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1. GSI and FAIR
![Aerial view of the GSI campus, April 2024.](/fileadmin/_processed_/8/f/csm_FAIR_Construction_Site_April_24___D._Fehrenz__GSI_FAIR11_8ab40960fb.jpg)
![Aerial view of the FAIR construction site, April 2024.](/fileadmin/_processed_/e/3/csm_FAIR_Construction_Site_April_24___D._Fehrenz__GSI_FAIR17_e5353bb0d8.jpg)
![Visualization of the future FAIR facility. Visualization of the future FAIR facility.](/fileadmin/_processed_/7/2/csm_FAIR_ion42_2022_Render-07_Aerial_mit-PH_6063ec65b4.jpg)
![Visualization of the future FAIR facility. Visualization of the future FAIR facility.](/fileadmin/_processed_/1/c/csm_FAIR_ion42_2022_Render-08_Aerial_mit-PH_6e35870385.jpg)
2. GSI and FAIR accelerator facility
2.1 Ion sources
The ion sources are the starting point of the GSI/FAIR accelerator facility. Here ions from all (natural) elements of the periodic table can be created with the help of high voltage (up to 300 000 V). Subsequent they can get accelerated in the linear and the ring accelerator.
![Ion sources - starting point of the accelerator facility Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/9/e/csm_GSI_FAIR_Ionenquellen_1_0572e9d194.jpg)
2.2 Linear Accelerator UNILAC
The linear accelerator UNILAC (UNIversal Linear ACcelerator) has a length of 120 meters. Ions, e.g. charged atoms of all chemical elements can be accelerated up to 20 percent of the speed of light (60,000 km/s) with this unit. The inside is only visible during maintenance work. The UNILAC is composed of three different consecutive accelerator structurees.
![Linear accelerator UNILAC. Photo: J. Hosan/HA Hessen Agentur](/fileadmin/_processed_/7/0/csm_GSI_FAIR_UNILAC_1_7b909125ac.jpg)
![Linear Accelerator UNILAC – Exterior View. Foto: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/6/1/csm_1_GSI_UNILAC_Aussen_1_02_5ab4feaddb.jpg)
![Linear Accelerator UNILAC – Exterior View. Foto: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/1/3/csm_2_GSI_UNILAC_Aussen_2_598f20565e.jpg)
![Linear Accelerator UNILAC – Interior View of the Alvarez Structure. Foto: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/2/e/csm_3_GSI_UNILAC_Innen_1_7d07a2efab.jpg)
![Linear Accelerator UNILAC – Interior View of the Alvarez Structure. Foto: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/c/2/csm_4_GSI_UNILAC_Innen_2_425d66aa1c.jpg)
![Linear Accelerator UNILAC – Interior View of the Alvarez Structure. Foto: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/2/8/csm_5_GSI_UNILAC_Innen_3_257da7b014.jpg)
![Linear Accelerator UNILAC – Interior View of the Alvarez Structure. Foto: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/8/3/csm_6_GSI_UNILAC_Driftroehren__101b4a528f.jpg)
![Linear accelerator - acceleration structure. Photo: A. Zschau/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/a/5/csm_GSI_FAIR_IH-Struktur_4d5c992385.jpg)
![Linear accelerator - super lense. Photo: A. Zschau/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/1/csm_GSI_FAIR_Superlinse_e55d9fdc55.jpg)
![Linear Accelerator UNILAC – Interior View of the RFQ Structure. Foto: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/c/5/csm_7_GSI_UNILAC_Superlinse_5d65c42b23.jpg)
![Linear Accelerator UNILAC – Interior View of the IH Structure. Foto: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/3/6/csm_9_GSI_UNILAC_RFQ_ca0d88a5d6.jpg)
2.2 Ring Accelerator SIS18
In the heavy-ion synchrotron SIS18 (ger. SchwerIonenSynchrotron) with a circumference of 216 meters he ion beam is further accelerated up to 90 percent of the speed of light (270,000 km/s) in the course of several hundred thousand circulations.
