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![Page 1: Constraining the nuclear matter equation of state using ... · Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool Constraining the nuclear matter equation of state using the](https://reader034.vdocuments.net/reader034/viewer/2022052104/603fc584ced7fd10020adfb6/html5/thumbnails/1.jpg)
Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the nuclear matter equation of state using the elliptic flow of light clusters
by A. Le Fèvre1, Y. Leifels1, W. Reisdorf1, J. Aichelin2, Ch. Hartnack2, and N. Herrmann3
!1GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
2SUBATECH, UMR 6457, Ecole des Mines de Nantes - IN2P3/CNRS - Université de Nantes, France
3Physikalisches Institut der Universität Heidelberg, Heidelberg, Germany
1
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the nuclear matter equation of state using the elliptic flow of light clusters
‣Constraining the stiffness of the EOS with the elliptic flow.
‣A clusterisation approach…
‣Towards the determination of the stiffness of the asymmetry
energy.
‣Summary and discussion.
by A. Le Fèvre1, Y. Leifels1, W. Reisdorf1, J. Aichelin2, Ch. Hartnack2, and N. Herrmann3
!1GSI Helmholtzzentrum für Schwerionenforschung GmbH, Darmstadt, Germany
2SUBATECH, UMR 6457, Ecole des Mines de Nantes - IN2P3/CNRS - Université de Nantes, France
3Physikalisches Institut der Universität Heidelberg, Heidelberg, Germany
1
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Introduction
[1] J. M. Lattimer, Ann. Rev. Nucl. Part. Sci. 62 (2012) 485. [2] A. Burrows, Rev. Mod. Phys. 85 (2013) 245. [3] A. Gezerlis, I. Tews, E. Epelbaum, S. Gandolfi, K. Hebeler, A. Nogga, A. Schwenk, Phys. Rev. Lett. 111 (2013) 032501
‣ The equation of state (EOS) of nuclear matter:
‣ of fundamental interest
‣ object of intense theoretical efforts since several decades
‣ an important ingredient in modeling fascinating astrophysical phenomena such as:
‣ compact stars [1]
‣ core collapse supernovae[2]
‣ The calculation of the nuclear EOS from first principles, such as very recently attempted in [3], is a very complex task.
‣ Nuclear physics based on empirical observations => even the most ’fundamental’ theory of nuclear forces requires a confrontation with empirical facts.
‣ 1st method, from astrophysicists: from ’neutron’ star masses and radii. But missing:
‣ precise model-independent radii,
‣ composition of the matter in the center of the stars.
NGC 1952, Crab Nebula pulsar neutron star imaged by the NASA/ESA Hubble Space Telescope
2
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Introduction
[1] J. M. Lattimer, Ann. Rev. Nucl. Part. Sci. 62 (2012) 485. [2] A. Burrows, Rev. Mod. Phys. 85 (2013) 245. [3] A. Gezerlis, I. Tews, E. Epelbaum, S. Gandolfi, K. Hebeler, A. Nogga, A. Schwenk, Phys. Rev. Lett. 111 (2013) 032501
‣ The equation of state (EOS) of nuclear matter:
‣ of fundamental interest
‣ object of intense theoretical efforts since several decades
‣ an important ingredient in modeling fascinating astrophysical phenomena such as:
‣ compact stars [1]
‣ core collapse supernovae[2]
‣ The calculation of the nuclear EOS from first principles, such as very recently attempted in [3], is a very complex task.
‣ Nuclear physics based on empirical observations => even the most ’fundamental’ theory of nuclear forces requires a confrontation with empirical facts.
‣ 1st method, from astrophysicists: from ’neutron’ star masses and radii. But missing:
‣ precise model-independent radii,
‣ composition of the matter in the center of the stars.
NGC 1952, Crab Nebula pulsar neutron star imaged by the NASA/ESA Hubble Space Telescope
2
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
IntroductionIQMD Au+Au@2 A.GeV simulation
‣ Alternative method: in earth laboratories, heavy ion collisions over a wide range of incident energies, system sizes and compositions. ‣ limited to Ebeam<10 A.GeV ⬅ some kind of a clock is available (sound velocity versus
participant-spectator interaction).
