Introduction Sample deposition system Cavity deposition system prototype Surface characterization Beyond niobium

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Transcription:

Genfa Wu Introduction Sample deposition system Cavity deposition system prototype Surface characterization Beyond niobium 1

United We Stand Succeed JLAB ECR thin film collaboration: JLAB: L. Phillips, R. Rimmer, A-M. Valente, H. Wang, A. Wu, G. Wu Cornell: H. Padamsee (LEPP), L. Hand (Physics) College of William and Mary: M. Kelley SANDIA: T. Renk Black Laboratory: R. Crooks 2

a glow discharge can be established using only metal vapor but the discharge is very unstable and this method is generally not practical. -- R. F. Bunshah, et., al., Deposition Technologies for Films and Coatings 3

Energetic deposition process Movchan-Demchishin Zone Model (MDT) An illustration of approximate deposition energy is shown in above figure. Different materials will have different energy ranges. J. A. Thornton, JVST, Vol. 11, No. 4, (1974) p666 4

The illustration of the energetic vacuum deposition by ECR plasma 5

Cavity deposition prototype 1200 1100 1000 B field [gauss] 900 800 700 600 0.0 0.5 1.0 1.5 2.0 Z Axis [in] 2.5 3.0 0.0 1.5 1.0 0.5 3.0 2.5 2.0 R Axis [in] Sample deposition system 7.5kW hearth, 130 A/s 1200 1100 1000 B field [gauss] 900 800 700 600 0.0 0.5 1.0 1.5 2.0 Z Axis [in] 2.5 3.0 0.0 1.5 1.0 0.5 R Axis [in] 3.0 2.5 2.0 Cavity deposition system 15 kw Rod-fed, 100 A/s 6

Cavity deposition prototype 9 10 8 7 11 12 6 System design of the Nb thin film coating on a 500MHz Cu cavity (1) 14kW rod-fed E-gun (2) 9000 l/s cryopump system (3) bucking coil for E-gun (4) top and bottom iron yokes (outer iron shield is removed for illustration) (5) center coils (6) Nb grid tube (7) bias insulator (8) WR284 waveguide E-bend and horn to the grid tube (9) T vacuum chamber (10) top coil (11) Cu cavity (12) bottom coil. 5 4 3 2 1 7

RF radiation 8

Optical image of copper surface Mechanical polished 100 µm chemical polished 120 µm Electropolished 15 µm after chemical etching Surface from BCP/EP was wavy Time consuming for Mech/EP 9

Low temperature Characterization Function Generator SC thin film 100 Ω 20MΩ Lock-in Amplifier A C D B THIN FILM SAMPLE 10

Transition temperature and RRR T r a n s i t i o n W i d t h T [ K ] 1. 5 1. 0 0. 5 0. 0 T T 6 2 0 3 0 4 0 5 0 6 0 7 0 8 0 9 0 1 0 01 1 0 S u b s t r a t e b i a s v o l t a g e [ V ] 1 1 1 0 9 8 7 T r a n s i t i o n T e m p e r a t u r e T [ K ] T r a n s i t i o n W i d t h T [ K ] 1. 5 1. 0 0. 5 T T 0. 0 6 5 0 6 0 7 0 8 0 9 0 1 0 0 S u b s t r a t e b i a s v o l t a g e [ V ] Bias voltage effect on transition temperature and transition width, measured by an inductive method. Substrate is A-cut sapphire (left), Substrate is electropolished copper (right). 1 1 1 0 9 8 7 T r a n s i t i o n T e m p e r a t u r e T [ K ] R R R 5 0 4 0 3 0 2 0 1 0 0 5 0 1 0 0 1 5 0 2 0 0 2 5 0 F i l m t h i c k n e s s [ n m ] T c = (T 90% + T 10% )/2 T c = (T 90% - T 10% )/2 11

Film characterizations SEM X-ray diffraction AFM Nb/Cu-90 Film RMS=94 nm, profilometer SIMS TEM 12

Summary of thin film sample Niobium Ion Energy is around 63 ev without bias voltage, and controllable. Cryogenically, the process achieves a reasonably high RRR niobium thin film with excellent superconducting transition temperature and width. RRR appears to be more closely related to the film thickness than to the deposition energy. Epitaxial growth of niobium on sapphire has been achieved. The substrate bias voltage of -60 V is believed to be the preferred value based on the transition width, the crystal orientation spread, and the AFM results. For a copper substrate, a better film quality likely requires higher deposition energy than sahhpire substrate, which needs further studies. 13

Summary of thin film sample (cont.) based on SIMS analysis Nb-Cu sample surfaces are smooth locally Nb-Cu surfaces may have much less hydrocarbons and other residuals or contaminants as compared with those on the Nb surfaces obtained conventionally (BCP or EP). Nb-Cu samples appear to have more oxygen on the surfaces and oxygen penetrates deeper into the interior of the samples. This may be resulted from the residual gases in the deposition chamber and from the fact that the grain size of Nb-Cu is small. 14

Beyond niobium, Material, we will look at: NbN, NbTiN, Nb3Sn, MgB2 Process we can setup: (Bias) Sputtering, Plasma, PLD. Collaboration process: Vacuum Arc, pulsed ion ablation Low power application: 4k medium performance for university or hospital operation. High power application: 4K high performance for compact, high power FEL 15