Our CF63 inline Faraday cup is a passively cooled solution for real-time charged particle beam current measurement, handling beam power loads up to 3 W and operating down to ultra-high vacuum conditions.

Special features

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• Fixed inline installation
• CF63 base flange
• Exchangeable apertures with diameters ranging from 0.5 mm up to 5 mm
• Triaxial wiring and feedthrough for the Faraday cup detector for low noise measurement
• Passive cooling for power loads up to 3 W

Our CF63 Faraday features passive cooling for power loads up to 30 W. It is retractable and positionable via a motorized linear feedthrough with a 100 mm stroke, offering precise control and flexibility for your system.

Special features

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• Linear feedthrough
• CF63 base flange
• Aperture diameter of 20 mm
• Designed for beam scanning applications of ion beams
• Applicable for electron beam energy up to 8 MeV
• passive cooling for thermal power loads up to 30 W (0.1 W/cm²)
• Retractable/positionable via motorized linear feedthrough with 100 mm stroke

Our CF63 Faraday cup features water cooling for power loads up to 60 W and maintains a temperature below 60°C in extreme UHV environments. It offers retractable installation on a pneumatic linear feedthrough with a 100 mm retraction length.

Special features

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• Linear feedthrough
• CF63 base flange
• 25 mm aperture diameter
• Designed for electron beam energies up to 8 MeV
• Water cooling for thermal power loads up to 60 W

Our CF63 Faraday cup features water cooling for thermal power loads up to 200 W. It is retractable and positionable via a motorized linear feedthrough with a 250 mm stroke, offering precise control and flexibility for your system.

Special features

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• Linear feedthrough
• CF63 base flange
• Aperture diameter of 25 mm
• Designed for beam scanning applications of ion beams
• Applicable for electron beam energy up to 8 MeV
• Water cooling for thermal power loads up to 200 W (10 W/cm²)
• Retractable/positionable via motorized linear feedthrough with 250 mm stroke

The 4-Jaw slit system can be used for ion beam diagnostics for the purpose of collimating or blanking the charged particle beam. Each slit is mounted on a linear feedthrough in order to be individually moved into and out of the beam.

The low lower system is designed for collimating beams of charged particles with an energy of 3 MeV and a beam power up to 6 W beam power in broad pressure ranges, down to ultra-high vacuum conditions.

Special features

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• 4 mm thick slit aperture made of copper
• Each slit is mounted to a motorized linear feedthrough
  thus being individually adjustable
• Travel length 40mm in steps of 0.71 μm
• BNC feedthrough for charged particle current readout on
  the individual aperture
• Vacuum chamber with DN63 ISO-F beamline connection
  flanges

The 4-Jaw slit system can be used for ion beam diagnostics for the purpose of collimating or blanking the charged particle beam. Each slit is mounted on a linear feedthrough in order to be individually moved into and out of the beam.

The high power system is designed for collimating beams of charged particles with an energy of 18 MeV and a beam power up to 270 W beam power in broad pressure ranges, down to ultra-high vacuum conditions.

Special features

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• Water cooled 6 mm thick slit aperture made of aluminum (3.0385. EN AW-1098)
• Each slit is mounted to a motorized linear feedthrough
  thus being individually adjustable
• Travel length 30 mm in steps of 1 μm
• Overlap of opposite apertures in insert position
• BNC feedthrough for charged particle current readout on
  the individual aperture
• Vacuum chamber with DN160 ISO-K beamline connection flanges

Centrally mounted on a CF100 flange, our neutral particle filter removes neutral particles from a particle beam. It operates by using electric fields to deflect charged particles along a bent beamline path while guiding neutral particles into a beam dump.

Special features

Sample design

• Aluminum chamber with ConFlat (CF) flange adapter
• DN100 CF beamline interface flanges
• DN100 CF and 2x DN40 CF accessory flanges (e.g., vacuum pump, viewport, vacuum gauge, beam dump, or Faraday cup installation)
• 2 pairs of vertical deflection plates
• Superimposing lens system for refocusing purposes

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The CF63 flange Wien filter separates charged particle beams by velocity using orthogonally superimposed magnetic and electric fields.

Special features

Sample design

• Suitable design for operation with singly charged low-energy ions (e.g., H₃O+, Ag+, K+, Cl–)
• 5 mm diameter entry and exit apertures
• Beam-stressed parts (e.g., electrodes, collimator, apertures) made of sputter-resistant materials
• Electrodes, magnetic yoke, and magnetic flux optimized to fit customer needs regarding beam energy and beam diameter
• SHV 10 kV electrical feedthrough on a single DN40 CF flange

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The CF63 flange Wien filter separates charged particle beams by velocity using orthogonally superimposed magnetic and electric fields.

Special features

Sample design

• Suitable design for operation with singly charged low-energy ions (e.g., H₃O+, Ag+, K+, Cl–)
• 4 mm diameter entry and exit apertures
• Beam-stressed parts (e.g., electrodes, collimator, apertures) made of sputter-resistant materials
• Electrodes, magnetic yoke, and magnetic flux optimized to fit customer needs regarding beam energy and beam diameter
• SHV 5 kV electrical feedthrough on a single DN40 CF flange

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The CF63 flange Wien filter separates charged particle beams by velocity using orthogonally superimposed magnetic and electric fields.

Special features

Sample design

• Suitable design for operation with singly charged low-energy ions (e.g., H₃O+, Ag+, K+, Cl–)
• 5 mm diameter entry and exit apertures
• Beam-stressed parts (e.g., electrodes, collimator, apertures) made of sputter-resistant materials
• Electrodes, magnetic yoke, and magnetic flux optimized to fit customer needs regarding beam energy and beam diameter
• SHV 10 kV electrical feedthrough on a single DN40 CF flange

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