![Heavy-ion synchrotron SIS18 - exterior view. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/e/csm_GSI_FAIR_SIS18_1_332de13710.jpg)
![Heavy-ion synchrotron SIS18 - exterior view. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/a/0/csm_GSI_FAIR_SIS18_2_5f4340fe8d.jpg)
![High frequency cavity at SIS18 Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/e/0/csm_GSI_FAIR_SIS18_4_9f8032d5a7.jpg)
![Beam diagnosis at SIS18 Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/7/7/csm_GSI_FAIR_SIS18_3_0b5911437d.jpg)
![Electron cooler at SIS18 Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/4/2/csm_GSI_FAIR_SIS18_5_5d3d67433c.jpg)
![Interior View of the Cavity. Photo: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/c/a/csm_3_GSI_SIS_Kavitaet_1_3f58a00115.jpg)
![Kicker magnet at SIS18 Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/5/6/csm_GSI_FAIR_SIS18_6_f23c1c3aa1.jpg)
2.3 Storage Ring ESR
In the storage ring ESR (ger. ExperimentierSpeicherRing) with a circumference of 108 meters ions accelerated in the UNILAC and SIS18 can be stored at very high speeds and used in experiments.
![Experimental storage ring ESR. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/b/5/csm_GSI_FAIR_ESR_1_27b0a6f142.jpg)
![Experiment set up at ESR. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/0/csm_GSI_FAIR_ESR_2_b9ec2e0fbd.jpg)
![Storage Ring ESR – Exterior View. Photo: J. Mai, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/9/7/csm_1_GSI_ESR_1_2dcf3268f6.jpg)
![Storage Ring ESR – Exterior View. Photo: J. Mai, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/4/7/csm_2_GSI_ESR_2_02_fb6a2e8467.jpg)
![Storage Ring ESR – Magnet. Photo: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/0/6/csm_3_GSI_ESR_Magnet_4e8b95e4ec.jpg)
![Storage Ring ESR – Magnet. Photo: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/3/f/csm_4_GSI_ESR_Magnet_2_331264c2c8.jpg)
2.4 Cryring
The Cryring is a storage ring with a circumference of 54 m. It can provide an especially high vacuum of 10-11 mbar. It is the first accelerator ring of the future FAIR facility and plays a crucial role for the testing of FAIR components as well as the control software of the SIS100 accelerator ring.
![Cryring – exterior view. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/0/5/csm_GSI_FAIR_Cryring_5_bc9b4791f8.jpg)
![Cryring – close up. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/2/3/csm_GSI_FAIR_Cryring_1_524b7f1c68.jpg)
![Cryring – close up. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/8/0/csm_GSI_FAIR_Cryring_2_95625bcb82.jpg)
![Cryring – close up. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/4/csm_GSI_FAIR_Cryring_3_281dcb2c9f.jpg)
![Cryring – close up. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/1/csm_GSI_FAIR_Cryring_4_b7c89fc8ef.jpg)
![Electron cooler at Cryring. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/1/5/csm_GSI_FAIR_Elektronenkuehler_8d0096d021.jpg)
2.4 Fragment Separator FRS
The 75 meters long FRS (FRagment Separator) ist located behind the ring accelerator SIS18. It is used to produce rare isotopes of naturally occurring heavy nuclei. Directly after the production they are sent to an experimental site or stored in the ESR.
![Fragment Separator FRS – Exterior View. Photo: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/7/3/csm_GSI_Beschleuniger_FRS_1_f3a169d4d4.jpg)
![Fragment Separator FRS – Exterior View. Photo: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/6/8/csm_GSI_Beschleuniger_FRS_3bc153a327.jpg)
3. Infrastructure
![Main control room. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/1/5/csm_GSI_FAIR_HKR_1_9271d6d8d8.jpg)
![GSI-Infrastructure – Main Control Room. Photo: J. Mai, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/f/9/csm_1_GSI_Hauptkontrollraum_1_8b1cb0df1a.jpg)
![GSI-Infrastructure – Main Control Room. Photo: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/e/1/csm_2_GSI_Hauptkontrollraum_2_feed930a5c.jpg)
![GSI-Infrastructure – Detector Prototype for the Measurement of Ion Bunches. Photo: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/b/c/csm_4_GSI_FAIR_Detektor_Prototyp_822dbfe80e.jpg)
![Detector laboratory - manufacturing of a Multiwire Drift Chamber (MDC) component. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/e/b/csm_GSI_FAIR_Detektorlabor_1_bcbeff7e61.jpg)
![Detector laboratory. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/7/3/csm_GSI_FAIR_Detektorlabor_2_6ef2d8de57.jpg)
![Detector laboratory. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/f/3/csm_GSI_FAIR_Detektorlabor_3_f5fff9594b.jpg)
3.1 Green IT Cube
The Green IT Cube is a high performance computing center used by scientists from GSI and FAIR to analyse the large amounts of data gained in the experiments. In its final assembly it will be one of the largest scientifc computer centers in the world with a cooling power of twelve megawatts. Thanks to an innovative cooling system the Green IT Cube will save 90 percent of the cooling energy compared to other supercomputers and thus is very energy efficient and cost saving.
