Study of a biperiodic slow-wave structure at medium energies

In the present work charged particle accelerators occupy the important place both in scientific, and in practical applications.

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Бібліографічні деталі
Дата:1999
Автори: Zagorodnov, O.G., Papkovich, V.G., Khizhnyak, N.A.
Формат: Стаття
Мова:English
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 1999
Назва видання:Вопросы атомной науки и техники
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/81364
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Study of a biperiodic slow-wave structure at medium energies / O.G. Zagorodnov, V.G. Papkovich, N.A. Khizhnyak // Вопросы атомной науки и техники. — 1999. — № 3. — С. 47. — Бібліогр.: 2 назв. — англ.

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spelling irk-123456789-813642015-05-15T03:02:30Z Study of a biperiodic slow-wave structure at medium energies Zagorodnov, O.G. Papkovich, V.G. Khizhnyak, N.A. In the present work charged particle accelerators occupy the important place both in scientific, and in practical applications. 1999 Article Study of a biperiodic slow-wave structure at medium energies / O.G. Zagorodnov, V.G. Papkovich, N.A. Khizhnyak // Вопросы атомной науки и техники. — 1999. — № 3. — С. 47. — Бібліогр.: 2 назв. — англ. 1562-6016 http://dspace.nbuv.gov.ua/handle/123456789/81364 en Вопросы атомной науки и техники Національний науковий центр «Харківський фізико-технічний інститут» НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description In the present work charged particle accelerators occupy the important place both in scientific, and in practical applications.
format Article
author Zagorodnov, O.G.
Papkovich, V.G.
Khizhnyak, N.A.
spellingShingle Zagorodnov, O.G.
Papkovich, V.G.
Khizhnyak, N.A.
Study of a biperiodic slow-wave structure at medium energies
Вопросы атомной науки и техники
author_facet Zagorodnov, O.G.
Papkovich, V.G.
Khizhnyak, N.A.
author_sort Zagorodnov, O.G.
title Study of a biperiodic slow-wave structure at medium energies
title_short Study of a biperiodic slow-wave structure at medium energies
title_full Study of a biperiodic slow-wave structure at medium energies
title_fullStr Study of a biperiodic slow-wave structure at medium energies
title_full_unstemmed Study of a biperiodic slow-wave structure at medium energies
title_sort study of a biperiodic slow-wave structure at medium energies
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
publishDate 1999
url http://dspace.nbuv.gov.ua/handle/123456789/81364
citation_txt Study of a biperiodic slow-wave structure at medium energies / O.G. Zagorodnov, V.G. Papkovich, N.A. Khizhnyak // Вопросы атомной науки и техники. — 1999. — № 3. — С. 47. — Бібліогр.: 2 назв. — англ.
series Вопросы атомной науки и техники
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AT papkovichvg studyofabiperiodicslowwavestructureatmediumenergies
AT khizhnyakna studyofabiperiodicslowwavestructureatmediumenergies
first_indexed 2025-07-06T06:06:06Z
last_indexed 2025-07-06T06:06:06Z
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fulltext STUDY OF A BIPERIODIC SLOW-WAVE STRUCTURE AT MEDIUM ENERGIES O.G.Zagorodnov, V.G.Papkovich, N.A.Khizhnyak NSC KIPT, Kharkov, Ukraine In the present work charged particle accelerators occupy the important place both in scientific, and in practical applications [1]. The wide spectrum of accelerator applications compels the developers to upgrade existing and to develop new accelerating structures to conform the most full up-to-date requirements in technical and physical characteristics (energy, currents etc.), as well as in practical (e.g. weight and size), including financial and economic ones. The biperiodic, coupling on a π-wave slow-wave structure (BSWS) [2] can