Magnetron sputtering of Superconducting Multilayer Nb3Sn Thin Film
Magnetron sputtering of Superconducting Multilayer Nb3Sn Thin Film Magnetron sputtering of Superconducting Multilayer Nb3Sn Thin Film
1008038.5°{110}sample1sample2sample3elative intensity604069.6°{211}20055.5°{200}82.5°{220}95.1°{310}121.7°{321}40 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.36 the XRD result of Run 11008038.5°{110}69.6°{211}sample1sample2sample3elative intensity60402055.5°{200}82.5°{220}95.1°{310}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.37 the XRD result of Run 21008038.5°{110}69.6°{211}sample1sample2sample3elative intensity60402055.5°{200}82.5°{220}95.1°{310}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.38 the XRD result of Run 336
1008038.5°{110}69.6°{211}sample1sample2sample3elative intensity60402055.5°{200}82.5°{220}95.1°{310}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.39 the XRD result of Run 410038.5°{110}69.6°{211}95.1°{310}sam ple2sam ple380elative intensity60402055.5°{200}82.5°{220}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.40 the XRD result of Run 51008038.5°{110}69.6°{211}sample1sample2sample3elative intensity60402055.5°{200}82.5°{220}95.1°{310}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.41 the XRD result of Run 637
- Page 1: UNIVERSITÀ DEGLISTUDI DI PADOVAFac
- Page 7 and 8: IndexINDEX ........................
- Page 9 and 10: IntroductionThe superconductor acce
- Page 11 and 12: Fig. 1.1 Disc-loaded traveling-wave
- Page 13 and 14: In Type-II superconductors, vortex
- Page 15 and 16: needed for preventing the supercond
- Page 17 and 18: The B1 crystal structure has a cubi
- Page 19 and 20: NbN cavities literature, is often h
- Page 21 and 22: superconducting magnet construction
- Page 23 and 24: 775°C. From the same diagram, it i
- Page 25 and 26: two types of electrons at the Fermi
- Page 27 and 28: Of course, there are some other kin
- Page 29 and 30: as shown in Fig.2.3. The four opera
- Page 31 and 32: Fig.2.8 turbomolecular pumpFig. 2.9
- Page 33 and 34: Fig. 2.14 The chamber covered with
- Page 35 and 36: Fig. 2.17 the gasket and the magnet
- Page 37 and 38: shown in Fig. 2.21 and Fig. 2.22. T
- Page 39 and 40: Fig. 2.26 The interface of the surf
- Page 41 and 42: Fig. 2.30 put the sample into the T
- Page 43: Fig. 2.34 the performance of the th
- Page 47 and 48: 2dsinθ= nλ (2.3)Fig.2.44 the diff
- Page 49 and 50: Chapter 3 Multilayer deposition of
- Page 51 and 52: 1 minute. The time of depositing mu
- Page 53 and 54: chamber 1 and is connected to the s
- Page 55 and 56: 3.2.2.2 Analysis resultⅠ The thic
- Page 57 and 58: In order to detect the component of
- Page 59 and 60: measure the RRR. So the resistance
- Page 61 and 62: 110100903480relative Intensity70605
- Page 63 and 64: frequency of the cavity which is in
- Page 65 and 66: Fig. 3.28 the inductor coilDuring t
- Page 67 and 68: Fig. 3.32 fixing the sample with Nb
- Page 69 and 70: second transition temperature is th
- Page 71 and 72: source is the bulk Nb sample. Altho
- Page 73 and 74: of 1A in the Fig. 3.37 and Fig. 3.4
- Page 75 and 76: Table 3.10 the description of the p
- Page 77 and 78: 1101001.0A10'-IND3 45 6 7 9 1011 12
- Page 79 and 80: 1101009080341.8A10'INDrelative inte
- Page 81 and 82: Reference1. A. Godeke, Nb3Sn FOR RA
1008038.5°{110}sample1sample2sample3elative intensity604069.6°{211}20055.5°{200}82.5°{220}95.1°{310}121.7°{321}40 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.36 the XRD result <strong>of</strong> Run 11008038.5°{110}69.6°{211}sample1sample2sample3elative intensity60402055.5°{200}82.5°{220}95.1°{310}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.37 the XRD result <strong>of</strong> Run 21008038.5°{110}69.6°{211}sample1sample2sample3elative intensity60402055.5°{200}82.5°{220}95.1°{310}121.7°{321}040 50 60 70 80 90 100 110 120 130 140Angle[degree]Fig. 2.38 the XRD result <strong>of</strong> Run 336
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