![Green IT Cube – Outside View G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/2/7/csm_GSI_Green_IT_Cube_2a_3a5bdc483f.jpg)
![Green IT Cube at night G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/e/3/csm_GSI_Green_IT_Cube_Nacht_4671c6a43f.jpg)
![Green IT Cube – Computer Corridor G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/6/2/csm_GSI_Green_IT_Cube_Gang_c40bade500.jpg)
![Inside the Green IT Cube.](/fileadmin/_processed_/d/1/csm_JH004447_d4f5ab45a6.jpg)
![Inside the Green IT Cube. Inside the Green IT Cube.](/fileadmin/_processed_/1/8/csm_GIC_2_140524_b7bfe55b08.jpg)
![Digital Open Lab inside the Green IT Cube Digital Open Lab inside the Green IT Cube](/fileadmin/_processed_/4/8/csm_GIC_3_140524_a184ec1dae.jpg)
![Inside the Green IT Cube.](/fileadmin/_processed_/6/e/csm_JH004451_ebc0f56eb9.jpg)
![Inside the Green IT Cube.](/fileadmin/_processed_/7/3/csm_JH004463_cc2b58abb2.jpg)
![Supercomputer L-CSC G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/9/7/csm_GSI_Green_IT_Cube_L-CSC_1_149505ecaf.jpg)
![Green IT Cube – Interior G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/9/d/csm_GSI_Green_IT_Cube_Innengeruest_b0edfda642.jpg)
![Supercomputer L-CSC T. Ernsting, Hessen schafft Wissen](/fileadmin/_processed_/a/1/csm_GSI_Green_IT_Cube_L-CSC_2_5417b66f07.jpg)
![Green IT Cube goes green G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/8/8/csm_GSI_Green_IT_Cube_Bauarbeiten_6fd77a3f5e.jpg)
4. Experiments
4.1 Heavy Elements
In this field of research scientist try to discover superheavy elements above the naturally occurring uranium with the atomic number 92. GSI hosts two experimental set-up's: SHIP (Separator for Heavy Ion reaction Products) and TASCA (TransActinide Separator and Chemistry Apparatus).
![Ion trap SHIPTRAP. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/e/6/csm_GSI_FAIR_SHIPTRAP_1_fd4a673b9d.jpg)
![Ion trap SHIPTRAP. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/2/2/csm_GSI_FAIR_SHIPTRAP_2_173c0cb78a.jpg)
![SHIP – Target Wheel. Photo: K. Back, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/0/a/csm_2_GSI_SHIP_2_9c9204e129.jpg)
![SHIPTRAP – Ion Trap Attached to SHIP. Photo: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/f/0/csm_6_GSI_SHIPTRAP_ca31ce4b16.jpg)
![TASCA – Detector Setup. Photo: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/4/b/csm_e115-2_01_2efe6c4a45.jpg)
![TASCA – Target Wheel. Photo: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/0/6/csm_8_GSI_TASCA_2_5360af106e.jpg)
4.2 HADES
The detection system HADES (High Acceptance Di-Electron Spectrometer) is one of the largest experiments at GSI. It is used for research on compressed hot nuclear matter produced in collisions of ion beam and target. Several layers of detectors identify different particles based on their charge, velocity or mass.
