Update on SPS Wire Scanner Prototype Measurements A

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Update on SPS Wire Scanner Prototype Measurements A. Valimaa With support from F. Caspers,

Update on SPS Wire Scanner Prototype Measurements A. Valimaa With support from F. Caspers, E. Piselli, L. Timeo, C. Vollinger

SPS Wire Scanner Structure • The wire scanner has two flanges on the side

SPS Wire Scanner Structure • The wire scanner has two flanges on the side to connect it to the beam pipe. • Three other flanges are for vacuum pumping or other purposes (top, bottom, back). • Tank is the placeholder for the drum in which the scanning mechanism is build on. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

SPS Wire Scanner Structure • In the centre acts the scanner mechanism, the fork

SPS Wire Scanner Structure • In the centre acts the scanner mechanism, the fork 17/09/2020 Alpo Välimaa, BE-ABP-HSC

SPS Wire Scanner Structure • The scanner consists of a fork and a wire.

SPS Wire Scanner Structure • The scanner consists of a fork and a wire. • They couple to electromagnetic cavity resonances. • For the measurements, we used a copper wire instead of a carbon wire for mechanical reasons; It is less fragile. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

SPS Wire Scanner Structure • The drum is for dismounting the scanner system when

SPS Wire Scanner Structure • The drum is for dismounting the scanner system when the tank is placed in the beam pipe. W. Andreazzi 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Motivation • The carbon wire of the fork of SPS wire scanner burns out

Motivation • The carbon wire of the fork of SPS wire scanner burns out due to excessive power dissipation on it. • Structure possibly creates an impedance problem. • The structure of the wire scanner allows resonances that couple to the fork. This is to be prevented. • It is critical to find out which of the cavity resonances are harmful to the fork and find a solution to damp them. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Measurement Setup • Measure S-parameters from two probes set inside cavity along the beam

Measurement Setup • Measure S-parameters from two probes set inside cavity along the beam line. • Transmission tells us the cavity modes excited and seen by the beam. • Reflection tells us the amount of coupling between the cavity and the probe • Perturb the system as little as possible (small coupling). 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Measurement Setup • Rotate the fork to see which resonances couple with the fork

Measurement Setup • Rotate the fork to see which resonances couple with the fork and how much 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Fork Angle Dependency • Transmission measurement on plain structure in function of fork position

Fork Angle Dependency • Transmission measurement on plain structure in function of fork position • 1 st resonance unaffected by the fork position • The fork seems to strongly couple near 300 MHz and 500 MHz • At high frequencies the probes are too strongly coupled on resonances -> modify couplers 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Mode Damping – Top Flange • We insert an all mode coupler from the

Mode Damping – Top Flange • We insert an all mode coupler from the top flange in order to damp oscillations inside the cavity. • Coupling strength limited by the depth we can penetrate into the cavity not touching the wire. • Through delicate measurements we can conclude that the coupler is coupling to both electric and magnetic fields. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Mode Damping • Increasing the surface area of the coupler with a copper foil

Mode Damping • Increasing the surface area of the coupler with a copper foil had positive effects via increased capacitive coupling • Some modes still unaltered -> insufficient alone 17/09/2020 Alpo Välimaa, BE-ABP-HSC

What If… • … we took the big flange cover off and let the

What If… • … we took the big flange cover off and let the cavity radiate? • We should see how much it is possible to damp the fields if we were able to damp all the resonances at the flange plane 17/09/2020 Alpo Välimaa, BE-ABP-HSC

…But Nothing Changed! • Then we understood that there is a reentrant cavity structure

…But Nothing Changed! • Then we understood that there is a reentrant cavity structure - between the drum and the tank – that couples to the main cavity inside the drum. • Test: Insert lossy material near the small gap where the fields possibly are most concentrated -> it works! 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Lossy contact over the gap • Test of a possible solution by inserting a

Lossy contact over the gap • Test of a possible solution by inserting a number of resistors of 10, 50 and 100 Ohm over the gap between the drum and the tank • The results were promising independent of the resistance within 10 -100 Ohm. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Resistor Number Dependency • Good damping is achieved with already two resistors. • Three

Resistor Number Dependency • Good damping is achieved with already two resistors. • Three resistors really perform well up to 700 MHz 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Resistor Position Dependency • Resistor positioning has some visible effect. • Better damping is

Resistor Position Dependency • Resistor positioning has some visible effect. • Better damping is achieved with symmetric positioning. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Carbon-Like Wire • To mimic the electrical properties of carbon wire, we decided to

Carbon-Like Wire • To mimic the electrical properties of carbon wire, we decided to replace the copper wire with a series of resistors summing up to 4 k. Ohm • Picture: New wire during assembly. View from the top flange. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Fork Angle Dependency – Carbon-Like Wire • Note: Less fork position dependent behaviour (fork

Fork Angle Dependency – Carbon-Like Wire • Note: Less fork position dependent behaviour (fork coupling) at low frequencies than in the case of copper wire! • This is to be analysed more delicately. 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Fork Angle Dependency – Carbon-Like Wire and Lossy Contact • Modes up to 700

Fork Angle Dependency – Carbon-Like Wire and Lossy Contact • Modes up to 700 MHz are clearly damped independent of fork position • At 225° fork very close to the probe at port 1 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Proposed Solution • Add feedthroughs to have the desired resistance over the gap but

Proposed Solution • Add feedthroughs to have the desired resistance over the gap but to place the resistors outside vacuum • Place them with 120 degree symmetry – if mechanical restrictions allow – to avoid azimuthal modes of lowest order • Details are to be optimized in simulations 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Thank you! 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Thank you! 17/09/2020 Alpo Välimaa, BE-ABP-HSC

Following steps • Re-measure without the wire • Modify the probe to have good

Following steps • Re-measure without the wire • Modify the probe to have good data on high frequencies • Resonant matching technique with the modified all mode coupler to damp selected higher order modes 17/09/2020 Alpo Välimaa, BE-ABP-HSC