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Low energy muon spin rotation and point contact tunneling on niobium thin films
The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch 1
• Sample preparation: G. Terenziani & S. Calatroni (CERN) • PCT: T. Proslier (ANL) & J. Zasadzinzki (Illinois Institute of
Technology, Chicago) • LEmuSR: A. Suter (PSI)
06/10/2014
Motivation
The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch 2
• Niobium on copper is the material of choice for many accelerator cavities
• Despite many advantages compared to bulk niobium the technology is limited by a stronger Q-slope. Origin and correlation to the surface properties is not yet understood
• Low energy muon spin rotation (LEmuSR) and point contact tunnelling (PCT) have been used for bulk niobium studies
• Our aim is to use these techniques on niobium on copper films in order to find out, whether these techniques can reveal differences compared to bulk niobium
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Content
The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch 3
• Point Contact Tunnelling (PCT) • Review of measurements on bulk niobium • Results on niobium films
• Low Energy Muon Spin Rotation (LEmuSR) • Review of measurements on bulk niobium • Results on niobium films
• Conclusions
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PCT on clean niobium
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E.L Wolf - Principles of Electron Tunneling Spectroscopy - Oxford Scholarship Online 2012
06/10/2014 The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch
PCT on bulk niobium - Low temperature baking effect
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unbaked
125°C baked (24h)
Observations: – Zero-bias conductance – Broadened DOS
The low temperature baking gives – Reduced zero bias conductance – Less broadened DOS
T. Proslier et al. – Tunneling study of cavity grade Nb: Possible magnetic scattering at the surface – APL 2008
06/10/2014 The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch
PCT on bulk niobium – High temperature baking effect
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Blue: 1000°C Baking Red: 1400°C Baking
P. Dhakal et al. - Effect of high temperature heat treatments on the quality factor of a large-grain superconducting radio-frequency niobium cavity – PRSTAB 2013
Higher baking temperature (better RF performance) shows: • less low energy gaps • smaller Γ values (sharper
distributions)
Few zero bias peaks Very few small gaps measured (<1 meV) Sharpest Distributions Very low Gamma/Delta values (< 10%) Homogeneous sample
PCT on niobium on copper (dcms)
Zero bias peaks -> mag impurities Small gaps measured (~1.3 meV) Distributions fairly sharp Good Gamma/Delta values (< 10%) Homogeneous sample
PCT on niobium on copper (HIPIMS)
Zero Bias Peaks
For RF measurements see Giovanni’s talk
No Zero bias peaks Small gaps measured (<1.3 meV) Widest Distributions High Gamma/Delta values Inhomogeneous sample
PCT on niobium on copper (strongly oxidized dcms) For RF measurements see T. Junginger, PhD thesis University of Heidelberg (2012)
Point Contact Tunnelling – Conclusion
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• Investigated by PCT Nb on Cu samples can look as good as the best performing bulk niobium samples
• HIPIMS sample showed zero bias peaks -> Magn. Impurities? • A sample with a huge residual resistance showed small gaps, a
wide distribution and high Gamma/Delta values but no zero bias peaks
• There is a correlation to the low field residual resistance but the stronger Q-slope of the Nb on Cu technology cannot be explained by the DC properties measured with PCT
RF≠DC 06/10/2014 The sixth international workshop on thin films and new ideas for RF superconductivity
Tobias.Junginger@cern.ch
LEmuSR on bulk niobium
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A. Romanenko et al. - Strong Meissner screening change in superconducting radio frequency cavities due to mild baking – APL 2014
Local (London) Non-local (Pippard)
• Non exponential penetration • Taking non-locality into account exponential fit possible • Cold region of 120°C baked sample shows a strong change in Meissner screening with depth
LEmuSR on niobium on copper
06/10/2014 The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch 12
λ=38.8 nm
λ=21.5 nm
λ=26.4 nm
• Penetration depth almost twice as deep in dcms compared to HIPIMS
• Local London theory applicable to Nb films
• No change in Meissner screening with depth
LEmuSR on niobium on copper
• Zero field spectra of HIPIMS sample shows clear signs of magnetization at the surface and at 105 nm depth
• For dcMS sample weaker signs are found at the surface and no signs at 105 nm depth
• Further experiments are necessary to rule out trapped flux and muon diffusion
Conclusions
The sixth international workshop on thin films and new ideas for RF superconductivity Tobias.Junginger@cern.ch 14
• With PCT we find zero bias peaks and muSR gives direct evidence of magnetization of the HIPIMS sample (Magn. Impurities?)