![HADES detector - rear view. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/a/f/csm_GSI_FAIR_HADES_3_71fb9b8d56.jpg)
![HADES detector - rear view. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/6/d/csm_GSI_FAIR_HADES_4_b1ec2f26e0.jpg)
![HADES with electromagnetic calorimeter (blue) Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/8/a/csm_GSI_FAIR_HADES_7_3f7973a124.jpg)
![HADES detector - set up of electromagnetic calorimeter. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/8/f/csm_GSI_FAIR_HADES_1_90250448b5.jpg)
![HADES from the inside Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/3/b/csm_GSI_FAIR_HADES_8_54cf362180.jpg)
![HADES – RICH Structure. Photo: A. Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/8/6/csm_2_GSI_Hades_seitlich_d2283c0d3e.jpg)
![Target made of gold foils for HADES detector. Photo: G. Otto/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/5/8/csm_GSI_FAIR_HADES_Target_1_4bcf78a41d.jpg)
![HADES detector Photo: T. Ernsting/HA Hessen Agentur](/fileadmin/_processed_/3/1/csm_GSI_FAIR_HADES_6_6a1d03dab3.jpg)
4.3 PHELIX
The high performance and high energy laser PHELIX (Petawatt High-Energy Laser for Ion EXperiments) is used for research in plasma and atomic physics. GSI offers the worldwide unique opportunity to conducted combined experiments with laser and ion beam.
![Starting point of PHELIX laser. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/3/1/csm_GSI_FAIR_PHELIX_1_ff9ed97539.jpg)
![Component of PHELIX laser. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/0/8/csm_GSI_FAIR_PHELIX_2_59fa0ec811.jpg)
![PHELIX – Amplifier. Photo: G. Otto, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/5/9/csm_1_GSI_Phelix_Verstaerker_8aefa56c1f.jpg)
![PHELIX – Experiment Chamber. Photo: T. Hahn, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/8/b/csm_2_GSI_Phelix_Kammer_564219db2f.jpg)
4.4 ALICE-Experiment at CERN in Geneva
The Large Hadron Collider LHC at CERN is the largest accelerator of the world. ALICE (A Large Ion Collider Experiment) belongs to the four large experiments located at LHC. The 25 meters long, 16 meters wide and 16 meters high apparatus weighs approx. 10.000 tons and hosts 18 detection systems. GSI has significantly contributed to two systems, the time projection chamber TPC and the transition radiation detector TRD.
Please note that the CERN terms of use apply to these pictures:
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![ALICE – Detektion System. Photo: CERN](/fileadmin/_processed_/9/0/csm_1_GSI_ALICE_7718ff4422.jpg)
![ALICE – Transition Radiation Detector TRD. Photo: CERN](/fileadmin/_processed_/6/f/csm_2_GSI_ALICE_dfb3acdb7e.jpg)
![ALICE – Time Projection Chamber TPC. Photo: CERN](/fileadmin/_processed_/4/7/csm_3_GSI_ALICE_8c95e60a6b.jpg)
![ALICE – Interior View of the Time Projection Chamber TPC. Photo: CERN](/fileadmin/_processed_/c/9/csm_4_GSI_ALICE_76a6352f9c.jpg)
5. Tumor Therapy
5.1 Cancer Therapy with Ion Beams at GSI
![Therapy – Treatment Facility at GSI. Photo: G. Otto/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/3/4/csm_GSI_FAIR_Therapie_1_fc07ff7cbd.jpg)
![Therapy – Treatment Facility at GSI. Photo: A Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/9/8/csm_1_GSI_Therapie_1_2dd8a57f01.jpg)
![Therapy – Treatment Facility at GSI. Photo: A Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/9/8/csm_2_GSI_Therapie_2_1546e26754.jpg)
![Therapy – Model of a Tumor Irradiation. Photo: A Zschau, GSI Helmholtzzentrum für Schwerionenforschung](/fileadmin/_processed_/c/6/csm_3_GSI_Therapie_Donut_5080d10bfb.jpg)
![Cell research in the laboratory of biophysics department. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/4/2/csm_GSI_FAIR_Biophysik_1_9e73b03ffc.jpg)
![Cell research in the laboratory of biophysics department. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/d/d/csm_GSI_FAIR_Biophysik_2_b12f693165.jpg)
6. FAIR
6.1 FAIR construction site
Follow this link to find the latest photos and videos of the FAIR construction site, e.g. the latest drone video, schowing the construction activities: Photos and videos FAIR construction site.
6.2 SIS100 dipole magnets
The dipole magnets of the future FAIR ring accelerator SIS100 will deflect the particles. In total 110 of these superconducting magnets will be installed in the accelerator ring.
