JLab infusion and LG flux expulsion update

Slides:



Advertisements
Similar presentations
Superconducting Materials R&D: RRCAT-JLAB Collaboration S B Roy Materials & Advanced Accelerator Science Division RRCAT, Indore Collaborators: M. K. Chattopadhyay,
Advertisements

Introduction to Ingot Niobium Andrew Hutton SSTIN10 Symposium Jefferson Lab Sept 22-24, 2010.
Thin Films for Superconducting Cavities HZB. Outline Introduction to Superconducting Cavities The Quadrupole Resonator Commissioning Outlook 2.
ILC PM Meeting S0 Webex Global Design Effort 1 S0/S1 Next Steps Lutz Lilje GDE.
Rong-Li Geng Jefferson Lab High Efficiency High Gradient Cavities - Toward Cutting Down ILC Dynamic Heat Load by Factor of Four R.L. Geng, ALCW2015,
Study of MgB 2 Thin Films on Nb by Pulse Laser Deposition S.Mitsunobu, S.Inagaki, H.Nakanishi, M.Wake and M.Fukutomi* KEK,NIMR*
Summary SRF project at Argonne National Laboratory (started 11/09) Investigators: Th. Proslier, J. Klug, N. Becker, M. Kharitonov, H. Claus, J.Norem, M.
Cornell SRF New Materials Program Nb 3 Sn Development Sam Posen and Matthias Liepe Cornell University TTC Meeting 6 December 2011 Beijing, China.
Structure of the task 12.2 Claire Antoine Eucard2 WP12 DESY
High Q R&D at JLab G. Ciovati, P. Dhakal, R. Geng, P. Kneisel, G. Myneni TTC Topical Meeting on CW SRF Cornell Univ., June 12 th -14 th, 2013.
R.L. Geng, 5/27-31,2013 ECFA LC2013, DESY 1 Update on Raising Q0 at Ultra-High Gradient via Large-Grain Niobium Material Rongli Geng Jefferson Lab ECFA.
Rongli Geng March 4, th LCC ILC Cavity Group Meeting
Q-Slope at High Gradients ( Niobium Cavities ) Review about Experiments and Explanations Bernard VISENTIN CEA - Saclay.
Sindhunil Barman Roy1 and Ganapati Myneni2
Advances in Development of Diffused Nb3Sn Cavities at Cornell
ALCPG2011, 3/19- 23, SRF Group Institute of Heavy Ion Physics, Peking University ALCPG /3/19-23, Eugene, Oregon, USA RF superconducting Cavity.
JLab Update Rongli Geng April 30, th LCC ILC Cavity Group Meeting.
High Temperature Heat Treatment to Raise the Quality Factor of Large Grain Niobium Cavities Pashupati Dhakal Gianluigi Ciovati Ganapati Rao Myneni July.
Centrifugal Barrel Polishing at Fermilab (Tuesday, December 6th at 10:20) Tesla Technology Collaboration IHEP, Beijing December 5 th -8 th, 2011.
Annual Meeting CERN - November 2005 Bernard V ISENTIN.
The Applied Superconductivity Center The National High Magnetic Field Laboratory Florida State University 7 th SRF MW Investigation: Variation of Surface.
Niobium RRR and Ta specifications for SRF cavities: a critical review G. Ciovati, P. Kneisel and G. Myneni 7 th SRF Materials Workshop, July 16 th 2012.
1 SIMS Characterization of Impurity Elements in Nb: The Effect of Heat Treatments ncsu.edu/aif jlab.org 1 P. Maheshwari, F. Stevie, D. Griffis, M. Rigsbee.
