research for srf cavities
play

Research for SRF Cavities T. Tajima, G. Eremeev*, M. Hawley, R. - PowerPoint PPT Presentation

Update on MgB 2 Thin Film Research for SRF Cavities T. Tajima, G. Eremeev*, M. Hawley, R. Schulze, LANL J. Guo, S. Tantawi, V. Dolgashev, D. Martin, C. Yoneda, SLAC B. Moeckly, Superconductor Technologies, Inc. (STI) I. Campisi, ORNL TTC


  1. Update on MgB 2 Thin Film Research for SRF Cavities T. Tajima, G. Eremeev*, M. Hawley, R. Schulze, LANL J. Guo, S. Tantawi, V. Dolgashev, D. Martin, C. Yoneda, SLAC B. Moeckly, Superconductor Technologies, Inc. (STI) I. Campisi, ORNL TTC Meeting, FNAL, Batavia, IL, USA, 19-22 April 2010 LA-UR-10-02476 *Presently at JLab U N C L A S S I F I E D Slide 1 Operated by Los Alamos National Security, LLC for NNSA

  2. We are trying to demonstrate Gurevich’s multi-layer superconductor proposal Simple single layer example E acc ~ 100 MV/m Assumptions  H c1 (Nb) = 170 mT H 0 = 355mT λ L (MgB 2 ) = 140 nm H i = 170mT ξ (MgB 2 ) = 5 nm H c1 (MgB 2 ) = 355 mT  d = 105 nm  Nb The film thickness needs to be determined  MgB 2 so that the decayed field at the Nb surface is below the RF critical field of Nb (~200 mT). Dielectric d = 105 nm material U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  3. 2-inch disk experiments have been carried out at SLAC using a 11.4 GHz 50 MW Klystron to generate short pulses (≤ 2 µs) and a TE 013 -mode copper hemispheircal host cavity Currently: Pulse width 1.6 µs Rep rate  1 Hz 2 inches (~50 mm) U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  4. The RF breakdown (quench) normally starts on the ring at half radius where the surface magnetic field peaks Typical distribution of superconducting and normal- G: Geometrical factor conducting regions after quench  Sample Q G /R 0 sample surface Magnetic field profile H  The cavity Q starts to decrease when part of sample quenches  One can calculate approx. surface resistance from sample Q 0 U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  5. Sample setup detail and current MgB 2 coating method Reactive co-evaporation of MgB 2 at Sample setup at SLAC Superconductor Technologies, Inc. (STI), Santa Barbra, CA. Temperature sensor Cold head Sample: <1.5 mm thick Copper sample holder: 6.35 mm thick B.H. Moeckly and W.S. Ruby, Supercond. Sci. Technol. 19 (2006) L21 – L24 U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  6. So far, 4 types of coatings have been tried in addition to bare Nb reference samples MgB 2 (100 nm) #2 #1 1000 nm MgB 2 B (10 nm) Bulk Nb Bulk Nb #3 #4 200 nm MgB 2 MgB 2 300 nm B 200 nm ~450 µm Sapphire Bulk Nb C-plane U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  7. Coating #1 Note the increase of O and Mg Element depth profile Nb B Actual Planned Mg MgB 2 (100 nm) Mg O B (10 nm) Bulk Nb A number of cracks on MgB 2 were observed after tests. U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  8. Coating #2 Elements depth profile Nb Note the increase of O Actual B Planned 1000 nm Mg MgB 2 O Bulk Nb A number of cracks on MgB 2 were observed after tests. U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  9. Coating #3 Elements depth profile Note the increase of O and Mg! Nb B Actual Planned Mg 200 nm MgB 2 B 200 nm O Bulk Nb Mg U N C L A S S I F I E D Slide 9 Operated by Los Alamos National Security, LLC for NNSA

  10. Coating #4 Elements depth profile • The actual depth profile showed very small Planned amount of oxygen and very close to the planned coating. MgB 2 300 nm • This indicates that the increased amount of Sapphire ~450 µm oxygen shown in the C-plane previous MgB 2 /(B)/Nb systems was from bulk Nb U N C L A S S I F I E D Slide 10 Operated by Los Alamos National Security, LLC for NNSA

