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Athmospheric Surface Treatments for improving 6Ghz Niobium cavities V. Palmieri, A. Rossi, K. Atroshchenko, D. Rizetto, A. Camacho, S.Yu. Stark * INFN – Legnaro National Laboratories University of Padua
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6 Ghz @4,2K Bulk Nb
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Low research budget Large amount of cavities 6 GHz
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Resistive Samples Pillbox cavities, etc Real cavities Inductive H c1 Measurement Calorimetric methods R S Differential measurements Microstrip Resonators 6 GHz cavities 1,5 /1,3 GHz monocells 1,3 GHz 3-cell cavity 1,3 GHz 9-cell cavities
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Proceedings of the 8 th SRF Workshop, Abano Terme, 1997
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Antonio 3 Rossi L L M
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No electron beam welding, neither for flanges Obtained by spinning from Nb scraps Short fabrication time Fast and low cost BCP and EP treatments Inexpensive Cryogenics Quick RF Measurements 6 GHz CAVITY MINILAB
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6 Ghz Cavity Geometry 20 mm 36 mm Seamless flanges [mm] Flange Area = 7 cm 2
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Cavity fabrication By Spinning from scraps of spun 1.5 GHz 1.5 GHz Cavity 6 GHz Cavity 40 cm
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Mini Mechanical Tumbling SiCZrO 2 Al 2 O 3 + SiO 2
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Mini EP
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A Mini – BCP / EP Lab
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6 GHz CAVITY MINI-furnace
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6 GHz CAVITY MINI-Camera
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Ready for the RF measurement
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6 GHz CAVITY: MINI-Kapton gasket
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Kapton® disc Cryogenic infrastructure Easy RF Measurement system: Pick Up Coupler (mobile) Pumping line Vacuum seals: (Two kinds) Indium wire INSERT
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Cryogenic infrastructure: Pick Up Coupler (mobile) Double Pumping line Bottom Part Pick-up Antenna Coupler Antenna Pick-up-Pipe Coupler - Pipe Pick-up Flange Bellow Coupler Flange The Bottom Part
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Cryogenic infrastructure: Triple Stand μ-metal Screen cavity
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Quick RF Measurements The insert has been conceived to even enter into a 450 lt Helium dewar INSERT DEWAR RF measuring system
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List of Dogmas 6 GHz cavities are not representative Any other flange, that is not Nb-Ti, is not reliable Kapton joints will not work … and even if they work, they will not be used!
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Nomogram (after Benvenuti, Palmieri, Vaglio) T = 4.2 K f = 500 MHz, s = 4
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List of Dogmas 2000° C is a too high temperature Over 1000°C you’ve contamination from crucibles and you will loose the dimensional control You can’t work around melting point of Niobium
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Fast ( takes only few sec) Cheap (Vacuum Technology Free) Simple (No need of special expertise) High Temperature Rapid Metathesis (Nitriding in Mushy State) The Process is:
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6 Ghz @4,2K Bulk Nb
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List of Dogmas You necessarily need good vacuum You must limit yourself to select only those A15 that can be prepared at T around 900°C In any case B1 and A15 materials will never work
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The Homologous Temperature 0 1 T [K] = = T m [K] for Nb 2467 °C
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T [K] = = T m [K] for Nb 0 0,81 2467 °C 1924 °C Mushy State
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T [K] = = T m [K] 0,98 0,9 1 2467 °C 2196 °C Mushy State 0,96 2357 °C2412 °C Premelting
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Premelting (also Surface melting) Even below its melting point (T m ), quasi-liquid films can be observed on crystalline surfaces
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The thickness of the quasi-liquid film is T - dependent This effect is common for all crystalline materials Premelting (also Surface melting)
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Nb NbN 3 mm Nb NbN
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-Nb N -Nb N
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Surface layers
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Nb 5 N 6 ; N 4 N 3 NbN 1-x ; -NbN (hexagonal); ’ NbN (hexagonal); -Nb2N (hexagonal); -Nb 4 N 3-x -Nb (N) (bcc solid solution) Niobium
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Bulk Nb NbN
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Temperature Time T m of Nb 3 – 30 sec
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As the -NbN -Nb 4 N 3-x phase transformation is a very fast, quasi-continuous Transition, it cannot be avoided by quenching
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Annealing doesn’t work
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Bulk Nb NbN
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Bulk Nb NbN
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Bulk Nb
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Nb 2 O 5 Melting point1512 °C Evaporation temperature 1700-1900 °C
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When the N/Nb ratio > 0.84, the -phase can be retained by quenching At N/Nb ratio < 0.8 it transforms in -Nb 4 N 3
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NbN @4,2K T = 4,2 K Bulk Nb
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High Temperatures for Nb Purification
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Bare Sample
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Conclusions 6 Ghz cavities allow a fast and dense statistics At 4,2 K the Q-value at low field increases of even a factor 5 The important parameters are given by the 3-T rule
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6 GHz
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6 Ghz @4,2K Bulk Nb
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