3
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
IntroductionIQMD Au+Au@2 A.GeV simulation
‣ Alternative method: in earth laboratories, heavy ion collisions over a wide range of incident energies, system sizes and compositions. ‣ limited to Ebeam<10 A.GeV ⬅ some kind of a clock is available (sound velocity versus
participant-spectator interaction).
3
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
IntroductionIQMD Au+Au@2 A.GeV simulation
‣ Alternative method: in earth laboratories, heavy ion collisions over a wide range of incident energies, system sizes and compositions. ‣ limited to Ebeam<10 A.GeV ⬅ some kind of a clock is available (sound velocity versus
participant-spectator interaction).
3
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
IntroductionIQMD Au+Au@2 A.GeV simulation
‣ Alternative method: in earth laboratories, heavy ion collisions over a wide range of incident energies, system sizes and compositions. ‣ limited to Ebeam<10 A.GeV ⬅ some kind of a clock is available (sound velocity versus
participant-spectator interaction).
z
x
V2
yY = rapidity pt = transverse momentum ΦR = reaction plane azimuthal angle
’Elliptic flow’: cos(2(Φ-ΦR)) mode, competition between ‘in-plane’ (V2>0) and ‘out-of-plane’ ejection (V2<0).
V1 = ‘side/directed flow’, <px/pt2>
Flows at high density in heavy-ion collisions
3
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
IntroductionIQMD Au+Au@2 A.GeV simulation
‣ Alternative method: in earth laboratories, heavy ion collisions over a wide range of incident energies, system sizes and compositions. ‣ limited to Ebeam<10 A.GeV ⬅ some kind of a clock is available (sound velocity versus
participant-spectator interaction).
z
x
V2
yY = rapidity pt = transverse momentum ΦR = reaction plane azimuthal angle
’Elliptic flow’: cos(2(Φ-ΦR)) mode, competition between ‘in-plane’ (V2>0) and ‘out-of-plane’ ejection (V2<0).
V1 = ‘side/directed flow’, <px/pt2>
Flows at high density in heavy-ion collisions
3
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
IntroductionIQMD Au+Au@2 A.GeV simulation
‣ Alternative method: in earth laboratories, heavy ion collisions over a wide range of incident energies, system sizes and compositions. ‣ limited to Ebeam<10 A.GeV ⬅ some kind of a clock is available (sound velocity versus
participant-spectator interaction).
3
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
‣ Present work: improve the situation in the 1 A.GeV regime, from extensive flow data published recently by the FOPI Collaboration (Au+Au @ 0.4-1.5 A.GeV) [4] ➜ close look at the elliptic flow data with improvements: ‣ 1) not only protons: d, t, 3He 4He having larger flow signals than
single nucleons. ‣ 2) not only mid-rapidity data: 80% of the target- projectile
rapidity gap.
[4] W. Reisdorf, et al. (FOPI Collaboration), Nucl. Phys. A 876 (2012) 1.
4
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
� IQMD-HM6 IQMD-SM
-0.5 0.0 0.5y0
-0.04
0.00
0.04
0.08
-v2
IQMD-HMIQMD-SM� FOPI
-0.5 0.0 0.5y0
Au+Au 1.2A GeV 0.25<b0<0.45 protonsElliptic flow
5
IQMD: J. Aichelin, Phys. Rep. 202 (1991) 233. C. Hartnack, et al., Eur. Phys. J. A 1 (1998) 151.
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
Complete shape of v2(y0): a new observable: v2n = |v20| + |v22|, from fit v2(y0) = v20 + v22 . y0
!➜ v2n(Ebeam) varies by a factor ≈1.6, >> measured uncertainty (≈1.1) ➜ clearly favors a ’soft’ EOS.
