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Production of strange - PPT Presentation

particles and hypernuclei in nuclear reactions at a few GeV New capabilities in the INCL intranuclear cascade model JeanChristophe David DPhN Nuclear Science Department ID: 742145

strange production hypernuclei particles production strange particles hypernuclei incl results gev data phys model exp abla intranuclear cascade rev

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Slide1

Production of strange particles and hypernuclei in nuclear reactions at a few GeV.New capabilities in the INCL intranuclear cascade model.

Jean-Christophe David

DPhN(Nuclear Science Department)

The 13

th

International Conference on Hypernuclear and Strange Particle PhysicsJune 24-29, 2018 – Portsmouth (USA)Slide2

IntroductionProduction of strange particles and hypernuclei in INCLProduction of

strange particles and

hypernuclei in nuclear reactions at a few GeV

.New

capabilities

in the INCL intranuclear cascade model.

So-

called

spallation

reactions

Reaction

between

a light projectile and a nucleus

Divided

in 2

steps

an

intranuclear

cascade

de-excitation of a hot nucleusSlide3

IntroductionProduction of strange particles and hypernuclei in INCLProduction of

strange particles and

hypernuclei in nuclear reactions at a few

GeV.

New capabilities

in the INCL intranuclear cascade model.

INCL

treats

the first

step

 ~2010: up to 2-3

GeV

2011: up to ~15

GeV

(

multipions

)

Combined

to

Abla

for the de-excitationSlide4

IntroductionProduction of strange particles and hypernuclei in INCLProduction of

strange particles and hypernuclei

in nuclear reactions at a few GeV

.New

capabilities

in the INCL intranuclear cascade model.INCL

treats

the first

step

 ~2010: up to 2-3

GeV

2011: up to ~15

GeV

(

multipions

)

2018: K,

L

,

S

added

improved

high

energies

open new

possibilities

strange

particle

emission

hypernucleus

production

Combined

to

Abla

for the de-excitation

L

evaporation

+

Hyperfission

addedSlide5

IntroductionProduction of strange particles and hypernuclei in INCLProduction of

strange particles and hypernuclei

in nuclear reactions at a few GeV.

New capabilities

in the INCL intranuclear

cascade model.INCL treats the first step

 ~2010: up to 2-3

GeV

2011: up to ~15

GeV

(

multipions

)

2018: K,

L

,

S

added

improved

high

energies

open new

possibilities

strange

particle

emission hypernucleus production Combined to Abla for the de-excitation L evaporation + Hyperfission added

With

A

renewal

interest

of

hypernucleus

studies

INCL/

Abla

in Geant4Slide6

PlanProduction of strange particles and hypernuclei in INCLIngredients of the models

ResultsK production

L productionHypernucleus productionSlide7

IngredientsProduction of strange particles and hypernuclei in INCLIN

CL

sreaction(prod./scatt./abs.) From exp. data, symmetries, models, hypotheses

(E,

Q) output particles From

exp. data, or isotropy, or phase-spaceNuclear Potential L:-28 / S:16 / K+:25 / K

-

:-60 / K

0

:15 / K

0

:-50 MeV

Decay

Not in the nucleus,

except

S

0Slide8

IngredientsProduction of strange particles and hypernuclei in INCLIN

CL

sreaction(prod./scatt./abs.) From exp. data, symmetries, models, hypotheses

(E,

Q) output particles From

exp. data, or isotropy, or phase-spaceNuclear Potential L:-28 / S:16 / K+:25 / K

-

:-60 / K

0

:15 / K

0

:-50 MeV

Decay

Not in the nucleus,

except

S

0

No

resonances

!

