Cocolios, J. Pakarinen, J.Cederkall, D. Voulot, F. Wernander Th. Kröll, S. Bönig, C. Bauer, M. von Schmid B. Bastin T. Grahn, A. Herzan A. Blazhev, M. Seidlitz, N. Warr, M. Albers, M. Pfeiffer, D. Radeck M. Rudigier, P. Thöle P. van Duppen, N. Bree, J. Diriken, N. Kesteloot, M. Huyse S. Sambi, K. Reynders L. P. Gaffney, P. A. Butler, M. Scheck, D.T. Joss, S.V. Rigby E. Kwan T. Chupp K. Wimmer, R. Lutter D. Cline, A.B. Hayes, C.Y. Wu P. Napiorkowski, M. Kowalczyk, K. Wrzosek-Lipska D.G. Jenkins M. Zielinska CERN-ISOLDE, Switzerland TU Darmstadt, Germany Ganil, France University of Jyväskylä, Finland University of Köln, Germany KU Leuven, Belgium University of Liverpool, UK Lawrence Livermore Laboratory, US University of Michigan, US TU München, Germany University of Rochester, US HIL University of Warsaw, Poland University of York, UK CEA Saclay, France Thank you! Dankjewel! and the REX-ISOLDE and MINIBALL collaborations

Future measurements Liam Gaffney - EuNPC [1] Robledo, L. M., & Bertsch, G. F. (2011). Phys. Rev. C, 84(5), ,228 U 226 Th Estimated intensity at FRIB for 228 U ~ 4x10 6 s -1 [2] P.T. Greenlees et al. J. Phys. G: Nucl. Part. Phys. 24 (1998) L63 [1] Robledo & Bertsch (2011). Phys. Rev. C, 84(5)

Q MeV/u 3 MeV/u 3 MeV/u 4.5 MeV/u 10 MeV/u 8 MeV/u 8 MeV/u 221,222 Rn 222,226,228 Ra 144 Ba 5.5 MeV/u Q HIE-ISOLDE 27 High Intensity and Energy upgrade CERN Long Shutdown; HIE-ISOLDE upgrade synchronised First experiments expected next month ( 182,184 Hg, ; October 2015!!)

Analysis - 220Rn: High/Low θ Liam Gaffney - EuNPC High CoM θ Low CoM θ

Analysis - 220Rn γ-γ Liam Gaffney - EuNPC γ(697 keV)