EoS constraints from a model-independent approach Francesca - - PowerPoint PPT Presentation

eos constraints from a model independent approach
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EoS constraints from a model-independent approach Francesca - - PowerPoint PPT Presentation

EoS constraints from a model-independent approach Francesca Gulminelli, Debarati Chatterjee - LPC Caen Jerome Margueron IPNL Adriana Raduta IFIN EoS and empirical constraints E o S c a n b e c ha ra c te rize d b y e mpiric a


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Francesca Gulminelli, Debarati Chatterjee - LPC Caen Jerome Margueron – IPNL Adriana Raduta – IFIN

EoS constraints from a model-independent approach

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EoS and empirical constraints

  • E
  • S c a n b e

c ha ra c te rize d b y e mpiric a l pa ra me te rs

/ e x:J,L

,…

  • DF

T mo de ls c o rre spo nding to diffe re nt E

  • S a re

c o mpa re d to e xp.da ta

  • ∆ de te rmine d

fitting the mo de l to the da ta

  • Co rre la tio ns a mo ng

a re typic a lly o b se rve d

M.Fortin et al, PRC 94,035804

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Problems

  • Nuc le i a re no t simply

dro ple ts o f nuc le a r ma tte r! E ne rg y func tio na ls c o nta in ma ny te rms

=> Unc e rta inty in g ra die nt c o upling s g e ts mixe d up with unc e rta inty in Pk

  • Phe no func tio na ls

c o nta in spurio us c o rre la tio ns a mo ng e mp.pa ra me te rs

=> re sults a re mo de l de pe nde nt

C.Ducoin et al PRC 2011

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Problems

  • Nuc le i a re no t simply

dro ple ts o f nuc le a r ma tte r! E ne rg y func tio na ls c o nta in ma ny te rms

=> Unc e rta inty in g ra die nt c o upling s g e ts mixe d up with unc e rta inty in Xn

  • Phe no func tio na ls

c o nta in spurio us c o rre la tio ns a mo ng e mp.pa ra me te rs

 re sults a re mo de l de pe nde nt

C.Ducoin et al PRC 2011

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A model independent approach

  • Nuc le i a re no t simply

dro ple ts o f nuc le a r ma tte r! E ne rg y func tio na ls c o nta in ma ny te rms

=> Unc e rta inty in g ra die nt c o upling s g e ts mixe d up with unc e rta inty in Pk

  • Phe no func tio na ls

c o nta in spurio us c o rre la tio ns a mo ng e mp.pa ra me te rs

=> re sults a re mo de l de pe nde nt

A single effective isoscalar gradient term to be fitted on nuclear masses , Taylor expansion around n0 , 1 !

  • 3
  • /

Steiner, Lattimer, Brown ApJ722(2010)33

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HNM: Quality of the Taylor expansion

Chiral EFT

I.Tews, T.Kruger,K.Hebeler,A.Schwenk PRL110(2013)032504

Sly5

E.Chabanat, P.Bonche, P.Hansel, J.Meyer, R.Schaeffer, NPA627(1997)710

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Symmetry energy

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Present uncertainty on Pk: prior distribution

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HNM: Constraints from neutron star physics

  • Ca usa lity: 0
  • NS sta b ility: 0 fo r in -e q uilib rium
  • Mma x>2Mo
  • L

imit o n DURCA:

  • No DURCA up to 2Mo – DURCA0
  • DURCA o nly fo r M>1.8Mo – DURCA1
  • DURCA o nly fo r M>1.6Mo – DURCA2
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Results

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Finite nuclei

  • Nuc le i a re no t simply

dro ple ts o f nuc le a r ma tte r! E ne rg y func tio na ls c o nta in ma ny te rms

=> Unc e rta inty in g ra die nt c o upling s g e ts mixe d up with unc e rta inty in Pk

A single effective isoscalar gradient term to be fitted on nuclear masses , Observables from -ETF with parametrized density profiles

  • 1
  • Analytical integration of the

Fermi integrals

F.Aymard et al., J.Phys.G43,045105(2016)

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Calibrating the gradient term

  • ,

, N= Z ∆ C 20 Optimized C Sly4

  • Residual deviations are

due to the semi- classical approximation

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Semi-magic isotopic chains

(N-Z)/ A + Z= 2 0 Z= 2 8 Z= 5 0 Z= 8 2

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Exploring the parameter space

Average binding-energy deviation Average binding-energy deviation

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Results: radii

  • Afte r filte r; c uto ff=0.2 Me V

Exp data

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Results: n-skin

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Results: correlations

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Conclusions

  • Co nstra ints o n E
  • S e mpiric a l pa ra me te rs ne e d b o th NS

physic s a nd la b o ra to ry e xpe rime nts

  • We pro po se a n e mpiric a l E
  • S a vo iding spurio us

c o nstra ints fro m the e ne rg y de nsity func tio na l fo rm

  • F

inite nuc le i o b se rva b le s fro m E T F with a sing le g ra die nt te rm fixe d fro m nuc le a r ma ss

  • Ba ye sia n de te rmina tio n o f pa ra me te rs with fla t o r

g a ussia n prio r

  • T

hird orde r de riva tive s still la rg e ly unc onstra ine d

  • SKIN CORRE

L AT E D T O L

  • AL

MOST NO CORRE L AT ION AMONG E MP.PARAME T E RS

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