RF Superconducting Materials Workshop at Fermilab, May 23 & 24, 2007 Advanced Nb oxide surface modification by cluster ion beams Zeke Insepov, Jim Norem.
High-Q, High Gradient Niobium-Coated Cavities at CERN
Surface Resistance of a bulk-like Nb Film Sarah Aull, Anne-Marie Valente-Feliciano, Tobias Junginger and Jens Knobloch.
Rongli Geng ILC Cavity Group Meeting October 25, 2011
Pulsed Energetic Condensation of Nb Thin Film Cavities at JLab
Juliette Plouin, Enrico Cenni, Olivier Napoly (CEA)
Update on the US decadal roadmap on SRF technology for HEP accelerators Sergey Belomestnykh FCC Week 2017 in Berlin 30 May 2017.
Research Theme 2: Beam Acceleration (Superconducting RF Cavities)
New Cavity Techniques and Future Prospects
CERN Studies on Niobium-Coated 1.5 GHz Copper Cavities
Superconducting RF Materials for Accelerators
Peng Sha Institute of High Energy Physics, CAS
Surface Analysis of the Quench Area Sample of Cavity Z111
High Q via N infusion R&D at Jefferson Lab
SUPERCONDUCTING THIN FILMS FOR SRF CAVITIES
Effort Torwards Improving Large Scale Production for SC Cavities
A COMMON R&D ON THE HIGH GRADIENT Nb CAVITIES
N infusion study at DESY
9-cell Vender Qualification test for LCLS-II
Recent SCRF Activities in IHEP
Materials, Advanced Accelerator Science & Cryogenics Division
TTC High Q0 Working Group Summary of developments since last TTC meeting C. Reece.
Effect of Surface Treatments on the Superconducting Properties of Niobium Presented by A.S.Dhavale Sept. 23, 2010.
TTC WG-2 focusing on Nb Material - Properties and Specifications -
TTC topical-meeting on CW SRF 2013
Future Thin Film Deposition Efforts at FNAL
Update from single-cell low temperature doping runs at JLab
Nick Walker (DESY) EU GDE Meeting Oxford
N-infusion, Vertical-EP, and ILC cost reduction efforts at Cornell
LCLS-II High Q0 Cavities: Lessons Learned
Cavity Treatment for High Q0 in Realistic Magnetic Fields
ON THE HIGH GRADIENT Nb CAVITIES
Development of Large Grain Cavities at DESY
SRF Surface Studies and the High Field Q-slope Mystery
Recap RGA during 800°C bake showed high mass contributions (Hydrocarbons) Samples within a standard 800°C bake showed precipitates as well TTC High Q Meeting.
Vertical Test Results of 9-Cell Cavities for LCLS-II
Recent 160 C “N infusion” impurity doping results
Surface resistance studies as a function of the mean free path
LCLS-II HE R&D ongoing results
Peng SHA, On behalf of CEPC SRF group
Nb films Sergio Calatroni for the new CERN SRF & films team 5/21/2019
JLab Doping Protocol Exploration
Quench Studies in Single and Multicell N-Doped Cavities
FLUX TRAPPING STUDIES ON LOW BETA CAVITIES
SRF Science and Technology
JLab Work on Low Temperature Near-Surface Diffusion aka “Infusion”
The LCLS-II HE High Q0 and Gradient R&D Program
Presentation transcript:

