(Session 23 - Cathodes II )

Slides:



Advertisements
Similar presentations
CHAPTER 3 MICROWAVE ‘O’ TYPE TUBES
Advertisements

3D simulations of device performance for 3D-Trench electrode detector Jianwei Chen a,b, Hao Ding a,b, Zheng Li a,b,c, *, Shaoan Yan a,b a Xiangtan University,
2 Section.
Development of a W-Band TE 01 Gyrotron Traveling-Wave Amplifier (Gyro-TWT) for Advanced Radar Applications 1 Department of Applied Science, Univ. of California,
Experimental, Numerical, and Analytical Studies of a Staggered Double Vane Structure for THz Application 10 th International Vacuum Electronics Conference.
SYNTHESIS AND ELECTRICAL CHARACTERIZATION OF BULK FULLY DENSE NANOCRYSTALLINE ELECTROLYTES PREPARED BY HIGH-PRESSURE SPARK PLASMA SINTERING U. Anselmi.
The Effect of Pressure on the Microstructure and Mechanical Properties of Spark Plasma Sintered Silicon Nitride Anne Ellis, Leah Herlihy, William Pinc,
1 Challenges of carbothermic route of solar silicon synthesis M.A. Arkhipov, A.B.Dubovskiy, A.A. Reu, V.A. Mukhanov, S.A. Smirnova Quartz Palitra Ltd.
Second-Harmonic Fundamental Mode Slotted Peniotron Pulsed Power Plasma Science Conference, PPPS-2001 Las Vegas, NevadaJune 7-22, 2001 This work has been.
Department of Chemical Engineering University of South Carolina by Hansung Kim and Branko N. Popov Department of Chemical Engineering Center for Electrochemical.
Western Consortium on the NanoPhysics of Electron Dynamics near Surfaces in High Power Microwave Devices and Systems Ryan Umstattd Naval Postgraduate School.
Institute for Plasma Research MURI 99 Frequency Doubling Harmonic Gyro-TWT’s (development and experimental studies) We will complete the optimization of.
1 Chapter 27 Current and Resistance. 2 Electric Current Electric current is the rate of flow of charge through some region of space The SI unit of current.
TE 21 Second-Harmonic Gyro-TWT Amplifier with an Axis-Encircling Beam S.B. Harriet*, D.B. McDermott, and N.C. Luhmann, Jr. Department of Applied Science,
Simulations of Neutralized Drift Compression D. R. Welch, D. V. Rose Mission Research Corporation Albuquerque, NM S. S. Yu Lawrence Berkeley National.
R&D For Accelerating Structures H. Padamsee. TESLA Niobium, one meter length, rf = 1.3 GHz Copper, 53 cm, rf = 11.4 GHz.
Gaussian TEL gun progress V. Kamerdzhiev, G. Kuznetsov, V. Shiltsev LARP Collaboration Meeting 10 Danfords on the Sound, Port Jefferson, NY, April 23-25,
Plasma Arc Lamp Operation
Microwave semiconductor devices
PREPARATION OF ZnO NANOWIRES BY ELECTROCHEMICAL DEPOSITION
Conventional Tubes Conventional Device tubes cannot be used for frequencies above 100MHz 1. Interelectrode capacitance 2. Lead Inductance effect 3. Transit.
Numerical and Experimental Design Study of Quasi-Optical (QO) Multi-Gap Output Cavity for W-band Sheet Beam Klystron 10 th International Vacuum Electronics.
Norhayati Soin 06 KEEE 4426 WEEK 7/1 6/02/2006 CHAPTER 2 WEEK 7 CHAPTER 2 MOSFETS I-V CHARACTERISTICS CHAPTER 2.
AAC 2006V.Shiltsev 1 Electron beam generation and control in Tevatron Electron Lenses Vladimir Shiltsev, R.Hively, V.Kamerdzhiev, G.Kuznetsov, H.Pfeffer,
National Science Foundation Energetics of Pore Elimination Ricardo H. R. Castro, University of California-Davis, DMR Outcome: Researchers at University.
Operated by Los Alamos National Security, LLC for the U.S. Department of Energy’s NNSA U N C L A S S I F I E D Slide 1 Dynamic Electron Injection for Improved.
The propagation of a microwave in an atmospheric pressure plasma layer: 1 and 2 dimensional numerical solutions Conference on Computation Physics-2006.
Travelling Wave Tube For Broadband amplifier helix TWTs (proposed by Pierce and others in 1946 ) are widely used For High average power purposes the.
CLIC meeting, Prospects for developing new tubes I. Syratchev, CERN.
Study of UV absorption and photoelectron emission in RPC (Resistive Plate Counters) detector with an UV source Carlo Gustavino (INFN-LNGS) RPC and their.
