Prospect of High Gradient Cavity H. Hayano, 10222013 Tohoku Forum for Creativity 2013.

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Presentation transcript:

Prospect of High Gradient Cavity H. Hayano, Tohoku Forum for Creativity 2013

Remarks of Rongli Geng at IWLC2010

>60MV/m by Thin-Film coated Cavity

Look review lecture by T. Tajima(LANL) for Thin Film coated Cavity Nb 3 Sn : tri-niobium tin MgB 2 : magnesium di-boride Multi-layer thin film concept

T. Tajima

How to make thin-film on Nb? Look presentation by Chaoyue Cao (IIT) for Point Contact Tunneling as a Surface Superconductivity Probe of bulk Nb and (Nb 1-x Ti x )N Thin 5 th Thin Film workshop 2012(Jlab)

A thin film synthesis process based on sequential, self-limiting surface reactions between vapors of chemical precursors and a solid surface to deposit films in an atomic layer-by-layer manner. Atomic layer deposition (ALD) C. Cao

30 ALD thin film materials C. Cao

Advantages: Atomic-level control of thickness and composition Smooth, continuous, pinhole-free coatings on large area substrates No line-of-sight limits excellent conformality over complex shaped surfaces Coat inside Nb SRF cavity with precise, layered structure ALD 1 μm 200 nm ZnO Si ALD is very good at coating non-planar surfaces C. Cao

32 Multilayer thin films for SRF Superconductor-Insulator multilayer [ Gurevich, Appl. Phys. Lett. 88, (2006 )] Potential path to high E acc and high Q 0 d B0B0 B i =B 0 exp(-Nd/ L ) C. Cao

Nb 1-x Ti x N Thin Films made by ALD TEM Chemistry: (NbCl 5 :TiCl 4 ) + Zn + NH 3 at 450°C, 500°C Can vary Ti content with NbCl 5 :TiCl 4 ratio (1:2 ~ 20% TiN) Impurity content: 0.05 atom % Cl 21 sec/cycle ("NH3 dose"-"purge"-"MCl x dose"-"purge"-"Zn dose"-"purge ") C. Cao

34 Nb 1-x Ti x N-based superconductor-insulator structures Aluminum nitride: AlN Oxygen-free insulator, stable interface with Nb(Ti)N Good thermal conductivity (285 W/m-K) Similar structure to Nb(Ti)N –0.27% mismatch between in-plane spacing of (001)-oriented AlN and (111)- oriented NbN Can be grown with AlCl 3 and NH 3 at same temperature as Nb(Ti)N C. Cao

49nm Nb 0.8 Ti 0.2 N on AlN T c = 12.8K by SQUID 2Δ/kT c = (BCS limit) Δ(meV) Γ(meV) C. Cao

28nm Nb 0.8 Ti 0.2 N (without AlN layer) T c = 8.3K by SQUID Δ(meV) Γ(meV) C. Cao

Point contact tunneling (PCT) technique is ideal for measuring the local surface superconducting energy gap and density of states (DOS) of samples with a natural barrier. Nb 1-x Ti x N on AlN gives Tc = 12.8K, Δ = meV, 2Δ/kTc = (BCS limit). Nb 1-x Ti x N (without AlN) Tc = 8.3K. High quality gap region DOS, low zero bias conductance. Δ = meV. Conclusion Substrate Strained layer, low Tc 12.8 K C. Cao

Application of thin-film on Nb to ILC? Technology of; (1)nm-level Smooth Nb cavity surface, (2) Well controlled thin-film formation on Nb cavity, will be required. Then, we can reach >100MV/m with TESLA cavity shape. Tumbling, electro-polish, etc. Hydroforming without welding. Atomic Layer Deposition (ALD)

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