JLab infusion and LG flux expulsion update Pashupati Dhakal 09/08/2017 Title Page

N-Infusion Update High purity fine grain Nb Cavity RDL-02: After the fabrication, the cavity was given standard ILC recipe of 150 mm EP, 800 C/2hrs furnace treatment, followed by 20 mm EP. Cavity was HPR before loading to the furnace and Nb caps were assembled in clean room. After each heat treatments (with caps), the baseline measurement was done to surface reset with 10 mm EP. Rs vs T data were taken from 4.3-1.5K at Bp~10mT in order to extract the material parameters. No post chemistry after the furnace treatment. Interior Page Design 1 Correction to earlier report: N2 gas was injected into the furnace ~280-290 C (unintentional)

RECENT WORK AT JLAB Interior Page Design 1 Standard ILC EP recipe

RECENT WORK AT JLAB Standard ILC EP recipe with Bake Interior Page Design 1 Standard ILC EP recipe with Bake

RECENT WORK AT JLAB Interior Page Design 1

RECENT WORK AT JLAB Interior Page Design 1

RECENT WORK AT JLAB Interior Page Design 1

RECENT WORK AT JLAB Interior Page Design 1 Work in Large grain cavities as well as process control are in progress.

Sample Coupons Study 800°C 800°C+ N2@120°C 800°C+ N2@140°C FSU/ASC Interior Page Design 1 The material looks non-uniform. Grain sizes vary between 10-70µm

Sample Coupons Study FSU/ASC 800°C 800°C+ N2@120°C 800°C+ N2@160°C Interior Page Design 1 Granular surface morphology on low temperature N doped samples

Sample Coupons Study FSU/ASC Interior Page Design 1 Preliminary XPS Result: Presence of a NbNO peak in low temperature N doped sample

Sample Coupons Study FSU/ASC Nb2O5 Nb2O5 204.3 202.3 Nb2O5 Nb2O5 Bulk NbN(1-x)Ox 202.3 NbOx/Nb Interior Page Design 1 800°C /3h (F9) 800°C+N2@160°C (F12) Nb Nb2O5 Bulk NbOx Nb2O5 NbN(1-x)Ox Nb Bulk Nb2O5, and NbN(1-y)Oy exists within first 10nm in low temperature N infused sample

Magnetization/AC Sussceptility Surface effect with N-infusion

SIMS One sample shower higher C content, may have segregated C Oxygen profile consistence with earlier studies of LTB Higher N concentration for 140 and 160C/48hrs treatments.

Sample Coupons Study Q-slope High Eacc High Q WHY? High Rres The lower residual resistance can be achieved by reducing the thickness of normal layer thickness and also the normal-superconducting interface resistance. Kubo & Gurevich, SRF2017

Conclusions Nitrogen Infusion at low temperature works and can be ideal processing recipe to achieve high Q, high gradient cavities. Low temperature N-doping of Nb affects the surface properties significantly Increase in Hc3 value, an indication of reduced electron mean free path on surface. Different baking temperature in N2 atmosphere leads to different surface condition. Preliminary XPS on low temperature nitrogen infused sample shows a presence of NbN(1-y)Oy and a protective Nb2O5 within the first 10nm. The presence of other sub-oxides cannot be ruled out. XPS analysis is in progress. But the bulk properties remains unaffected Tc is unchanged Number of pinning sites (evident from magnetization loop) are almost same. The effect is different from high temperature N-doping. Sample study shows higher flux trapping efficiency, similar to conventional nitrogen doping. Interior Page Design 1

Flux Expulsion on LG cavities Where does the flux trap? Surface or bulk? RF only sees the surface flux trapping where as flux expulsion is bulk effect. We measure the flux expulsion and flux trapping studies on LG cavities with different impurities in order to see the correlation of purity (bulk RRR) and surface preparations (EP, LTB and N-doping)

Flux Expulsion on LG cavities

Flux Expulsion on LG cavities Surface (EP) RRR = 107 RRR = 60 RRR = 486 Cavity DT>4K(Bsc/Bn ~ 1.5) dRres/dBa nW/mG DT<0.1K(Bsc/Bn ~ 1) TC1N1 (RRR=60) 0.13 ±0.01 0.51 ±0.02 KEK-R5 (RRR=107) 0.10 ±0.02 0.28 ±0.04 G2 (RRR=486) 0.11 ±0.01 0.57 ±0.02

Cavity G2 (EP vs N-doped) DT>4K (Bsc/Bn ~ 1.5) dRres/dBa nW/mG DT<0.1K(Bsc/Bn ~ 1) dRress/dBa nW/mG G2 (EP) 0.11 ±0.01 0.57 ±0.02 G2 (EP+N2-7umEP) 0.13 ±0.01 1.06 ±0.03

KEK-R5 (EP vs LTB 120/24hrs) Increase due to LTB Cavity DT>4K (Bsc/Bn ~ 1.5) dRres/dBa nW/mG DT<0.1K(Bsc/Bn ~ 1) dRress/dBa nW/mG KEK-R5 (EP) 0.10 ±0.02 0.28 ±0.04 KEK-R5 (EP+LTB) 0.10 ±0.01 0.41 ±0.03

DT <0.1K DT >4 K

Eacc = 36 MV/m, Q0 = 2x1010

Summary Good flux expulsion (DT>4K) regardless of RRR dRres/dBa ~ 0.1-0.13 nW/mG, regardless of RRR and surface preparations as long as DT > 4K. The trapping sensitivity increase from 0.57 to 1.06 nW/mG (about a factor of 2) in N-doped cavity made from high purity LG niobium The trapping sensitivity increase from 0.28 to 0.41 nW/mG due to LTB in cavity made from medium purity Nb. May help to understand the bulk/surface pinning effect on Rres. More details analysis to follow…..