Only

final states (

decay

products

) are

taken

into

accountAll details

in J. Hirtz et al.,

submitted

to EPJ+

And a

study

about V

L

(A)

in J.L. Rodriguez-Sanchez et al.,

submitted

as Rapid Communication in PRCSlide9

Production of strange particles and hypernuclei in INCLDifficulty finding elementary cross sections!1

st set (382 channels)17%,

from experiments 18%, using isospin

symmetry at initial/final states

37%,

using isospin symmetry at intermediate steps (Feynman

diagrams

)

28%,

from

models

and

hypotheses

100%

2

nd

set

from

models

and

hypotheses

IngredientsSlide10

Results Production of strange particles and hypernuclei in INCLSlide11

Results Production of strange particles and hypernuclei in INCLKaon - HyperonSlide12

Production of strange particles and hypernuclei in INCLResults – K+

productionSlide13

Production of strange particles and hypernuclei in INCLKAOS - W. Scheinast et al., PRL 96, 072301 (2006)

Results – K+ productionSlide14

Production of strange particles and hypernuclei in INCLKAOS - W. Scheinast et al., PRL 96, 072301 (2006)Results – K-

productionSlide15

Production of strange particles and hypernuclei in INCLLBL - S. Schnetzer et al., Phys. Rev. C 40, 640(1989)Results – K

+ productionSlide16

Production of strange particles and hypernuclei in INCLLBL - S. Schnetzer et al., Phys. Rev. C 40, 640(1989)Results – K

+ productionSlide17

Production of strange particles and hypernuclei in INCLLBL - S. Schnetzer et al., Phys. Rev. C 40, 640(1989)Results – K

+ productionSlide18

Production of strange particles and hypernuclei in INCLLBL - S. Schnetzer et al., Phys. Rev. C 40, 640(1989)Results – K

+ productionSlide19

Production of strange particles and hypernuclei in INCLM. Büscher et al., Eur. Phys. J. A 22, 301-317(2004)Thanks Nikolai Mokhov for LAQGSM data

Results – K+ production

Forward

directionSlide20

Production of strange particles and hypernuclei in INCLResults – K+ production – High energy

E-802 Collaboration Phys

. Rev. D 45, 3906 (1992)Slide21

Production of strange particles and hypernuclei in INCLHADES Collaboration, T.Gaitanos and J. Weil,Phys. Rev. C 90, 054906 (2014)Results – K

0s production

INCL

overestimates

, but a part

explained by…C.-M. Herbach et al.,NIMA 562 (2006) 729–732

s

R

(

p+Nb

– 1.2

GeV

):

1063+/-40 mbSlide22

Production of strange particles and hypernuclei in INCLResults – L production

HADES Collaboration, Eur

. Phys. J. A (2014) 50:81Slide23

HADESmeasurementGeant4 simulationUrQMD simulationHADES

result

Efficiency

Production of

strange

particles

and

hypernuclei

in INCLSlide24

Production of strange particles and hypernuclei in INCL

Results – L

production(efficiency included

)

« 

Momentum content » beyond ~y=0.8 different from one model to another (UrQMD,

GiBUU

, INCL)

Extrapolation in the «

blind

» zone

difficult

(model

dependent

)Slide25

ResultsProduction of strange particles and hypernuclei in INCLHypernucleiSlide26

Results - HypernucleiProduction of strange particles and hypernuclei in INCLSlide27

Results - HypernucleiProduction of strange particles and hypernuclei in INCLSlide28

ConclusionsProduction of strange particles and hypernuclei in INCL Strangeness implemented

in INCL (and Abla) … and INCL/Abla in Geant4 Ingredients not always

well known…...However, results quite good compared to exp. data or other modelsK+ production: OK in momenta and angles At forward emission angle data are missing Role of

DN-induced channels . important at low Ep . improvement of elementary

s needed

K- production: Some key channels seem missing in INCLK0 production: A possible slight overestimation, but exp. data neededL production: Exp. data are too scarce to conclude, but encouragingHypernucleus: Good results but too scarce data

Future

Improvements...

X

added ?

New projectiles (e

-

, p) ?Slide29

CollaboratorsJason Hirtz (PhD) INCLJose Luis Rodriguez Sanchez (Post-Doc) AblaAlain Boudard, Joseph Cugnon, Sylvie Leray, Davide Mancusi, Georg SchnabelSlide30

Thank you!Production of strange particles and hypernuclei in INCL