238 U 4+ 20 Ne 1+ A/z (after stripping) 2,8 3,3 2,0 Stripping Efficiency [%] 20 15 90 Magnetic Rigidity [Tm] (before Stripping) 3,0 4,1 1,4 Magnetic Rigidity [Tm] (after Stripping) 1,3 1,6 1,0 Beam Intensity [...] Transfer Line (TK) MUCIS, MEVVA PIG HSI (RFQ, IH1, IH2) LEBT HLI (ECR, RFQ, IH) Gas Stripper Poststripper (Alvarez, Cav.) TK to SIS18 TK_1 (entrance) Foilstripper TK_9 (exit) Bunch Frequency 36.136 MHz [...] MHz 36.136 MHz W [MeV/u] 11,4 11,4 11,4 β [%] 15,591 15,591 15,591 100% Horizontal Rms-Emittance, norm. [mm·mrad]* 0,349 0,351 0,345 100% Vertical Rms-Emittance, norm. [mm·mrad]* 0,298 0,454 0,532 95% L

Poststripper MUCIS, MEVVA PIG HSI (RFQ, IH1, IH2) LEBT HLI (ECR, RFQ, IH) Gas Stripper Poststripper (Alvarez, Cav.) TK to SIS18 Alvarez 1 Alvarez 2 Alvarez 3 Alvarez 4 Frequency 108.41 MHz 108.41 MHz 108 [...] Energy [MeV/u] 3,6 5,9 8,6 11,4 β [%] 8,761 11,216 13,514 15,591 100% Horizontal Rms-Emittance, norm. [mm·mrad] 0,244 0,269 0,320 0,349 100% Vertical Rms-Emittance, norm. [mm·mrad] 0,306 0,287 0,301 0,298 [...] (ER’s) Number 15 Max. effective Beschleunigungsspannung [MV pro ER] 1,2 130 Xe 21+ 238 U 28+ 20 Ne 7+ Max. Acceleration Voltage [MeV/u] 2,9 2,1 6,3 Max. Beam Energy [MeV/u] 14,3 13,5 17,7

Efficiency [%] 15,0 12,0 40,0 Magnetic Rigidity [Tm] (before Stripping) 11,1 10,1 3,4 Magnetic Rigidity [Tm] (after Stripping) 1,1 1,4 0,5 Beam Intensity [emA] (at Gasstripper) 169,6 105,0 35,0 Beam Intensity [...] 136 MHz 36.136 MHz β [%] 5,473 5,473 5,473 100% Horizontal Rms-Emittance, norm. [mm·mrad]* 0,111 0,122 0,225 100% Vertical Rms-Emittance, norm. [mm·mrad]* 0,111 0,123 0,296 95% Longitudinal Rms-Emittance [...] (at Gasstripper) 29,4 25,0 2,8 Power (average) [kW] (Duty Factor 2 %) (at Alvarez Entrance) 4,4 3,0 1,1 The quoted beam intensties and beam power values refer to the theoretical current limit of the prestripper

2.537 2.537 - 5.398 100% Horizontal Rms-Emittance, norm. [mm·mrad] 0.1 - 1.5 100% Vertical Rms-Emittance, norm. [mm·mrad] 0.1 - 1.5 100% Longitudinal Rms-Emittance [keV/u·ns] 1.3 - 1.8 Energy spread [keV/u] [...] High Charge Injector (HLI) MUCIS, MEVVA PIG HSI (RFQ, IH1, IH2) LEBT HLI (ECR, RFQ, IH) Gas Stripper Poststripper (Alvarez, Cav.) TK to SIS18 Resonator RFQ Buncher IH-DTL Frequency 108.408 MHz 108.408 [...] 0.265 48 Ca 2+ (A/z = 4.8) Max. Electrode Voltage [kV] 44 - 240 Effective Acceleration Voltage [MV] 1.428 - 5.088 RF-Power, Pulse [kW] 61.714 - 54.958 RF-Power (avg.), Duty Factor 25% [kW] 15.429 - 13.739