  11. Comparison of low-power Q 0 – T data: MgB 2 (300nm)/Sapphire showed significantly higher Q 0 MgB 2 (300nm)/Sapphire limited by the Q 0 of copper dome 400,000 #1: MgB2(100nm)/B(10nm)/Nb #2: MgB2(1000nm)/Nb 350,000 #3: MgB2(200nm)/B(200nm)/Nb 300,000 #4: MgB2(300nm)/Sapphire Nb (single crystal RRR~300) 250,000 Copper Q 0 200,000 150,000 100,000 50,000 0 0 20 40 60 80 100 120 Sample temperature (K) U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

  12. Coating #4, MgB 2 (300nm)/Sapphire: Q 0 vs. B peak at 3 K MgB 2 quenches at 25 mT (Only one sample has been tested so far.) 400,000 350,000 300,000 250,000 Q 0 200,000 150,000 100,000 50,000 0 0 5 10 15 20 25 30 B peak (mT) U N C L A S S I F I E D Slide 12 Operated by Los Alamos National Security, LLC for NNSA

  13. Coating #4, MgB 2 (300nm)/Sapphire: B C,RF vs. T 30 25 20 B C,RF (mT) 15 10 5 0 0 5 10 15 20 25 30 35 40 T (K) U N C L A S S I F I E D Slide 13 Operated by Los Alamos National Security, LLC for NNSA

  14. Measured quench fields at 3 K have been low. For #1- #3, thermal effect due to high surface resistance and effect of cracks are involved and confusing. Coating Series No. Planned coating Quench field (mT) #1 MgB 2 (100nm)/B(10nm)/Nb ~30 Actual T was #2 MgB 2 (1000nm)/Nb ~30 probably higher!  10 (~50 on Nb) #3 MgB 2 (200nm)/B(200nm)/Nb #4 MgB 2 (300nm)/Sapphire 25 Nb alone has shown a quench field of 60-70 mT and it is likely to be a thermal quench not magnetic, which is caused by high residual resistance. U N C L A S S I F I E D Slide 14 Operated by Los Alamos National Security, LLC for NNSA

  15. Issues and plans to address them Unexpectedly high residual resistance of Nb (~2 m Ω ) compared  to the expected BCS resistance of ~15 µ Ω at 11.4 GHz at 3 K • Measure the external magnetic field and try to shield it and see the effect The effect of reducing the film thickness has not been seen  • A series of MgB 2 /Al 2 O 3 /Nb is under test to reduce the reaction between MgB 2 and Nb • Try MgB 2 (<100nm)/Al 2 O 3 /MgB 2 (<100nm)/Al 2 O 3 /MgB 2 (<100nm)/Sapphire Non-uniform coating due to relatively rough surface (R a >10 nm)  • We started to use mechanical-chemical polishing by Cabot Microelectronics Polishing Company that produces R a <1 nm Cracks  • Changing substrate thickness from ~0.6 to ~1.2 mm has helped. U N C L A S S I F I E D Slide 15 Operated by Los Alamos National Security, LLC for NNSA

  16. Summary  We are trying to demonstrate the principle of multi- layer superconductor coating to increase the achievable magnetic field  We have not been successful yet, but there has been increased understanding on what is happening  Our goal in 2010 is to demonstrate the first milestone of >200 mT (0 K) or equivalent fields at respective temperatures with flat 2-inch diameter samples after addressing some issues that have emerged. U N C L A S S I F I E D Slide 16 Operated by Los Alamos National Security, LLC for NNSA

  17. Acknowledgements  Many thanks to: • Sponsor (DTRA) • P. Kneisel (JLab) • A. Canabal (U. Maine) • S. Lesiak (CMPC) • Other LANL workers: — R. Depaula, I. Apodaca (MPA-STC) — B. Day (MST-7) — R. Montoya (PF-FS) — J. Harrison, (AOT-MDE) U N C L A S S I F I E D Operated by Los Alamos National Security, LLC for NNSA

Recommend


More recommend