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4.2 Phases <strong>of</strong> Strongly Interact<strong>in</strong>g Matter<br />

Figure 9. Di-electron <strong>in</strong>variant mass spectra measured by HADES.<br />

The Ar+KCl data (symbols) are compared to a superposition <strong>of</strong> p+p<br />

and p+n data, represented by the shaded area.<br />

<strong>in</strong> Figure 9, which depicts the di-electron <strong>in</strong>variant mass<br />

spectra for Ar+KCl collisions (symbols), and for a superposition<br />

<strong>of</strong> p+p and p+n collisions (shaded area), both<br />

normalised to the measured pion yields. HADES will<br />

systematically study the orig<strong>in</strong> <strong>of</strong> the dilepton excess <strong>in</strong><br />

collisions <strong>of</strong> heavy systems up to Au+Au.<br />

Outlook<br />

Strange particles and dileptons are the most promis<strong>in</strong>g<br />

diagnostic probes <strong>of</strong> nuclear matter at two to three times<br />

saturation density as created <strong>in</strong> nucleus-nucleus collisions<br />

at 1 - 2 A GeV. Strangeness production <strong>in</strong> nuclear<br />

collisions is be<strong>in</strong>g systematically <strong>in</strong>vestigated by the<br />

FOPI collaboration at GSI. With<strong>in</strong> this study, experimental<br />

evidence for the existence <strong>of</strong> a strange dibaryon decay<strong>in</strong>g<br />

<strong>in</strong>to a Lambda and a proton was found. The HADES<br />

collaboration has also started a strangeness programme,<br />

and identified double-strange Ξ hyperons at deep subthreshold<br />

beam energies. HADES identified for the first<br />

time ω mesons via the dilepton channel <strong>in</strong> collisions<br />

between light nuclei at low energies. These measurements<br />

should be cont<strong>in</strong>ued and extended to heavy<br />

collision systems, both for strangeness and dileptons.<br />

The theoretical conjecture <strong>of</strong> a fi rst-order deconf<strong>in</strong>ement<br />

phase transition and a QCD critical endpo<strong>in</strong>t<br />

exist<strong>in</strong>g at large baryon-chemical potentials, together<br />

with the <strong>in</strong>trigu<strong>in</strong>g observations made <strong>in</strong> heavy ion<br />

collisions at low SPS energies, triggered new experimental<br />

activities at the major heavy ion laboratories:<br />

the beam energy scan programme at RHIC, the fixedtarget<br />

NA61/SHINE experiment at CERN-SPS, the NICA<br />

collider project at JINR <strong>in</strong> Dubna, and the proposed<br />

fixed-target Compressed Baryonic Matter (CBM) experiment<br />

at FAIR.<br />

The collider experiments at RHIC and NICA have<br />

the advantage <strong>of</strong> a constant acceptance as function<br />

<strong>of</strong> beam energy. On the other hand, when runn<strong>in</strong>g at<br />

low beam energies, collider experiments are restricted<br />

to the measurement <strong>of</strong> abundantly produced particles<br />

due to limitations <strong>in</strong> lum<strong>in</strong>osity. The same is true for<br />

the experiment NA61/SHINE at the SPS, which operates<br />

at max. 80 Hz (although SPS could deliver much<br />

higher <strong>in</strong>tensities). In contrast, the experiments at FAIR<br />

are designed for extremely high lum<strong>in</strong>osities, enabl<strong>in</strong>g<br />

the systematic measurement <strong>of</strong> multi-differential cross<br />

sections with unprecedented statistics even for rare<br />

diagnostic probes like multi-strange hyperons, lepton<br />

pairs, charmonium and open charm.<br />

The SIS-100 accelerator at FAIR will deliver heavy ion<br />

beams with energies up to 14 A GeV to the HADES and<br />

CBM experimental setups. This energy range is ideally<br />

suited to produce and to <strong>in</strong>vestigate net baryon densities<br />

as they exist <strong>in</strong> the cores <strong>of</strong> neutron stars. For the first<br />

time, penetrat<strong>in</strong>g probes like dileptons and multi-strange<br />

particles such as Ω-hyperons will be used to study systematically<br />

the properties <strong>of</strong> baryonic matter <strong>in</strong> this beam<br />

energy range. The 30 GeV proton beams from SIS-100<br />

will allow pioneer<strong>in</strong>g measurements to be performed on<br />

(open) charm production at threshold energies, as well as<br />

the detailed study <strong>of</strong> charm propagation <strong>in</strong> cold nuclear<br />

matter. The SIS-300 accelerator will deliver high-<strong>in</strong>tensity<br />

heavy ion beams with energies up to 45 A GeV to the<br />

high-rate CBM experiment provid<strong>in</strong>g excellent conditions<br />

for the <strong>in</strong>vestigation <strong>of</strong> the QCD phase diagram at large<br />

baryon-chemical potentials.<br />

92 | <strong>Perspectives</strong> <strong>of</strong> <strong>Nuclear</strong> <strong>Physics</strong> <strong>in</strong> <strong>Europe</strong> – NuPECC Long Range Plan 2010

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