Length [m] 9,35 0,8 9,1 10,3 Inner Tank Diameter [m] 0,762 0,86 1,829 2,034 Energy Range [keV/u] 2.2 -120 120 120 - 743 743 -1395 β [%] 0.217-1.605 1,605 1.605-3.995 3.995-5.473 100% Horizontal Rms-Emittance [...] (average), Duty Factor 2% [kW] 5 1 17 18 Beam Power [kW] 106 - 560 591 20 Ne 1+ (A/z = 20) Max. Electrode Voltage [kV] 42 65 354 323 Effective Acceleration Voltage [MV] 2,4 - 12,5 13,1 RF-Powerloss, Pulse [kW] [...] Injector (HSI) MUCIS, MEVVA PIG HSI (RFQ, IH1, IH2) LEBT HLI (ECR, RFQ, IH) Gas Stripper Poststripper (Alvarez, Cav.) TK to SIS18 Resonator RFQ Superlense IH1 IH2 Frequency 36.136 MHz 36.136 MHz 36.136

beam: heating nhelix laser beam: diagnostics 3 < Z < 92 0.3 -1 kJ @ 1 - 15 ns, 2w (2010) 100 J @ 6 -14 ns E = 3 -13 MeV/u 50 J @ 0.5 - 2 ps = 100 TW (compressed 12 cm beam) 5 J @ 0.5 ns (Thomson scattering) [...] 108/36 MHz, Δtion = 3 ns (FWHM) 300 J @ ~ ns (broad spectral width) <1 mJ @ 0.5 ns (interferometry) Parameter PHELIX Wert Langpuls Pulslänge 1,5 - 20 ns Langpuls Energie bis zu 250 J Langpuls Wellenlänge 527 [...] Lasern ein kleiner Laser, der bei 355 nm Wellenlänge einen 500 ps langen Puls mit einer Energie von 1 mJ liefert. Dieser wird für Interferometriemessungen verwendet, mit denen z.B. die Elektronendichte

Argonne, USA, Report ANL/PHY-97/1, p. 259-264 Heavy and superheavy nuclei S. Hofmann Proceedings of the Int. Conf. on Nuclear Structure Around the Turn of the Century, July 1-6, 1996, Crete, Greece; Z. Phys [...] superheavy elements in cold fusion reactions Denisov, V.Yu. and Hofmann, S. Phys. Rev. C61, 034606-1-15, 2000 Effect of the entrance channel on the synthesis of superheavy elements G. Giardina, S. Hofmann [...] Quint, B., Schött, H.J., Zychor, I., Leino, M.E., and Gollerthan, U. GSI Annual Report 1985, GSI-86-1, p. 29, 1986 Evidence for 264 108, the Heaviest Known Even-Even Isotope G. Münzenberg, P. Armbruster

Quark Matter (SQM 2019) Jun 10-15, 2019, Bari, Italy Low-x 2019 Aug 26-Sep 1, 2019, Nicosia, Cyprus ALICE FSP Meeting 2019 Sep 1-3, 2019, Seeon, Deutschland 16th SPARC Topical Worksho p Sep 9-13, 2019, Jena [...] Supported Conferences, Workshops and Events 2024 Physics opportunities with proton beams at SIS100 Feb 06-09, 2024, Wuppertal, Germany Gravitational Wave Probes of Fundamental Physics (GWPFP24) Feb 12-16 [...] Conditions Jul 27-29, 2022, Trondheim, Norway 14th Quark Confinement and the Hadron Spectrum Conference Aug 1-6, 2022, Stavanger, Norway Diffraction and Low-x 2022 Sep 24-30, 2022, Cosenza, Italy International

target is installed carrying away the heat radiation from the targets. The low cross section regime (<1pb = 1 SHE event/10days) for the synthesis of SHE requires even higher beam intensities than the ones accepted [...] compounds providing higher melting points are also under investigation. Some of the projectiles (1 pb : 1 fusion per ~ 3 . 10 18 particles) coming from the UNILAC fuse with a target particle and build an [...] efficiency reasons built as a velocity filter with separated fields (2 electrostatic fields E1 and E2 and 4 dipole magnets M1-M4) in a mirrorsymmetric arrangement with respect to central separation plane - the

al program had been started to investigate nuclear structure of isotopes in the element range Z ≥ 100 by means of α - γ - decay spectroscopy. Of special interest is the region of strongly deformed nuclei [...] An overview of isotopes that have been investigated at SHIP within the last decade is given in fig. 1. Present techniques allow for detailed nuclear structure investigations up to isotopes with production [...] are in progress or considered in next future will pin down the cross section limit to approximately 1 pb. Then, nuclear structure investigations of superheavy element up to Z = 118 will be in reach. Highlights