� HM� SM� FOPI
Au+Auprotons
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.05
0.10
0.15
0.20
0.25
0.30
� HM� SM� FOPI
Au+Autritons
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.2
0.4
0.6
0.8
1.0
� HM� SM� FOPI
Au+Audeuterons
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.2
0.4
0.6
� HM� SM� FOPI
Au+Au3He
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.2
0.4
0.6
0.8
1.0
1.2
beam energy (A GeV)
0.25<b0<0.45 ut0>0.4
v 2n(0
.8)
beam energy (A.GeV)
0.25<b0<0.45 ut0>0.4
6
FOPI Collaboration / NPA 876 (2012) 1-60
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
� HM� SM� FOPI
Au+Auprotons
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.05
0.10
0.15
0.20
0.25
0.30
� HM� SM� FOPI
Au+Autritons
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.2
0.4
0.6
0.8
1.0
� HM� SM� FOPI
Au+Audeuterons
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.2
0.4
0.6
� HM� SM� FOPI
Au+Au3He
0.4 0.6 0.8 1.0 1.2 1.4 1.6
0.2
0.4
0.6
0.8
1.0
1.2
beam energy (A GeV)
0.25<b0<0.45 ut0>0.4
v 2n(0
.8)
Complete shape of v2(y0): a new observable: v2n = |v20| + |v22|, from fit v2(y0) = v20 + v22 . y0
!➜ v2n(Ebeam) varies by a factor ≈1.6, >> measured uncertainty (≈1.1) ➜ clearly favors a ’soft’ EOS.
6
FOPI Collaboration / NPA 876 (2012) 1-60
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
1 2l/ l0
HM/SM/FOPI
-16
-12
-8
-4
0
4
8
E/A
(MeV
)
HM
SMFOPI constraint
FOPI density rangeGMR constraint
‣ Phenomenological EOS H M a n d S M i n c l u d e t h e saturation point at ρ/ρ0 = 1, E/A = −16 MeV by construction.
‣ ➜ fixes the absolute position of the curves:
‣ the heavy ion data are only sensitive to the shape, i.e. the pressure (derivative).
‣ ➜ a stiff EOS, characterised by K 0 = 3 8 0 M e V i s n o t i n agreement with the flow data in the incident energy range 0.4 - 1.5 A.GeV. !
7
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
‣ Phenomenological EOS H M a n d S M i n c l u d e t h e saturation point at ρ/ρ0 = 1, E/A = −16 MeV by construction.
‣ ➜ fixes the absolute position of the curves:
‣ the heavy ion data are only sensitive to the shape, i.e. the pressure (derivative).
‣ ➜ a stiff EOS, characterised by K 0 = 3 8 0 M e V i s n o t i n agreement with the flow data in the incident energy range 0.4 - 1.5 A.GeV. !
7
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Constraining the stiffness of the EOS with the elliptic flow.
‣ Phenomenological EOS H M a n d S M i n c l u d e t h e saturation point at ρ/ρ0 = 1, E/A = −16 MeV by construction.
‣ ➜ fixes the absolute position of the curves:
‣ the heavy ion data are only sensitive to the shape, i.e. the pressure (derivative).
‣ ➜ a stiff EOS, characterised by K 0 = 3 8 0 M e V i s n o t i n agreement with the flow data in the incident energy range 0.4 - 1.5 A.GeV. !
7
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Which density has been probed?
IQMD transport model[5,6] various phenomenological EOS’s: » ‘stiff’ = H & HM (+
momentum dependent), K0 = 380 MeV
» ‘soft’ = S & SM (+momentum dependent), K0 = 200 MeV.
Here: protons in Au+Au at 1.5 A.GeV, b=3 fm
= time / passing time
Density
Number of collisions
Mean-field momentum transfer
at centre-of-mass
full target-projectile overlap
Purpose = characterise which ’typical’ densities where probed in the FOPI experiments => at which time V2 develops, and which conditions influence it the most.
8
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Which density has been probed?
UrQMD Au+Au at 1.5 A.GeV, b=3 fm
>0.4)t0
(u0
y-1 -0.5 0 0.5 1
2V
0
0.05
0.1scaled1.5 A.GeV - SM - t
0.390.781.051.633.92
‣ The elliptic flow in his final dependence with rapidity develops fast: during the passing time.