Aerosol Limits for Target Tracking Ronald Petzoldt ARIES IFE Meeting, Madison, WI April 22-23, 2002.
High gradient acceleration Kyrre N. Sjøbæk * FYS 4550 / FYS 9550 – Experimental high energy physics University of Oslo, 26/9/2013 *k.n.sjobak(at)fys.uio.no.
The selection of operating mode for 10MW L-band MBK with high efficiency Institute of Electronics, Chinese Academy of Sciences Beijing, China November.
Development of The Klystrons for J-PARC Project
Effect of Re Alloying in W on Surface Morphology Changes After He + Bombardment at High Temperatures R.F. Radel, G.L. Kulcinski, J. F. Santarius, G. A.
Ka and W Band TE 01 Gyro-Devices Stutend : Yo-Yen Shin Advisor : Yi Sheng Yeh Department of Electrical Engineering, Southern Taiwan University of Technology,
Spatial Amplification in a Disk-on-Rod Traveling-Wave Amplifier 1 Department of Nuclear Engineering and Radiological Sciences, University of Michigan,
MVE MURI 99 Kick-off Meeting R. Barker, Technical Monitor Started 1 May 99 October 1999 Overview of UCD MURI Gyro-Device Program PI: Prof. N.C. Luhmann,
1 W-Band Harmonic Multiplying Gyrotron Traveling Wave Amplifier Student : ChiaWei Hung Advisor : Yi Sheng Yeh.
O. Jambois, Optics Express, 2010 Towards population inversion of electrically pumped Er ions sensitized by Si nanoclusters Jeong-Min Lee
2015 International Perforating Symposium Europe 2015 International Perforating Symposium Europe 1 PENETRATION OF HIGH DENSITY TUNGSTEN BASE POROUS JETS.
47th Annual Meeting of the Division of Plasma Physics, October 24-28, 2005, Denver, Colorado ECE spectrum of HSX plasma at 0.5 T K.M.Likin, H.J.Lu, D.T.Anderson,
Second Harmonic TE 21 Gyrotron Backward Wave Oscillator 報 告 人:吳 庭 旭 指 導 教 授:葉 義 生 老師 南台科技大學 電機所.
Improved Distributed - Loss Gyro-TWA Yi Sheng Yeh, Chi-Wen Su, Yu-Tsung Lo, Ting-Shu Wu, Department of Electrical Engineering, Southern Taiwan University.
RF System and EBIS of RAON
MICROWAVE AMPLIFIERS Alan Phelps A.W. Cross, K. Ronald, C.G. Whyte, A.R. Young, W. He, I.V. Konoplev, A.W. Cross, K. Ronald, C.G. Whyte, A.R. Young, W.
Doubly Convergent Multiple Beam Guns Lawrence Ives, Thuc Bui, Michael Read Calabazas Creek Research, San Mateo, CA. USA Adam Attarian, Billy Tallis, Cynthia.
Linac RF System Design Options Y. Kang RAD/SNS/NScD/ORNL Project – X Collaboration Meeting April , 2011.
Objectives Approach Accomplishments & Future  Experimentally demonstrated RPM oscillation  Simulations predict Mode-Control-Cathode (MCC) phase-locks.
SPES Target Group Data…… INFN-CISAS-CNR collaboration The Ablation Ion Source for refractory metal ion beams A preliminary design.
Prospects for developing new tubes
KCS 2016 Multilevel Resistive Switching Memory based on Two-Dimensional (2D) Nanomaterials Gwang Hyuk Shin, Byung Chul Jang, Myung Hun Woo, and Sung-Yool.
High efficiency work and MBK development for accelerators
Beam dynamics simulation with 3D Field map for FCC RF gun
Development of X-band 50MW klystron in BVERI
Preliminary results for electron lens with beam current of 20 A
Yeong-Shin Park and Y. S. Hwang
Simulation of Luminosity Variation
Dispersion of Carbon Nanotubes in Alumina using a Novel Mixing Technique and Spark Plasma Sintering of the Nanocomposites with Improved Fracture Toughness.
A.V. Rogov1, Yu.V. Martynenko1,2, Yu.V. Kapustin1, N.E. Belova1
140kW, 94GHz Heavily Loaded TE01 Gyro-TWT
Poster T8-We-43 Generation of Boron Ion Beams by Vacuum Arc Ion Source with Lanthanum Hexaboride and Boron Carbide Cathodes V. Frolova, A. Nikolaev, E.
High Efficiency X-band Klystron Design Study
High Efficiency X-band Klystron Design Study
DOE Plasma Science Center Control of Plasma Kinetics
MEBT1&2 design study for C-ADS
Physics Design on Injector I
On the Korean Contributions for
Gain Computation Sven Reiche, UCLA April 24, 2002
Plans for future electron cooling needs PS BD/AC
Presentation transcript:

