Status of the PANDA Cluster-Jet Target Quarter 1/2018

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Presentation transcript:

Status of the PANDA Cluster-Jet Target Quarter 1/2018 The Cluster-Jet Target Gas System and Beam Line Adjustments Status of the PANDA Cluster-Jet Target Quarter 1/2018 PANDA Collaboration Meeting 2018/1 GSI Darmstadt, Germany Benjamin Hetz WWU Münster Institut für Kernphysik WWU Münster Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2017/3

Long Term Stability of the PANDA Cluster-Jet Target State of the PANDA Cluster-Jet Target Quarter 1/2018 Long Term Stability of the PANDA Cluster-Jet Target Stable cluster-jet beam: Using “designated” PANDA nozzle candidate Replaced broken H2 purification and gas system Solved exceptional nozzle clogging problems Thickness 𝜌 𝐴 = 1.4 ×10 15 atoms/ cm 2 @ PANDA IP (optimization ongoing) Setup in next to PANDA geometry and hardware configuration Camera X Camera Z Jet Beam Direction Skimmer Skimmer Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

Cluster-Jet Beam Monitor Systems State of the PANDA Cluster-Jet Target Quarter 1/2018 Cluster-Jet Beam Monitor Systems Both system yield information about: Jet beam thickness Jet beam width/form Jet beam stability Jet beam position in beamline Needed for optimization of Target thickness Target alignment Accelerator beam line/interaction point vacuum Absolute thickness monitor system (AMS) Absolute thickness information Destructive system (using moving rod through jet beam) Optical monitor system (OMS) Relative thickness information Non-destructive system (using scattered light) Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

Refined Absolute Thickness Monitor Systems (AMS) State of the PANDA Cluster-Jet Target Quarter 1/2018 Refined Absolute Thickness Monitor Systems (AMS) First AMS at scattering chamber for automatic beam measurements “Jet beam stability” Second simple, manual AMS Located at PANDA interaction distance 𝜌 𝐴 = 1.4 ×10 15 atoms/ cm 2 “Thickness/vacuum optimization” Third possible, manual AMS in preparation by our mechanical workshop Located at beam dump inlet “Perfect jet beam adjustment” Drawback: destructive monitor system rod position installed installed Automatic Absolute Thickness Monitor System in preperation Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

Refined Optical Monitor Systems (OMS) State of the PANDA Cluster-Jet Target Quarter 1/2018 Refined Optical Monitor Systems (OMS) Advantage: non-destructive System Matched optical, relative thickness to absolute thickness monitor systems proportional response OMS suited for target beam monitoring at PANDA without influence on jet beam/vacuum conditions Scaled Ratio of OMS/AMS Nozzle Pressure / bar Daniel Klostermann, Bachelor Thesis y axes 4 -4 Jet Beam Direction -4 -2 2 4 z axes False colour Image of TVC, beam diameter approx. 2.4 mm Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

Mie Scattering (S. Grieser) State of the PANDA Cluster-Jet Target Quarter 1/2018 Mie Scattering (S. Grieser) New Setup Cluster size/mass measurements in the regime of PANDA target operation conditions New setup : 0° between rotation plane and glass fibre (prior 7°) Spatial filter in front of glass fibre Auxiliary construction to find out the centre First measurements with cluster-jet beam in preparation Planned for spring 2018 Old Setup Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

New Nozzle Production Process (S. Grieser) State of the PANDA Cluster-Jet Target Quarter 1/2018 New Nozzle Production Process (S. Grieser) Galvanic deposition combined with laser production techniques Minimal narrowest inner nozzle diameter Reached: 12 µm inner diameter 𝜌 𝐴 ≈ 10 1𝟒 atoms/ cm 2 @ PANDA IP distance New Nozzles in preparation: Highest interest in the production of (10 – 30) µm inner diameter nozzles with thicknesses in the order of 10 1𝟓 atoms/ cm 2 Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

Studies on Vacuum Conditions State of the PANDA Cluster-Jet Target Quarter 1/2018 Studies on Vacuum Conditions Measurements of flow rates into each chamber Installation of slit collimator Additional orifices installed/under investigation Minimization of beam dump back flow rates Determination of cluster-jet beam contribution Work in progress Special slit collimator used at the PANDA target source (size 800 mm x 210 mm used) Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1

PANDA Cluster-Jet Target at COSY State of the PANDA Cluster-Jet Target Quarter 1/2018 PANDA Cluster-Jet Target at COSY Approved beam time at the COSY accelerator in Jülich August 2018 Installation during maintenance phase june 2018 Direct PANDA related target – ion beam interaction studies Vacuum conditions in presence of an ion beam Target influence on quality and lifetime of accelerator beam Investigation on cooling systems behaviour 2 MeV electron cooler stochastic cooling barrier bucket PANDA cluster-jet target placed at the COSY accelerator in Jülich (by Daniel Bonaventura) Benjamin Hetz – WWU Münster – PANDA Collaboration Meeting 2018/1