9
‣ The elliptic flow in strength and shape is mostly influenced by the force of the mean field
‣ The ’ typ ica l ’ dens ity of the ’measured’ EOS can be built from the mean value weighted by this force up to the passing time.
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Simulations: the scenario
UrQMD Au+Au at 1.5 A.GeV, b=3 fm
‣ The density range, relevant to the EOS evidenced by the FOPI Collaboration, spans in the range ρ = (1.25 − 2.0) ρ0.
10
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
E=E1kin +E2
kin +V1+V2
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
2) Take randomly 1 nucleon out of one fragment
E=E1kin +E2
kin +V1+V2
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
2) Take randomly 1 nucleon out of one fragment
E=E1kin +E2
kin +V1+V2
3) Add it randomly to another fragment
E’=E1’kin +E2’
kin +V1’+V2’
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
2) Take randomly 1 nucleon out of one fragment
E=E1kin +E2
kin +V1+V2
3) Add it randomly to another fragment
E’=E1’kin +E2’
kin +V1’+V2’
If E’ < E take the new configuration
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
2) Take randomly 1 nucleon out of one fragment
E=E1kin +E2
kin +V1+V2
3) Add it randomly to another fragment
E’=E1’kin +E2’
kin +V1’+V2’
If E’ < E take the new configurationIf E’ > E take the old with a probability depending on E’-E
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
2) Take randomly 1 nucleon out of one fragment
E=E1kin +E2
kin +V1+V2
3) Add it randomly to another fragment
E’=E1’kin +E2’
kin +V1’+V2’
If E’ < E take the new configurationIf E’ > E take the old with a probability depending on E’-ERepeat this procedure very many times...
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
![Page 27: Constraining the nuclear matter equation of state using ... · Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool Constraining the nuclear matter equation of state using the](https://reader034.vdocuments.net/reader034/viewer/2022052104/603fc584ced7fd10020adfb6/html5/thumbnails/27.jpg)
Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
11
2) Take randomly 1 nucleon out of one fragment
E=E1kin +E2
kin +V1+V2
3) Add it randomly to another fragment
E’=E1’kin +E2’
kin +V1’+V2’
If E’ < E take the new configurationIf E’ > E take the old with a probability depending on E’-ERepeat this procedure very many times... It leads automatically to the most bound configuration.
2 steps: 1) Pre-select good «candidates» for fragments according to proximity criteria: real space coalescence = Minimum Spanning Tree (MST) procedure.
!* Simulated Annealing Procedure: PLB301:328,1993; later called SACA. * P.B. Gossiaux, R. Puri, Ch. Hartnack, J. Aichelin, Nuclear Physics A 619 (1997) 379-390 * 2010 version: publication in progress…
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
12
Ingredients of the binding energy of the clusters : ① Volume component: mean field (Skyrme, dominant), for NN, NΛ (hypernuclei) ② Surface effect correction: Yukawa term.
③ Asymmetry energy : 23.3 MeV.(<ρ’B>)(γASY-1).(<ρ’n>-<ρ’p>)2/<ρ’B> ④ Extra « structure » energy (N,Z,ρ) = BMF(ρ).((Bexp-BBW)/(BBW-BCoul-Basy))(ρ0)
⑤ 3He+n recombination. ⑥ Secondary decay: GEMINI.
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
12
Ingredients of the binding energy of the clusters : ① Volume component: mean field (Skyrme, dominant), for NN, NΛ (hypernuclei) ② Surface effect correction: Yukawa term.
③ Asymmetry energy : 23.3 MeV.(<ρ’B>)(γASY-1).(<ρ’n>-<ρ’p>)2/<ρ’B> ④ Extra « structure » energy (N,Z,ρ) = BMF(ρ).((Bexp-BBW)/(BBW-BCoul-Basy))(ρ0)
⑤ 3He+n recombination. ⑥ Secondary decay: GEMINI.
➲ Remarks:
• Advantage of SACA : the fragment partitions can reflect the early dynamical conditions (Coulomb, density, flow details, strangeness...). Fragment partitions already determined at the passing time of the colliding system.
