An interactive procedure of a transverse beam matching and correction in INR Linac

An application package is developed to carry out an interactive procedure for a transverse beam matching and correction in INR Linac. The results of multiple beam profile measurements in several accelerator areas are used. The currents in steering coils are found to suppress the beam displacement....

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Datum:2006
Hauptverfasser: Bragin, S.E., Feschenko, A.V., Grekhov, O.V., Lebedeva, N.F., Mikhailov, V.N., Mirzojan, A.N., Moiseev, V.A., Volodkevich, O.M.
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Veröffentlicht: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2006
Schriftenreihe:Вопросы атомной науки и техники
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Online Zugang:http://dspace.nbuv.gov.ua/handle/123456789/79862
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Zitieren:An interactive procedure of a transverse beam matching and correction in INR Linac / S.E. Bragin, A.V. Feschenko, O.V. Grekhov, N.F. Lebedeva, V.N. Mikhailov, A.N. Mirzojan, V.A. Moiseev, O.M. Volodkevich // Вопросы атомной науки и техники. — 2006. — № 3. — С. 116-118. — Бібліогр.: 2 назв. — англ.

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spelling irk-123456789-798622015-04-06T03:01:55Z An interactive procedure of a transverse beam matching and correction in INR Linac Bragin, S.E. Feschenko, A.V. Grekhov, O.V. Lebedeva, N.F. Mikhailov, V.N. Mirzojan, A.N. Moiseev, V.A. Volodkevich, O.M. Ускорители заряженных частиц An application package is developed to carry out an interactive procedure for a transverse beam matching and correction in INR Linac. The results of multiple beam profile measurements in several accelerator areas are used. The currents in steering coils are found to suppress the beam displacement. The gradients in quadrupole lenses are calculated to match the beam. This procedure is successfully used in accelerator tuning. Разработан пакет программ для проведения интерактивной процедуры поперечного согласования и коррекции пучка по результатам измерения профилей пучка на различных участках линейного ускорителя ИЯИ РАН. Определяются режимы включения корректирующих элементов для выведения пучка на ось ускорителя и градиенты полей квадрупольных линз для согласования пучка с фокусирующим каналом ускорителя. Разработанная процедура успешно используется при настройке режимов работы ускорителя. Розроблено пакет програм для проведення інтерактивної процедури поперечного узгодження і корекції пучка за результатами виміру профілів пучка на різних ділянках лінійного прискорювача ІЯД РАН. Визначаються режими включення коригувальних елементів для виведення пучка на вісь прискорювача і градієнти полів квадрупольних лінз для узгодження пучка з фокусуючим каналом прискорювача. Розроблена процедура успішно використається при настроюванні режимів роботи прискорювача. 2006 Article An interactive procedure of a transverse beam matching and correction in INR Linac / S.E. Bragin, A.V. Feschenko, O.V. Grekhov, N.F. Lebedeva, V.N. Mikhailov, A.N. Mirzojan, V.A. Moiseev, O.M. Volodkevich // Вопросы атомной науки и техники. — 2006. — № 3. — С. 116-118. — Бібліогр.: 2 назв. — англ. 1562-6016 PACS: 29.27.Eg http://dspace.nbuv.gov.ua/handle/123456789/79862 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
topic Ускорители заряженных частиц
Ускорители заряженных частиц
spellingShingle Ускорители заряженных частиц
Ускорители заряженных частиц
Bragin, S.E.
Feschenko, A.V.
Grekhov, O.V.
Lebedeva, N.F.
Mikhailov, V.N.
Mirzojan, A.N.
Moiseev, V.A.
Volodkevich, O.M.
An interactive procedure of a transverse beam matching and correction in INR Linac
Вопросы атомной науки и техники
description An application package is developed to carry out an interactive procedure for a transverse beam matching and correction in INR Linac. The results of multiple beam profile measurements in several accelerator areas are used. The currents in steering coils are found to suppress the beam displacement. The gradients in quadrupole lenses are calculated to match the beam. This procedure is successfully used in accelerator tuning.
format Article
author Bragin, S.E.
