Atomic-scale characterization of Nb for SRF cavities using UV

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Presentation transcript:

Atomic-scale characterization of Nb for SRF cavities using UV laser-assisted LEAP tomography and Cs-corrected TEM YoonJun Kim1, David Seidman1, Runzhe Tao2, Robert Klie2 1. Department of Materials Science and Engineering Northwestern University, Evanston, IL 2. Department of Physics, University of Illinois, Chicago, IL 7th SRF Materials Workshop, JLAB Newport News, VA July 16-17, 2012

 LEAP Tomography - Pure Nb coupon A pure Nb coupon had been analyzed using LEAP. - Sample ID: R06_17114.RHIT Sample preparation: (1) (at FNAL) Pure Nb coupons supplied by Alex Romanenko - A buffered chemical polished single-grain Nb sheet. - Test coupons were cut using electrical discharge machining (EDM). Approximate dimensions of 10 x 10 x 2 mm3 (2) (at NU) Tip preparations - Baked at 800 oC for 4 hours in UHV furnace - Pt deposition using South Bay Technology - Ion beam sputtering (≈150nm) - Lift-out method using a dual-beam FIB LEAP tomography conditions (1) Pulse rate: 250 kHz (2) Pulse energy: 50 pJ (necessary for oxide analysis) (3) Temp.: 30 K (4) Evaporation rate: 0.50%

 LEAP Tomography – Results (3-D reconstruction) Detector Histogram Tip Profiling 3-D Reconstruction H O Nb Ga NbH NbO NbO2 Nb2O5 Pt 300 nm

 LEAP Tomography – Results (3-D reconstruction) Results: 3D-reconstruction (Front view) Sequence (Top down) : Pt (not displayed)  Oxides (~5 nm, NbO2NbONb2O5)Pure Nb (~5 nm)  Nb, H, NbH mixture (~40 nm)  Bulk Nb Nb H NbH NbO NbO2 Nb2O5

 LEAP Tomography – 3-D reconstruction- top views All (0-10 nm) All Nb NbO NbO2 Nb2O5

 LEAP Tomography – 3-D reconstruction- top views All (10-20nm) All Nb NbO NbO2 Nb2O5

 LEAP Tomography – 3-D reconstruction- top views All (20-35 nm) All Nb NbO H NbH

 Overall O/Nb and H/Nb Ratios along Z-axis Oxide Pure Nb Bulk Nb Hydride layer 1.5 1.0 0.7 O/Nb ratio is highest value of 1.5 at the top surface as deep as 2 nm, then decreases and is 1.0 at 4 nm depth. H/Nb fluctuates inside of oxide layer and stabilizes at ~0.7 below a depth of 10 nm (possibly b or z phases). Further phase identification has been performed using TEM/EELS in collaboration with Prof. R. Klie and R. Tao at University of Illinois at Chicago.

 TEM/STEM Analysis – 1. Hydride Selected Area Diffraction Patterns at R.T. (300K) 110 zone BCC + superlattice reflections 110 zone of BCC

 TEM/STEM Analysis – 1. Hydride T. Schober et al., Topics in Applied Physics, 29, 11-71, 1978 Selected Area Diffraction Patterns at 94 K z H/Nb≈0.70 e b H/Nb≈1 H/Nb≈0.75

 EELS – Plasmon peaks analyses at 94K Bach et al., Microc. Microanal. 15, 505-523, 2009 Nb2O5 NbO2 NbO Nb Pt Layer Oxide Bulk Nb 1 2 3 4 5 6 7 8 9 10 1 2 3 4 5 Nb2O5 NbO2 NbO2 NbO2 6 7 8 9 10 NbO2 NbO NbO NbO NbO Nb Nb

Oxide type identification using Plasmon peak  TEM/EELS vs. LEAP Tomography Oxide type identification using Plasmon peak Pt Layer Oxide layer NbO2 Nb2O5 NbO Nb Nb2O5 NbO2 NbO Nb NbH H <Core-loss peak of Nb M and O K-edges> Three different oxides (NbO2, NbO, and Nb2O5) are coexist with 4-5 nm in thickness. NbO2 is observed to be a predominant oxide type quantitatively Sequence of oxides is not perfectly identical between EELS (NbO2 Nb2O5NbO) and LEAP tomography (NbO2NbO Nb2O5).

 Summary 3-D LEAP tomographic reconstructions show oxides, hydride, and bulk Nb layers. Oxide layers consist of NbO, NbO2, and Nb2O5, 5 nm in thickness, followed by a pure Nb layer about 5nm in thickness. All types of oxides are found around 110 type pole regions of Nb, but NbO is also rich in 100 type pole regions. NbH layer forms at 40 nm between pure Nb layers and is found mostly around 110 type pole regions of Nb. O/Nb ratio within oxide layer decreases from 1.5 to 1.0 and H/Nb ratio within hydride layer is 0.70. There are bumps of H/Nb ratio (rich in H ) at the interfaces between layers. Oxide analyses compared to EELS analyses : From line scans of the surface region based on the low-loss EELS spectrum at 94 K, oxide layer consists mostly of NbO and NbO2. This agrees with LEAP tomographic analyses.

 Acknowledgements This study is funded by USDOE through Fermi National Accelerator Laboratory (FNAL). We are grateful to Drs. Lance Cooley and Alex Romanenko in FNAL for supplying samples and valuable discussions. The LEAP tomographic measurements were performed at the Northwestern University Center for Atom-Probe Tomography (NUCAPT). The LEAP tomograph was purchased and upgraded with funding from NSF-MRI (DMR-0420532) and ONR-DURIP (N00014-0400798, N00014-0610539, N00014-0910781) grants.