• In the framework of QMD, HSD, <ρclusters> ≺ 0.5. ρ0 ⇒ isotope yields of SACA with Easy probe it
at sub-saturation densities
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
13
simple coalescence no Basy, no Bstruct. Basy, no Bstruct. Basy, + Estruct.
IQMD-SACA central Xe+Sn @ 100 A.MeV
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
SACA: a clusterisation approach…
13
simple coalescence no Basy, no Bstruct. Basy, no Bstruct. Basy, + Estruct.
IQMD-SACA central Xe+Sn @ 100 A.MeV
FOPI
W. Reisdorf and the FOPI Collaboration NPA 848 (2010) 366–427
IQMD-SACA
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool 14
Another application of SACA : hypernuclei production
Λ
np
ΛtIQMD+SACA 58Ni+58Ni
at 1.91 A.GeV (b < 6 fm) -
tcluster.=20 fm/c
Z hypernuclei0 1 2 3
A hy
pern
ucle
i
1
2
3
4
5
6
-610
-510
-410
-310
-210
= 20fm/c) - soft+mdi, kaon pot.cluster.
Ni at 1.93 A.GeV (b < 6 fm, t58Ni+58IQMD+SACA
Soft EOS with m.d.i. with Kaon pot.
n-Λ p-Λ
Λ3H
Λ4He
Λ5He
Λ6He
Λ4H
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
15
Directed flow
FOPI Collaboration / NPA 876 (2012) 1-60
FOPI γasy = 1
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
15
Directed flow
FOPI Collaboration / NPA 876 (2012) 1-60
FOPI γasy = 1γasy = 0.5
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
15
Directed flow
FOPI Collaboration / NPA 876 (2012) 1-60
FOPI γasy = 1γasy = 0.5γasy = 1.5
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
16
γasy = 1
FOPI Collaboration / NPA 876 (2012) 1-60Elliptic flow
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
16
γasy = 1
FOPI Collaboration / NPA 876 (2012) 1-60Elliptic flow
!The differences in t/3He elliptic flow increases with energy
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
17
FOPI
PRELIMINARY
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Towards the determination of the stiffness of the asymmetry energy.
18
The higher the bombarding energy, the stronger the sensitivity.
at mid-rapidity
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
‣ The spectator clock can presumably be used to try to extend improved EOS constraints to densities (3-4 ρ0) in future accelerator systems such as FAIR.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
‣ The spectator clock can presumably be used to try to extend improved EOS constraints to densities (3-4 ρ0) in future accelerator systems such as FAIR.
‣ Beyond 4 A.GeV, other ideas are needed to extract EOS information from heavy ion data.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
‣ The spectator clock can presumably be used to try to extend improved EOS constraints to densities (3-4 ρ0) in future accelerator systems such as FAIR.
‣ Beyond 4 A.GeV, other ideas are needed to extract EOS information from heavy ion data.
‣ A realistic treatment of the clusterisation is needed to account for e.g. Easymmetry effects.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
‣ The spectator clock can presumably be used to try to extend improved EOS constraints to densities (3-4 ρ0) in future accelerator systems such as FAIR.
‣ Beyond 4 A.GeV, other ideas are needed to extract EOS information from heavy ion data.
‣ A realistic treatment of the clusterisation is needed to account for e.g. Easymmetry effects.
‣ The stiffness of the asymmetry energy can be discriminated by the shape (v2n) the elliptic flow over a large range of rapidity (not only mid-rapidity) of 3He and tritons. -> Prelimininary indication of 0.5<= γasy < 1 by confronting IQMD-SACA to FOPI data.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
‣ The spectator clock can presumably be used to try to extend improved EOS constraints to densities (3-4 ρ0) in future accelerator systems such as FAIR.
‣ Beyond 4 A.GeV, other ideas are needed to extract EOS information from heavy ion data.
‣ A realistic treatment of the clusterisation is needed to account for e.g. Easymmetry effects.
‣ The stiffness of the asymmetry energy can be discriminated by the shape (v2n) the elliptic flow over a large range of rapidity (not only mid-rapidity) of 3He and tritons. -> Prelimininary indication of 0.5<= γasy < 1 by confronting IQMD-SACA to FOPI data.