• No change in Meissner screening with depth • Higher RRR does not necessarily result in a
less pronounced Q-slope (see also talks of Sarah and Giovanni)
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Backup Slides
06/10/2014
The sixth international workshop on thin films and new ideas for RF
superconductivity Tobias.Junginger@cern.ch
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Muon-spin rotation (μSR) technique
Sµ(0)
Bμ = (2π/γμ) νμ
Depth dependent µSR measurements
λ
B(z)
z
Bext
0
superconductor
B(z) = Bext exp(−z /λ)
Jackson et al., Phys. Rev. Lett. 84, 4958 (2000)
More precise: use known implantation profile
Jackson et al., Phys. Rev. Lett. 84, 4958 (2000)
Standard DCMS Temp dependence
HIPIMS 86 Hz Statistic
Zero bias peaks -> mag impurities Small gaps measured (<1.3 meV) Broadest Distributions Large Gamma/Delta values (> 10%) Inhomogeneous sample
HIPIMS 86 Hz Temp dependence
HIE e9 Statistic
Few Zero bias peaks – Small gaps measured (<1.3 meV),
broad distribution Distributions fairly sharp in gamma Good Gamma/Delta values (< 10%)
with few “hot spots”.
HIE e9 Temp dependence
HIE i9 Statistic
Small gaps measured (<1 meV), broad distribution
Distributions fairly sharp in gamma Good Gamma/Delta values (< 10%)
with few “hot spots”.
HIE i9 Temp dependence
06/10/2014
The sixth international workshop on thin films and new ideas for RF
superconductivity Tobias.Junginger@cern.ch
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06/10/2014
The sixth international workshop on thin films and new ideas for RF
superconductivity Tobias.Junginger@cern.ch
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M.2.7
M.2.3
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Tested Substrate Surface Treatment
Coating RBCS [nΩ]
Rres [nΩ]
RRR Δ/kB [K]
Remarks
4/12 M1.1 SUBU HIPIMS 140 A
400 (530)
310 3.7 17.8 Peel off already at this test?
9/12 M2.1 SUBU dcms 515 (6861)
3640 (1) - Peel off at iris
12/12 H8.6 EP in 1999 SUBU
dcms 526 91 - - Peel off on cut-off tube
02/13 H8.7 EP in 1999 SUBU
dcms 491 131 - - Millimetre sized defects observed
05/13 H8.8 EP in 1999 SUBU
HIPIMS 200 A
520 15 (8) - Slow cool down
07/13 M.1.2 SUBU HIPIMS 140 A
? 13000 - - Peel off
08/13 M2.2 SUBU HIPIMS 200 A
313 (4171)
55 (15.7) -
11/13 M2.3 EP+SUBU HIPIMS 200A
352 (4691)
4.4 13.1 18.0 EP; Field emission
12/13 M2.4 EP+SUBU HIPIMS 240 A
378 (5031)
13.3 22.1 18.0 Q-switch/Field emission
03/14 M.1.3 EP+SUBU HIPIMS 55 A
376 53 - - Q-switch/Field emission/Strong Q-slope
04/14 M.2.5 EP+SUBU HIPIMS 240 A
413 123 - - Residual resistance increased by processing
[1] Quadratically scaled to 1.5 GHz for comparison [2] Values in parenthesis have only been obtained from frequency shift