![SIS100 dipole magnet - view inside the magnet. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/0/csm_GSI_FAIR_SIS100-Magnet_3_b66ba67b59.jpg)
![SIS100 dipole magnet. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/d/3/csm_GSI_FAIR_SIS100-Magnet_1_e88641e67f.jpg)
![SIS100 dipole magnet. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/a/d/csm_GSI_FAIR_SIS100-Magnet_2_0f0b9b520e.jpg)
![SIS100 dipole magnet. Photo: Babcock Noell](/fileadmin/_processed_/8/8/csm_GSI_FAIR_SIS100Magnet_4_babffb337a.jpg)
6.3 Serial test facility
At the serial test facility all superconducting magnets of the future FAIR accelerator SIS100 will be tested prior to installation. With liquid helium they are cooled to minus 269°C. Subsequently, they are tested for their capability to provide high and rapidly changing magnetic fields.
![Serial test facility. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/c/f/csm_GSI_FAIR_Kryotestanlage_3_8d68d61a94.jpg)
![Serial test facility. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/9/c/csm_GSI_FAIR_Kryotestanlage_2_e5b7adfc31.jpg)
![Serial test facility. Photo: J. Hosan/GSI Helmholtzzentrum für Schwerionenforschung GmbH](/fileadmin/_processed_/2/b/csm_GSI_FAIR_Kryotestanlage_1_162e9054b8.jpg)
6.5 FAIR visualizations
![Visualization of future FAIR facility. Visualization of future FAIR facility.](/fileadmin/_processed_/3/4/csm_ion42_2022_Render-01_1091e0118a.jpg)
![Visualization of future FAIR facility. Visualization of future FAIR facility.](/fileadmin/_processed_/b/4/csm_ion42_2022_Render-02_570095a093.jpg)
![Visualization of future FAIR facility. Visualization of future FAIR facility.](/fileadmin/_processed_/5/3/csm_ion42_2022_Render-03_68edad95e2.jpg)
![Visualization of future FAIR facility. Visualization of future FAIR facility.](/fileadmin/_processed_/4/0/csm_ion42_2022_Render-04_2814dd3a20.jpg)
![Visualization of future FAIR facility. Visualization of future FAIR facility.](/fileadmin/_processed_/c/0/csm_ion42_2022_Render-05_aefe1c55bc.jpg)
![Visualization of future FAIR facility. Visualization of future FAIR facility.](/fileadmin/_processed_/d/f/csm_ion42_2022_Render-06_bc88fdf30d.jpg)
![SIS100 particle accelerator, Visualization](/fileadmin/_processed_/c/7/csm_SIS100_Visualization___GSI__FAIR__Zeitrausch_7fc9830fef.jpg)
![SIS100 particle accelerator, Visualization](/fileadmin/_processed_/9/0/csm_FAIR_SIS_100_01_Visualization___GSI__FAIR__Zeitrausch_9cd041bcdd.jpg)
![Super FRS, Visualization](/fileadmin/_processed_/7/2/csm_FAIR_Super_FRS_02_Visualization___GSI__FAIR__Zeitrausch_efe2a9c63f.jpg)
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Terms of Use
Image and film use policy: GSI Helmholtzzentrum für Schwerionenforschung GmbH owns the right of use for all images and films published on this website – if not stated otherwise. For non-commercial purposes and for personal information and educational purposes, GSI will grant a free, non-transferable right of use under the following conditions: The copyright holder and the author must be featured clearly readable as proprietor, as it is stated beneath the images and films. (Example: „Image: GSI Helmholtzzentrum für Schwerionenforschung GmbH, Name of photographer“.) The granted right of use does not cover any modification of the image or film.
The use for other than the above stated or commercial purposes is not permitted without prior consultation of GSI. In case you would like to use an image for commercial purposes (e. g. advertising), please contact the GSI public relations office (info(at)gsi.de). In this case we require a written statement about your intentions (via E-Mail) and additionally a draft of your voucher copy to be published. Only after this procedure GSI can decide whether to place the requested image or film at your disposal.
Footage: All films shown here can be requested at the GSI in the Department of Press and Public Relations (info(at)gsi.de).
YouTube: If you follow the link to YouTube, you are leaving the GSI website and go to an external website, whichs privacy policies may differ from that of the GSI website. GSI has no control of the content of the external side.
This image and film use policy is laid down in English and German. In case of aberration, the German version shall in all cases prevail.