‣ The same can be obtained via the ratio of the elliptic flow values of neutrons and protons.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Summary and discussion
‣ A single parameter v2n, characterising the elliptic flow over a large rapidity interval, for protons and other light isotopes -> clear discrimination for soft EOS.
‣ Relevant density range: estimated from the simulations to span ρ = (1.25 − 2.0)ρ0.
‣ The spectator clock can presumably be used to try to extend improved EOS constraints to densities (3-4 ρ0) in future accelerator systems such as FAIR.
‣ Beyond 4 A.GeV, other ideas are needed to extract EOS information from heavy ion data.
‣ A realistic treatment of the clusterisation is needed to account for e.g. Easymmetry effects.
‣ The stiffness of the asymmetry energy can be discriminated by the shape (v2n) the elliptic flow over a large range of rapidity (not only mid-rapidity) of 3He and tritons. -> Prelimininary indication of 0.5<= γasy < 1 by confronting IQMD-SACA to FOPI data.
‣ The same can be obtained via the ratio of the elliptic flow values of neutrons and protons.
➲ See AsyEOS experiment: ongoing analysis, forthcoming talks by P. Russotto and J. Brzychczyk.
19
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Comparison to microscopic calculations
Katayama 2013± Sym--- Au
0.5 1.0 1.5 2.0l/ l0
-16
-12
-8
-4
E/A
(MeV
)
Dirac-Brueckner-Hatree-Fock (DBHF) calculation[10] using the Bonn A[11] nucleon-nucleon potential
(three representative microscopic calculations compared with our new constraints)
[10] R. Brockmann, R. Machleidt, Phys. Rev. C 42 (1990) 1965.
[11] T. Katayama, K. Saito, Phys. Rev. C 88 (2013) 035805. 20
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Comparison to microscopic calculations
Sammarruca 2012� DBHF6 Chiral
0.5 1.0 1.5 2.0l/ l0
-16
-12
-8
-4
E/A
(MeV
)
(three representative microscopic calculations compared with our new constraints)
2 symmetric nuclear matter EOS’s from [12]:
1) ’DBHF’ = meson theoretic potential together with the DBHF method 2) ’Chiral’= use of effective field theory (EFT) with density dependent interactions derived from leading order chiral three-nucleon forces.
[12] P. Danielewicz, G. Odyniec, Phys. Lett. B 157 (1985) 168. 21
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool
Comparison to microscopic calculations
Fritsch 2005--- / 2/ N± / 2/ N 6
0.5 1.0 1.5 2.0l/ l0
-16
-12
-8
-4
E/A
(MeV
)
(three representative microscopic calculations compared with our new constraints)
Using the chiral approach[13]: 2 rather different EOS’s including or not virtual ∆ excitations. » the virtual ∆-excitations help locate
the EOS at the right horizontal place around ρ = 0.16 fm−3.
» the ∆ leads to a rather marked stiffening of the EOS (K0 = 304 MeV)
» because ’cold’ EOS ? » finite temperature in the reaction =>
the ∆ are real rather than virtual. The theoretical ’∆ stiffness’ could then be a dispersion effect rapidly changing with temperature.
[13] S. Fritsch, N. Kaiser, W. Weise, Nucl. Phys. A 750 (2005) 259. 22
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool Y. Leifels – ASTRO 2013
Beam energy dependence of elliptic flow
v2 at mid-rapidity elliptic flow ➢ pressure gradient of compression
zone ➢ shadowing of spectators ➢ at low energies
− attraction due to mean field of nucleons
➢ at high energies − lacking shadowing of
spectators
23
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool Y. Leifels – ASTRO 2013
Elliptic flow and the nuclear matter EOS
P. Danielewicz et al. Science 298, 1592 (2002)
elliptic flow
24
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Arnaud Le Fèvre - NuSYM14 – 7-9 July 2014 – Liverpool Y. Leifels – ASTRO 2013
Elliptic flow and the nuclear matter EOS
P. Danielewicz et al. Science 298, 1592 (2002)
elliptic flow
side flow
24