Feschenko, A.V.
Grekhov, O.V.
Lebedeva, N.F.
Mikhailov, V.N.
Mirzojan, A.N.
Moiseev, V.A.
Volodkevich, O.M.
author_facet Bragin, S.E.
Feschenko, A.V.
Grekhov, O.V.
Lebedeva, N.F.
Mikhailov, V.N.
Mirzojan, A.N.
Moiseev, V.A.
Volodkevich, O.M.
author_sort Bragin, S.E.
title An interactive procedure of a transverse beam matching and correction in INR Linac
title_short An interactive procedure of a transverse beam matching and correction in INR Linac
title_full An interactive procedure of a transverse beam matching and correction in INR Linac
title_fullStr An interactive procedure of a transverse beam matching and correction in INR Linac
title_full_unstemmed An interactive procedure of a transverse beam matching and correction in INR Linac
title_sort interactive procedure of a transverse beam matching and correction in inr linac
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
publishDate 2006
topic_facet Ускорители заряженных частиц
url http://dspace.nbuv.gov.ua/handle/123456789/79862
citation_txt An interactive procedure of a transverse beam matching and correction in INR Linac / S.E. Bragin, A.V. Feschenko, O.V. Grekhov, N.F. Lebedeva, V.N. Mikhailov, A.N. Mirzojan, V.A. Moiseev, O.M. Volodkevich // Вопросы атомной науки и техники. — 2006. — № 3. — С. 116-118. — Бібліогр.: 2 назв. — англ.
series Вопросы атомной науки и техники
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fulltext AN INTERACTIVE PROCEDURE OF A TRANSVERSE BEAM MATCH- ING AND CORRECTION IN INR LINAC S.E. Bragin, A.V. Feschenko, O.V. Grekhov, N.F. Lebedeva, V.N. Mikhailov, A.N. Mirzojan, V.A. Moiseev, O.M. Volodkevich Institute for Nuclear Research of the Russian Academy of Sciences, Moscow, Russia E-mail: bragin@inr.ru An application package is developed to carry out an interactive procedure for a transverse beam matching and correction in INR Linac. The results of multiple beam profile measurements in several accelerator areas are used. The currents in steering coils are found to suppress the beam displacement. The gradients in quadrupole lenses are calculated to match the beam. This procedure is successfully used in accelerator tuning. PACS: 29.27.Eg 1. INTRODUCTION The Linac of Institute for Nuclear Research of the Russian Academy of Sciences (INR) is a high intensity accelerator [1]. Therefore, it is important to achieve op- timal beam transportation throughout the accelerator with minimum beam losses. There are five areas in the high energy accelerator part (above 100 MeV) where the measurements are done to observe and to adjust beam characteristics. 2. INSTRUMENTATION Transverse behavior of the beam is monitored by wire scanners. From three to five wire scanners are in- stalled in each measuring area of the accelerator. The scanner consists of two perpendicular wires, which are parallel to horizontal and vertical axes. The two-wire as- sembly is moved across the beam by a step motor. Scan- ning is made through the whole accelerator channel aperture in the range of ±20 mm. A scan step is set by an operator and can be equal to 0.5, 1 or 2 mm. The du- ration of measuring cycle depends on a number of scan- ners used and is about 10…15 minutes. Processing of experimental profiles (Fig.1) gives rms size of the beam and position of the beam centre for both transverse planes. These data along with information on focusing structure of the measuring area are further used for data treatment. Fig.1. Example of beam profile measurement 3. TREATMENT OF PROFILE MEASURE- MENTS The results of rms beam size and the beam centre measurements in the point of wire scanner longitudinal location for each phase plane represent vertical lines. The disposition of these lines can be transferred to an arbitrary point of measuring area by a matrix transfor- mation. The results of measurements with several scanners transferred to a selected position represent a set of lines. The phase ellipse is inscribed with the iteration algo- rithm in central part of the phase space separated by the lines, the sum of distances for all the lines to the ellipse being minimized (Fig.2). The parameters of phase ellipses αx, βx, γx, αy, βy, γy