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Commissioning of a TE011 cavity for surface resistance measurement by calorimetric method G. Martinet , M. Fouaidy, N. Hammoudi, S. Blivet, M. Labaste ,[object Object],[object Object],[object Object],[object Object]
Motivations ,[object Object],[object Object],[object Object],[object Object],[object Object]
Principle of the method For radius  r>40mm  P STAT =P RF       T STAT =   T  RF  Determination  of  R S  coefficients   (a, b, c)  by least square method R=0 Rcav=55 Rseal=58 q HF Nb Cavity RF part LHe Thermometric  part q STAT Vacuum Heater
Advantages and limitations of calorimetric method ,[object Object],[object Object],[object Object],[object Object],T=1.7K T=4.2K Field Limitations     For Bs<5mT: thermal instabilities  due to switching from natural convection to nucleate boiling (Not hard limit!)    For Bs>15mT: power limitation  due to  dissipations  in the  cylindrical part  of the cavity (bulk  Nb)
Expected performances With a detectable heating of 0.1 mK, the expected sensitivity should correspond to the following tables ,[object Object],[object Object],[object Object],1 40 45 20 75 5 Sensitivity (n Ω ) @1.8K B s (mT) 5 15 10 10 45 5 Sensitivity (n Ω ) @4.2K B s (mT)
Cavity design TE012 TE011
Thermometric system ,[object Object],[object Object],[object Object],[object Object],[object Object]
Reception of mechanical parts Thermometric chamber and niobium cavity has been received (august 2009) Dedicated system developed for chemical treatment and HPR process Design of a new nozzle to prevent electrical discharge
Conditioning for RF test Discs support  for chemical treatment (“handmade” process) Cavity handling frame for chemical treatment and clean room assembly Preparation for HPR treatment of the sample and the cavity
RF results for the TE011 cavity Estimated Q0 value and dissipated power for theoretical R BCS  (Nb RRR300) :  @4.2K: 1.6 10 8  (1.1 10 8 ) and P cav =152W (62mT) @1.8K: 2.0 10 10  (1.4 10 10 ) and P cav =1.2W(62.mT) Huge residual resistance due to bad chemical treatment (80µm BCP, T ≈20°C)
Thermometric measurement Bpeak=52mT @ 4.2K reached! Good sensitivity (200mT/W for Nb@4.2K)
Schedule ,[object Object],[object Object],[object Object],[object Object]
 

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Martinet - Commissioning of a TE011 cavity for surface resistance measurement by calorimetric method

  • 1.
  • 2.
  • 3. Principle of the method For radius r>40mm P STAT =P RF   T STAT =  T RF  Determination of R S coefficients (a, b, c) by least square method R=0 Rcav=55 Rseal=58 q HF Nb Cavity RF part LHe Thermometric part q STAT Vacuum Heater
  • 4.
  • 5.
  • 7.
  • 8. Reception of mechanical parts Thermometric chamber and niobium cavity has been received (august 2009) Dedicated system developed for chemical treatment and HPR process Design of a new nozzle to prevent electrical discharge
  • 9. Conditioning for RF test Discs support for chemical treatment (“handmade” process) Cavity handling frame for chemical treatment and clean room assembly Preparation for HPR treatment of the sample and the cavity
  • 10. RF results for the TE011 cavity Estimated Q0 value and dissipated power for theoretical R BCS (Nb RRR300) : @4.2K: 1.6 10 8 (1.1 10 8 ) and P cav =152W (62mT) @1.8K: 2.0 10 10 (1.4 10 10 ) and P cav =1.2W(62.mT) Huge residual resistance due to bad chemical treatment (80µm BCP, T ≈20°C)
  • 11. Thermometric measurement Bpeak=52mT @ 4.2K reached! Good sensitivity (200mT/W for Nb@4.2K)
  • 12.
  • 13.