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1 Nucleus-Nucleus Collisions in NA49-future An introduction for everybody The main goal of studying nucleus-nucleus collisions in NA49-future is the investigation of the transition between two phases of strongly interacting matter: gas of hadrons and quark-gluon plasma NA49-future

Nucleus-Nucleus Collisions in NA49-future

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Nucleus-Nucleus Collisions in NA49-future. An introduction for everybody. The main goal of studying nucleus-nucleus collisions in NA49-future is the investigation of the transition between two phases of strongly interacting matter:. gas of hadrons. and. quark-gluon plasma. - PowerPoint PPT Presentation

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Page 1: Nucleus-Nucleus Collisions  in NA49-future

1

Nucleus-Nucleus Collisions in NA49-future

An introduction for everybody

The main goal of studying nucleus-nucleus collisions in NA49-future is the investigation of the transition between two phases of strongly interacting matter:

gas of hadrons

and

quark-gluonplasma

NA49-future

Page 2: Nucleus-Nucleus Collisions  in NA49-future

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NA49-future aims to discover the critical point of strongly interacting matter

Tem

pera

ture

Baryochemical potentialNA49-future

Models of strong interactions predict a sharp phase boundary (1st order phase transition) between hadron gas

and quark-gluon plasma ending in a critical point

NA49 at the CERN SPSstudying collisions of

two lead nuclei (Pb+Pb)found evidence for

the transition betweenhadron gas and

quark-gluon plasma

NA49-future will study properties of this transition

in order to establish fundamental features of

strongly interacting matter

Page 3: Nucleus-Nucleus Collisions  in NA49-future

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The main ideas behind the NA49-future nucleus-nucleus program can be related to the well known properties of water

(water properties are determined by electro-magnetic interactions)

Phases of strongly interacting matterPhases of water

NA49-future

Page 4: Nucleus-Nucleus Collisions  in NA49-future

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w

N/

5

10

15

20

25

)1/2

F (GeV

0 1 2 3 4 5-1

0

1

2

FIT(A+A)-(p+p)

+/+

K

0.1

0.2

)1/2

F (GeV

0 5 10 15

) (M

eV)

+T

(K

100

200

300

A+A:NA49AGSRHICp+p

Collision energy

Pro

pert

ies o

f p

rod

uced

had

ron

sHeating curves of strongly interacting matter measuredby NA49 at the CERN SPS serve as evidence for a transition between hadron gas and quark-gluon plasma,

similarly the heating curve of water shows the transitions between the phases of water

Q (heat added)

100

0

Heating of water vapor

Heat used to vaporize water to water vapor

Heating of water

tem

pera

ture

(oC

)

Ice

NA49-future

Page 5: Nucleus-Nucleus Collisions  in NA49-future

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The phase diagram of water

is well established but

the properties of thetransition between hadron

gas and quark-gluon plasmastill have to be uncovered

1st order phase transition NA49-future

Baryochemical potential (MeV)

Tem

pera

ture

(M

eV

)

NA49-future

??

critical point

Page 6: Nucleus-Nucleus Collisions  in NA49-future

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In our daily life ...

droplets of water

droplets of stronglyinteracting matter

10-12

the properties of stronglyinteracting matter can bestudied only in collisions

of heavy nucleiNA49-future

Page 7: Nucleus-Nucleus Collisions  in NA49-future

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COLLISIONS OF TWO NUCLEI -the only tool to study properties of

strongly interacting matter in the laboratory

NA49-future

UrQMD

produced particles measuredin the NA49 apparatus

(scale 10 m)

snapshot of the producedmatter after the collision

(scale 10-14 m)

Page 8: Nucleus-Nucleus Collisions  in NA49-future

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LHC

SPS

NA49-future

NA49-future

NA49-future at the CERN SPS

Page 9: Nucleus-Nucleus Collisions  in NA49-future

9

-future

NA49-future

Page 10: Nucleus-Nucleus Collisions  in NA49-future

10

10 20 30 40 80 158

energy (A GeV)

10 20 30 40 80 158

In+In

energy (A GeV)

Pb+Pb

C+C

Si+Si

= 2∙106 registered collisions

NA49 NA49-future

NA49-future

NA49-future plans to perform a comprehensive scan in energy and size of colliding nuclei to study the properties of the transition between hadron gas and quark gluon plasma

p+p

Page 11: Nucleus-Nucleus Collisions  in NA49-future

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10 20 30 40 80 158

energy (A GeV)

In+In

C+C

Si+Si

= 2∙106 registered collisions

NA49-future

New data registered by NA49-future

p+p

ener

gy (A

GeV

)

may lead to a discovery of the criticalpoint of strongly interacting matter

by an observation of a hill of fluctuations

p+pC+C

Si+Si

In+In

20

4080

158

30

Page 12: Nucleus-Nucleus Collisions  in NA49-future

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10 20 30 40 80 158

energy (A GeV)

In+In

C+C

Si+Si

= 2∙106 registered collisions

NA49-future

New data registered by NA49-future

p+p

will uncover properties of the transitionbetween hadron gas and quark-gluonobserved by NA49 in Pb+Pb collisions

10 20 30 40 80 158

energy (A GeV)

Page 13: Nucleus-Nucleus Collisions  in NA49-future

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The NA49-future Collaboration:

101 physicists from 24 institutes and 15 countries:

University of Athens, Athens, GreeceUniversity of Bari and INFN, Bari, ItalyUniversity of Bergen, Bergen, NorwayUniversity of Bern, Bern, SwitzerlandKFKI IPNP, Budapest, HungaryCape Town University, Cape Town, South AfricaJagellionian University, Cracow, PolandJoint Institute for Nuclear Research, Dubna, RussiaFachhochschule Frankfurt, Frankfurt, GermanyUniversity of Frankfurt, Frankfurt, GermanyUniversity of Geneva, Geneva, SwitzerlandForschungszentrum Karlsruhe, Karlsruhe, GermanySwietokrzyska Academy, Kielce, PolandInstitute for Nuclear Research, Moscow, RussiaLPNHE, Universites de Paris VI et VII, Paris, FrancePusan National University, Pusan, Republic of KoreaFaculty of Physics, University of Sofia, Sofia, BulgariaSt. Petersburg State University, St. Petersburg, RussiaState University of New York, Stony Brook, USAKEK, Tsukuba, JapanWarsaw University of Technology, Warsaw, PolandUniversity of Warsaw, Warsaw, PolandRudjer Boskovic Institute, Zagreb, CroatiaETH, Zurich, Switzerland

NA49-future