RUPAC2012 - List of Authors (Khoruzhiy, V.M.)

Paper	Title	Page
TUPPB014	Cooling of Electron Beams	342
	V.M. Khoruzhiy NSC/KIPT, Kharkov, Ukraine
	Cooling of electron beams (transversal velocities reducing) in storage rings (cyclic accelerators) may be realized using gyromonotron device as part of storage ring at straight-line portion. The gyromonotron is a HF oscillator for cm and mm band of wavelength in which electron beam with nonzero transversal velocities is used for excitation electromagnetic wave. Energy of transversal motion of electron beam converts into energy of electromagnetic wave during multiple passing the same bunches with repetition frequency f0 through gyromonotron. We choose frequency f0 (and corresponding wavelength AL) as minimal frequency (H111 mode) for gyromonotron's resonator. As well known, frequency f0 of H111 mode gives possibility to determine radius of the resonator R~AL/(21.71). We assumed above that resonator's length L/(2R)>1. It is possible for gyromonotron's solenoid to determine longitudinal magnetic field Hz(kOE)=11/AL(cm) for low relativistic beam's energy. For gyromonotron's operation at given frequency it's needed realization of condition for relativistic cyclotron frequency Om_rel/(23.14)~ f0. Emitted beam radiation dissipates inside gyromonotron’s resonator (output window is absent). Q-quality gyromonotron’s resonator and pitch factor PF of electron beam have to satisfy condition Q PF>1 (for "warm" or superconducting (SC) resonators).

Paper

Title

Page

Cooling of Electron Beams

342

V.M. Khoruzhiy
NSC/KIPT, Kharkov, Ukraine

Cooling of electron beams (transversal velocities reducing) in storage rings (cyclic accelerators) may be realized using gyromonotron device as part of storage ring at straight-line portion. The gyromonotron is a HF oscillator for cm and mm band of wavelength in which electron beam with nonzero transversal velocities is used for excitation electromagnetic wave. Energy of transversal motion of electron beam converts into energy of electromagnetic wave during multiple passing the same bunches with repetition frequency f0 through gyromonotron. We choose frequency f0 (and corresponding wavelength AL) as minimal frequency (H111 mode) for gyromonotron's resonator. As well known, frequency f0 of H111 mode gives possibility to determine radius of the resonator R~AL/(2*1.71). We assumed above that resonator's length L/(2*R)>1. It is possible for gyromonotron's solenoid to determine longitudinal magnetic field Hz(kOE)=11/AL(cm) for low relativistic beam's energy. For gyromonotron's operation at given frequency it's needed realization of condition for relativistic cyclotron frequency Om_rel/(2*3.14)~ f0. Emitted beam radiation dissipates inside gyromonotron’s resonator (output window is absent). Q-quality gyromonotron’s resonator and pitch factor PF of electron beam have to satisfy condition Q* PF>1 (for "warm" or superconducting (SC) resonators).