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Q-drop:

The International Workshop on Thin films and new ideas for pushing the limits of RF Superconductivity. Q-drop:. The Gap Dependence on Magnetic field. Enzo Palmieri. ISTITUTO NAZIONALE DI FISICA NUCLEARE Laboratori Nazionali di Legnaro &

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Q-drop:

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  1. The International Workshop on Thin films and new ideas for pushing the limits of RF Superconductivity Q-drop: The Gap Dependence on Magnetic field Enzo Palmieri ISTITUTO NAZIONALE DI FISICA NUCLEARE Laboratori Nazionali di Legnaro & Padua University, Science Faculty, Material Science Dept Work supported by the European Community Research Infrastructure Activity under the FP6 “Structuring the European Research Area” programme (CARE, contract number RII3 CT-2003- 506395)

  2. 11 10 0 Q 10 10 2 K 1,8 K 1,6 K 9 10 0 10 20 30 40 E [MV/m] acc Low field Q-Slope Medium field Q-Slope High field Q-drop Best 9-cell cavity result (after electro-polishing) (Courtesy D. Proch)

  3. 11 10 0 Q 10 10 2 K 1,8 K 1,6 K 9 10 0 10 20 30 40 E [MV/m] acc Low field Q-Slope

  4. Courtesy C. Benvenuti et al Nb/Cu sputtered cavity at CERN Sincefirst cavities were baked in the cryostat at ~150°C for ~48 hours the low field Q-slope was also reported for bulk Nb cavities

  5. Cavity spun at LNL and treated/measured at KEK

  6. Courtesy G. Ciovati

  7. (Courtesy G. Bisoffi)

  8. Presented at the 9-th RF Superconductivity Workshop, Santa Fè, NM, 1999 Renzo Parodi - RF SUPERCONDUCTIVITY AT INFN_GENOA Typical plot of Qo vs Eacc for cavities treated by Dry Oxidation of the surface after a medium temperature annealing

  9. Vacuum SC 2 SC 1 l1 Hz a l2 Let us suppose that: on bulk niobium (SC 2 ) we put an overlayer of a different superconductor (SC 1) a is the tickness of the SC 1 l1 is the penetration depth of the SC 1 l2 is the penetration depth of the SC 2

  10. x metal H z E Vacuum y THE ELECTROMAGNETIC RESPONSE OF A METAL For a semi-infinite conductor that fills the +x half-space and has a plane surface at x = 0 H(x) = H(0) e (ikx-wt) the Surface Impedance is defined as:

  11. Vacuum SC 2 SC 1 l1 Hz a l2 Two Superconductors: SC 2 + SC 1

  12. Vacuum SC 2 SC 1 l1 l2 Hz a

  13. Vacuum SC 2 SC 1 l1 Q2 l2 DQ Hz a Q1 l1/a For a “2 Superconductor system”

  14. 11 10 0 Q 10 10 2 K 1,8 K 1,6 K 9 10 0 10 20 30 40 E [MV/m] acc Medium field Q-Slope

  15. Q2 Hz a Q1 l1/a Vacuum SC 2 SC 1 l1 l2 An hypotesis: Gap and Penetration depth depends on magnetic field

  16. Q2 Q2 Hz a Q1 Q1 l1/a l1/a Vacuum SC 2 SC 1 l1 l2

  17. Q2e-k2b = + Q2 Why Q increases with field? The more l1 increases vs field Q1 The more SC2 ( low losses) is involved b

  18. = + The ticker is SC 1, the smoother is the Q-rise a/l0 Q2 O 0.1 1 10 Q1 b b

  19. D = D0 - pfvs I.I. Kulik, V. Palmieri, "THEORY OF DEGRADATION AND NON LINEAR EFFECTS IN Nb-COATED SUPERCONDUCTING CAVITIES", Proceedings of the Eight Workshop on RF Supercoductivity, Abano, Italy, October 1997, V. Palmieri, A. Lombardi eds. Special Issue of Particle Accelerators, Vol. 60,(1998)p.257-264 ? The Ginzburg-Landau result D= D0 (1 – H2/HC2) does not apply!!!

  20. D= D0 (1 – H2/HC2) This formula has done a lot of damage to our community for the understanding of the Q-Slope R.H. White and M. Tinkham, Magnetic-Field Dependence of Microwave Absorbtion and Energy gap in Superconducting Films, Phys Rev, vol 136, 1A, (1964), p. A203 “…..The qualitative features of D/D0 dependenceslike (1 – h2) and (1-h2)1/2 arevery different from those of the experimental absorption curves reported here …. due to the disagreement between these results and previous theory and experiment, it must be concluded that the above procedure for determining an effective energy gap parameter as a function of H is too naive.” Y. Nambu, S.F. Tuan, Phys, Rev. Lett. 11, 119 (1963); Phys.Rev.133, A1, (1964) “…Electrons moving parallel to the surface play a special role: since the magnetic filed will confine such an electron and the one with which it is paired to opposite surfaces of the film, they contribute little to the superconductivity pairing energy…”

  21. This relation goes back to first principles D = D0 - pfvs It means to take into account the supercurrent! If for Superconducting Magnets the fundamental and indipendent parameters are 3: TC, HC and JC, ….. why for Superconducting cavities, JC disappeared? Is 40 MV/m (1600 G) a field not strong enough?

  22. REVIEWS OF MODERN PHYSICS VOLUME 34, NUMBER 4 OCTOBER 1962 Critical Fields and Currents in Superconductors* JOHN BARDEEN UNIVERSITY OF ILLINOIS, Urbana, Illinois … II.THERMODYNAMIC RELATIONS To discuss the thermodynamics of a superconductor in a magnetic field or with current flow, it is most convenient to take the external field H and the superfluid velocity vs as independent variables. …… The displacement of the pairs causes an increase in free energy of the system which may be expressed simply in terms of Js…… APPENDIX B. DIRECT CALCULATION OF CHANGE OF GAP WITH CURRENT ... In the low temperature limit, there are no excitations formed and thus no change in D until the velocity vs reaches the value for which it is favorable to form pairs of excitations, corresponding to transfer of an electron from one side of the Fermi sea to the other.This criterion is (depairing condition) or

  23. l

  24. l The parasitic term PfVs is neglectable at high value of the pure bulk Nb case l l It becomes important at low - thin film case - contaminated surface after low temp baking

  25. Is a key parameter; low values give: - high Q - higher slope Courtesy C. Benvenuti et al l For film coated cavities there is no hope to get rid of the slope, unless RRR is increased, but in this case Q values will be lower than the actual

  26. 0 Q High field Q-drop 11 10 10 10 2 K 1,8 K 1,6 K 9 10 0 10 20 30 40 E [MV/m] acc

  27. D ns Js Vm Vs Vs Vs In local electrodynamics of superconductivity, j = j1+j2 Where J1 is the Meissner current At small supercurrent but at larger Vs, GL theory foresees a deparing effect by the current Over Vmthe superconducting state become unstable

  28. Conclusions: • Low field - The hypotesis of an overlayer explains the Q rise • Medium field – The gap decrease linearly vs field • D = D0 – pf vs l l This effect is neglectable for high but is felt when is reduced Film coated cavities: no hope to get rid of the slope, unless RRR is increased, but in this case Q values will be lower than the actual • High field – The gap closes at VC, but js start decreasing at Vm< Vc. Between Vm and VC, there is instability

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