(Session 23 - Cathodes II ) 13:40 Thursday, 30 April 2009 High Current Density and Long Life Nanocomposite Scandate Dispenser Cathode Fabrication Jinfeng Zhao, Larry Barnett, and Neville C. Luhmann Jr. Department of Applied Science, University of California-Davis (UCD), CA 95616, USA Na Li and Ji Li Beijing Vacuum Electronics Research Institute, Beijing, China 10th International Vacuum Electronics Conference (IVEC2009) April 28 - 30th 2009

Why W-Sc Nanopowder Cathodes ? Millimeter/THz sources require reduced cathode area and low to moderate beam compression →high current density fully space charge limited operation:30 -100+ A/cm2 Gyro-TWTs at W-Band and beyond require smooth surfaces for reduced velocity spread (proportional to roughness(1/2)), uniform emission, and high current density: 40+ A/cm2 End of tube life often due to barium deposits leading to arcing as well as Ba depletion →low temp. operation critical (lifetime improvement by x4 for each 50 °C reduction) Long lived HPM cathodes for conditioning and rep rated operation: 100+ A/cm2

Gyro-TWT Performance Dependence on Beam Quality Nonlinear large signal code predicts output power, efficiency and gain For predicted velocity spread Dvz/vz = 5% -Bandwidth Dw/w = 5% - Pout= 110 kW - h = 22% - Large signal gain = 45 dB

Impact of Cathode Roughness on MIG* Beam Velocity Spread W-Sc Nanopowder Conventional Scandate Cathode New UCD MIG Design: 50 degree cathode with compression of only 12 (Bgun=3.0 kG). EGUN gives 3.9% axial spread and 1.7% transverse spread.

BVERI-BJUT W-Sc Nanopowder Cathode Concept Benefit of adding scandia into nano tungsten powder by chemical synthesis Improve emission uniformity. Increase emission capability. Resist ion bombardment. Nano sized scandia-doped tungsten powder Combined by aqueous solution method (Liquid-solid or Liquid-liquid ) Spherical tungsten grains Scandium oxide absorb on the surface of spherical tungsten grains. Sc-W powders with more uniformly distributed Sc2O3 were obtained Space charge limited current densities of more than 30 A/cm2 at 850 oCb achieved 500 hours achieved at 100 A/cm2 in tests at SLAC Data from Beijing Vacuum Electronics Research Institute (BVERI) & Beijing University of Technology (BJUT)

1. Nano Sc2O3-doped W powder Fabrication Nano Composite Cathode Fabrication—UCD Optimize Nano composite Sc2O3-doped W matrix 1. Nano Sc2O3-doped W powder Fabrication Sol-Gel Process

Nano Sc2O3-added W Powder Fabrication—UCD Sc2O3-added W powders SEM Results

Nano Sc2O3-added W Powder Fabrication—UCD Sc2O3-added W powders SEM Results

Nano Sc2O3-added W Powder Fabrication—UCD Sc2O3-added W powders SEM Results

Nano Sc2O3-added W Powder Fabrication—UCD Sc2O3-added W powders SEM Results

Nano Sc2O3-added W Powder Fabrication—UCD Sc2O3-added W powders SEM Results

Nano Sc2O3-added W Powder Fabrication—UCD Conclusions: Uniform Nano Sc2O3-doped W powder has been made with different particle size, such as average particle size around 72 nm, 146 nm, 272 nm, and 614 nm, respectively.

