Spatial Amplification in a Disk-on-Rod Traveling-Wave Amplifier 1 Department of Nuclear Engineering and Radiological Sciences, University of Michigan,

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Spatial Amplification in a Disk-on-Rod Traveling-Wave Amplifier 1 Department of Nuclear Engineering and Radiological Sciences, University of Michigan, Ann Arbor 2 Air Force Research Laboratory, Kirtland AFB, Albuquerque, NM 3 Leidos Corporation, Reston, VA MIPSE Graduate Student Symposium October 7, Patrick Y. Wong 1, Brad Hoff 2, David H. Simon 1, David Chernin 3, Peng Zhang 1, Y.Y. Lau 1, Ronald M. Gilgenbach 1 Work supported by AFOSR Award No. FA , AFRL Award No. FA , and L-3 Communications.

Motivations and Objectives Motivations: Many high power microwave devices have narrow bandwidth, concentrating more on high power output Disk-on-Rod Traveling Wave Tube (TWT) may provide both high power output and wide bandwidth by its use of an annular beam (for high current) and slow-wave structure (for wide bandwidth) Objectives: Do an in-depth study of the viability of this Disk-on-Rod TWT Derive and solve the exact hot-tube dispersion relation to find the spatial amplification rate Compare against Particle-in-Cell code ICEPIC, MAGIC, and CHRISTINE Relate to Pierce’s General Theory of TWTs 2

τ a R w’ w b L h Schematic Diagram: Disk-on-Rod TWT 3 Electron Beam Disk-on-Rod Slow-Wave Structure Outer Shell

4 The cold-tube dispersion relation relates the angular frequency ω to the wavenumber (propagation constant) of the fundamental mode β 0 of the circuit wave in the absence of the electron beam

Cold-Tube Dispersion Relation Comparison 5 [1] D. M. H. Hung, I. Rittersdorf, P. Zhang et al., Phys. Rev. Lett. 115, (2015). Operating Point Absolute Instability [1] Good agreement between the analytic field theory, HFSS, and ICEPIC

(ω p = beam plasma frequency, R = plasma reduction factor)

Plasma Reduction Factor 7

Pierce’s General Three-Wave TWT Theory 8 Exact hot-tube dispersion relationPierce’s 3-Wave Dispersion Relation (approximate) General form of dispersion relation, exact or approximate: [Beam Mode] [Circuit Mode] = [Coupling Constant] C = coupling constant (proportional to R s ) QC = “space charge effect” (proportional to R N )

Dimensions [cm] b3.5 R2.8 a2.3 h1.3 w’0.3 w τ0.1 τ a R w’ w b L h Test Case Parameters 9 Operating Parameters V [kV] β 01 [m -1 ]100 f 01 [GHz]2.832

Spatial Amplification Rate vs Beam Current using Pierce Theory 10 The analytic theory, ICEPIC, CHRISTINE, and MAGIC all show general agreement

Frequency Response at 50 A DC beam current 11 There is fair agreement between theory and ICEPIC

Absolute Instability Simulated For the given test case parameters, there is an absolute instability at upper band edge [1]. The MAGIC simulations confirm this: 12 [1] D. M. H. Hung, I. Rittersdorf, P. Zhang et al., Phys. Rev. Lett. 115, (2015). SignalAbsolute Instability Signal Absolute Instability

Summary & Future Work The hot-tube dispersion relation for a Disk-on-Rod TWT driven by an annular electron beam is obtained. The cold-tube limit is verified by HFSS and ICEPIC The theoretical spatial amplification rate as a function of beam current agrees well with ICEPIC, MAGIC, and CHRISTINE for synchronous interaction. The agreement in the frequency response from the theory and ICPIC is only fair, a subject for future study. A possible absolute instability at upper band edge is observed in ICEPIC, also a subject for future study. 13