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R' F' Casten

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Masses, Bubbles and Two Nucleon Transfer: A ... How the world, with all its apparent complexity and diversity can be constructed ... Daeg Brenner, Jing-ye Zhang ... – PowerPoint PPT presentation

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Title: R' F' Casten


1
Masses, Bubbles and Two Nucleon Transfer A New
Perspective on Nuclear Collectivity
Microscopic Drivers of Structural Evolution
R. F. Casten The Yale Elderly Professor of
Physics WNSL, Yale June 18, 2009
2
  • Themes and challenges of Modern Science
  • Complexity out of simplicity -- Microscopic
  • How the world, with all its apparent complexity
    and diversity can be constructed out of a few
    elementary building blocks and their interactions
  • Simplicity out of complexity Macroscopic
  • How the world of complex systems can display such
    remarkable regularity and simplicity

3
Broad perspective on structural evolution
4
Microscopic origins of collectivity
correlations, configuration mixing and
deformation Residual interactions
Crucial for structure
Crucial for masses
5
Sn Magic no valence p-n interactions
Critical role of the valence p-n interaction
Both valence protons and neutrons
NpNn Scheme
6
Getting at the p-n interactionsMasses Reflect
Nucleonic Interactions
Total mass/binding energy Sum of all
interactions Mass differences Separation
energies shell structure, phase transitions,
collectivity Double differences of masses
Interaction filters
  • Shell structure
    1 MeV
  • Quantum phase transitions 100s keV
  • Collective effects
    100s keV
  • Interaction filters
    10-15 keV

Macro
Micro
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Measurements of p-n Interaction Strengths
  • dVpn
  • Average p-n interaction between
  • last protons and last neutrons
  • Double Difference of Binding Energies
  • ?Vpn (Z,N)    ¼ B(Z,N) - B(Z, N-2)  - 
    B(Z-2, N) - B(Z-2, N-2)

Ref J.-y. Zhang and J. D. Garrett
9
Valence p-n interaction Can we measure it?
?Vpn (Z,N)     ¼ B(Z,N) - B(Z,
N-2) -  B(Z-2, N) - B(Z-2, N-2)
-
-
-
p n p
n p n
p n
-
Int. of last two n with Z protons, N-2 neutrons
and with each other
Int. of last two n with Z-2 protons, N-2
neutrons and with each other
Empirical average interaction of last two
neutrons with last two protons
10
Orbit dependence of p-n interactions simple
ideas
Low j, high n
High j, low n
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16
Can we extend these ideas beyond magic regions?
17
Away from closed shells, these simple arguments
are too crude. But some general predictions can
be made
p-n interaction is short range similar orbits
give largest p-n interaction
Largest p-n interactions if proton and neutron
shells are filling similar orbits
18
Empirical p-n interaction strengths indeed
strongest along diagonal.
Empirical p-n interaction strengths stronger in
like regions than unlike regions.
Low j, high n
High j, low n
New mass data on Xe isotopes at ISOLTRAP ISOLDE
CERN Neidherr et al, preliminary
19
p-n interactions and the evolution of structure
Direct correlation of observed growth rates of
collectivity with empirical p-n interaction
strengths
20
BEWARE OF FALSE CORRELATIONS!
21
W. Nazarewicz, M. Stoitsov, W. Satula
Realistic Calculations
  • Microscopic Density Functional Calculations
    with Skyrme forces and different treatments of
    pairing

22
Density Functional Theory
My understanding of DFT
Would you like to see it again? OK.
So, I hope all this is clear.
Anyway, Nazarewicz, Stoitsov and Satula
calculated masses for over 1000 nuclei across the
nuclear chart with several interactions, and,
from these masses, computed the p-n interactions
using the same double difference expression.
Lots of results. A few examples
23
Agreement is remarkable. Especially so since
these DFT calculations reproduce known masses
only to 1 MeV yet the double difference
embodied in dVpn allows one to focus on sensitive
aspects of the wave functions that reflect
specific correlations
24
The new Xe mass measurements at ISOLDE give a new
test of the DFT
25
One last thing
Two regions of parabolic anomalies. Two
regions of octupole correlations Possible
signature?
26
http//workshop.turkfizikdernegi.org
27
Summary
  • p-n interactions and the evolution of
    collectivity
  • Mass filters dVpn available far from
    stability
  • Crossing pattern around doubly magic nuclei --
    orbit overlaps
  • Maximum for similar shell filling along
    diagonal in N-Z plot
  • Maximum in like quadrants (p-p or h-h vs p-h or
    h-p)
  • Correlation with growth rates of collectivity
  • Comparison with DFT calculations
  • Possible signature of octupole correlations

28
Principal Collaborators
  • Burcu Cakirli (Istanbul)
  • Daeg Brenner, Jing-ye Zhang
  • Dennis Neidherr, Klaus Blaum, Magda Kowalska and
    the entire ISOLTRAP collaboration
  • Yuri Litvinov and the GSI Schottky mass group
  • Witek Nazarewicz, Mario Stoitsov, and Wojtek
    Satula
  • (Lee for secretly editing my first slide)
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