serve as one of such versions of the proton linac accelerating structure in the energy range (20-100) MeV (0.15<β<0.45). In such BSWS quarter wavelength the strip-geometry resonators are as accelerating cells. Coupling resonators are chosen as the quarter wavelength resonators too, but they are made as a loop. These loopback coupling resonators are put in accelerating resonator electromagnetic field symmetry planes. Shorting metal planes are put in end faces of BSWS. The accelerating resonators are placed at distances of a quarter wavelength (λg/4) from the faces of shorting metal plates. Thus, they are in places of BSWS crests, whereas the loopback coupling resonators are placed in nodes of the BSWS. Accordingly, all coupling resonators are unexcited. 0 0 . 2 5 0 . 7 5 1 0 1 z / L E / E 0 d r i f t t u b e g a p d r i f t t u b e Fig. 1. The electrical field distribution along a gap The high-frequency accelerating fields in the BSWS are π/2- modes, i.e. the phase shift between neighbouring resonators of link and accelerating resonators is equal to π/2. In BSWS the interaction of accelerated charged particles with a slow wave is the π- interaction. Therefore BSWS operation is chosen under the standing wave condition as the most practical one. The measurements of BSWS parameters were carried out on an experimental structure model. There are four copper rings with a diameter D = 201 mm in the model. Two-quarter wavelength accelerating vibrators and one loopback coupling resonator are inside of it. The length L0 of each ring is equal to a quarter of a wavelength in BSWS and makes 39 mm, so the wavelength is λg = 4L0 = 0,156 m. The electrical accelerating field distribution (in relative units, E0 is an electric field strength in the gap middle) on the accelerator axis in the middle gap between two neighbouring accelerating electrodes is shown in Fig.1. The common observed dates are shown in Table 1. Table 1. Main parameters of investigated BSWS Resonator length (in BSWS one wavelength is two accelerating vibrators). m, λg = 4L0 0,156 Total effective length of gaps in the resonator, m, geff 0,083 5 Working frequency of π- wave, MHz, f0 475,3 Free space wavelength, m, λ0 0,631 Phase velocity in BSWS at working frequency of π-mode, βph 0,247 Energy of accelerated protons, MeV, W 30 Own quality-factor of the half wavelength resonator, Q1 2975 Own quality-factor of the resonator on one wavelength, Q2 3854 Quality-factor of the indefinitely long resonator, Q∞ 5514 Displacement of frequency by a metal ball (r = 2,6.10-3 m), Hz, ∆f 99277 Efficiency of a gap, T 0,859 Shunt impedance, MΩ/m, Rsh 16,7 The relation of shunt impedance to quality- factor, MΩ/m, Rsh/Q∞ 3028 Effective shunt impedance, MΩ/m, Zeff 25,86 Attenuation field constant, mcs, τ = Q∞/πf0 3,69 Depth of a skin layer, micron, δ 3 Relation of a wavelength to a diameter, λ0/D 3 Table 2. A comparison of accelerating structures (given for f = 150 MHz) Structure BSWS Alvarez H111 Rsh/Q∞, MΩ/m 955 Zeff , MΩ/m 14,53 29 9 Q∞ 9785 60000 (94475) τ, mcs 20 127 (200) δ, micron 5,4 * In brackets the computed values are given. Thus, the BSWS under consideration should have values Zeff of about (20-27) MΩ/m. It is much higher than the effective shunt impedance of structures with a parallel connection of gaps and is comparable to values Zeff of Alvarez structure at a working frequencies of 150 MHz in the considering energy range being investigated. REFERENCES 1. CERN Courier. Applying the Accelerator. Special issue. 1995. Vol.35. P.1-25. 2. O.G.Zagorodnov, V.G.Papkovich, N.A.Khizhnyak. An investigation of biperiodic slow-wave structure. Preprint KIPT 93-1.-Kharkov, KIPT, 1993. 19 p. (in Russian). ВОПРОСЫ АТОМНОЙ НАУКИ И ТЕХНИКИ. 1999. №3. Серия: Ядерно-физические исследования. (34), с. 47. 47 REFERENCES