Sc2O3-added W Matrix — UCD Top Surface By using 72 nm initial nano powder After Regular Furnace Sinter Grain size in matrix is 400-500 nm Pore size ~ 400 nm Cross Section

Sc2O3-added W Matrix — UCD Top Surface By using 272 nm initial nano powder After Regular Furnace Sinter Grain size in matrix is 500-600 nm Pore size ~ 400 nm Cross Section

Sc2O3-added W Matrix — UCD Top Surface By using 587 nm initial nano powder After Regular Furnace Sinter Grain size in matrix is 1 – 2 µm Pore size ~ 0.5 µm Cross Section

Sc2O3-added W Cathode — UCD SEM images on the top surface of UCD cathode After Furnace Sinter: Average grain size in cathode is 600 nm and very uniform

Sc2O3-added W Cathode — UCD SEM images on the top surface of UCD cathode After Furnace Sinter: Average grain size in cathode is 700 nm and very uniform

Sc2O3-added W Cathode — UCD SEM images on the top surface of UCD cathode After Furnace Sinter: Average grain size in cathode is 900 nm and very uniform

Cathode Testing at BVERI Current Density vs Cathode Button Voltage J = 73.56 A/cm2 , 1000 °C Using UC Davis Material

Cathode Testing at UC Davis Multiple rapid cathode life test facility New High Perveance Cathode Life Test Vehicle Rapid button test System operational Cathode testing and life testing underway at UC Davis: eight vehicles operational with another four nearing completion G. Scheitrum and A. Hasse Three 3.0 P CLTVs completed

Cathode Testing at UC Davis Current Density versus Cathode Button Voltage Comparison: Spectra-mat 311X 20 A/cm2 at 1150 °C UCD cathode: 80 A/cm2 fully space charge limited

Cathode Testing at UCD Current Density vs Cathode Button Voltage UC Davis Pellet impregnated by Spectra-Mat

Interpretation of Cathode Testing Results at UC Davis The 1150o C data increases to 40 A/cm2 and drops slightly from the SCL line (slope of 1.5),then continues to 80 A/cm2 at a slope of 1.5 (full space charge limited). Interpreted as field emission in the high current range where the deviation from the ideal SCL (zero extraction voltage) is not a drop in emission current capability, but a drop in the actual space charge limited current due to the required extraction field.

Interpretation of Cathode Testing Results at UC Davis Speculate that field emission points are formed: The optimum point formation, density of points and/or sharpness of the points, is at ~1150o Cb The initial activation is very fast at ~1150o Cb and minimal at < 1100o Cb Assuming the point density is proportional to the number of grains leads to the conclusion that smaller grains will have more points and the cathode will have higher emission density up to the limit that it starts decreasing the field on each point and limiting total emission. Hence, there is a maximum grain-point density (under study)

Cathode Testing Summary Spark Plasma Sintering Summary of cathode testing: 80 A/cm2 fully space charge limited current density has been obtained at 1150 oCb Cathode life testing has been at 1150 oCb for 800 h following 768 h at 950 oCb Cathode made by smaller particles had 50/cm2 emission at 1050 oCb Future Plans for cathode testing: Investigate performance of cathodes made by different initial Sc2O3-W nanopowder average particle sizes: 100, 300, 500 nm, etc. Cathodes made with different porosities Cathodes made with different Sc2O3 concentrations Investigate robustness with respect to reactivation Conduct life tests in new 3.0 P CLTV’s Spark plasma sintering Sumitomo SPS-2050 Spark Plasma Sintering

Thank You Work supported by: AFOSR under Grant F9550-99-04-1-0353 (MURI04 “NanoPhysics of Electron Dynamics near Surfaces in High Power Microwave Devices and Systems”) NSWC Crane HiFIVE DARPA, Contract No. G8U543366, through a subcontract from Teledyne Scientific.

TE01 Gyro-TWT Dispersion Diagram 27/34 TE01 Gyro-TWT Dispersion Diagram w = sWc + kzvz s = 1 s = 2 kz(/m) 50 100 150 200 -4000 4000 w/2p (GHz) TE11(1) TE21(1) TE01(1) TE02(2) operating point (grazing intersection) Potential Gyro-BWO interaction s=1 s=2 100 kV, a=1.0 Beam mode dispersion: w = sWc + kzvz Wave mode dispersion: w2 = wc2 +c2kz2 Absolute instabilities must be stabilized : TE11(1), TE21(1), TE02(2) ,TE01(1)