and the emittances εx and εy are calculated in rms mean- ing for any point of interest. Below the results of treat- ment of measurements are presented for a 100 MeV INR Linac measuring area. Fig.2. The inscribed beam phase ellipses related to the entrance of the measuring area at 100 MeV region ____________________________________________________________ PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY. 2006. № 3. Series: Nuclear Physics Investigations (47), p.116-118.116 The method mentioned above has computational er- rors in determination of the ellipse parameters which de- pend on mutual disposition of the lines. To decrease these errors, a procedure is carried out for several points along the measuring area. Then the parameters of all the ellipses are transformed to the point of interest by the matrix transformation and the mean values of the pa- rameters are calculated. For example, the parameters at the entrance of the 100 MeV measuring area are the fol- lowing: βx =1.01±0.03 mm/mrad; βy =1.48±0.04 mm/mrad; αx =-1.22±0.04; αy =0.24±0.04; εx=0.63±0.01 mm⋅mrad; εy =0.66±0.01 mm⋅mrad The errors shown represent procedural errors of the method and are only the part of the total errors. Similarly one can get a series of transformed straight lines for a beam centre. Ideally, an intersection point of these lines is a beam centre in a phase space. Normally, due to errors, all the lines do not intersect in one point, so the point of beam centre is found by minimizing the sum of distances to all the lines (Fig.3). Similarly to the procedural errors for ellipse parameters there are proce- dural errors for centre determination and the values re- lated to Fig.3 are: Xcentre= -0.13±0.17 mm; Ycentre=0.50±0.14 mm; X′centre= -0.16±0.31 mrad; Y′centre=-0.80±0.18 mrad Fig.3. Determination of the beam centre for the en- trance of the measuring area at 100 MeV region Fig.4. Lattice (a) and tracing of the β -function before (b) and after (c) matching procedure Fig.5. Tracing of the beam centre before and after correction (first step of procedure) 4. MATCHING PROCEDURE Reconstruction of transverse beam phase ellipses and determination of the beam centers in an arbitrary longitudinal point is necessary for the subsequent proce- dure of beam matching and correction. The elements of focusing structure and wire scanners for 100 MeV mea- suring area are shown in Fig.4,a. The tracing of the found phase space ellipse parameters along the measur- ing area is presented in Fig.4,b. To minimize the beam size, a specially developed matching algorithm is used. The gradients in the first four quadrupoles (for 100 MeV area) or quadrupole doublet assemblies (for other measuring areas) are varied to match the entrance beam parameters found by the method mentioned above with the downstream accelerator structure. After ____________________________________________________________ PROBLEMS OF ATOMIC SCIENCE AND TECHNOLOGY. 2006. № 3. Series: Nuclear Physics Investigations (47), p.116-118.117 selection and setting the values of gradients the profile measurements are repeated. Fig.4,c shows a behavior of the beam after proper matching. Sometimes the match- ing procedure must be iterated several times for better results. 5. BEAM CENTRE CORRECTION There are additional windings in the quadrupoles to produce an additional dipole field for beam steering. Two steering elements for each plane are used in each measuring area. A standard correction procedure [2] en- ables to suppress displacement and angle of the beam at the exit of the second steering element in both horizon- tal and vertical planes. The correction procedure is carried out after comple- tion of the procedure of beam matching. The steering currents are calculated with a separate code. Fig.5 demonstrates a behavior of beam centre throughout the measuring area before and after correc- tion. To estimate the correction efficiency a special pa- rameter was introduced. It is determined as an rms devi- ation of the beam centre from the ideal axis averaged over the measuring area. Fig.5 demonstrates an im- provement of beam behavior after the first step of cor- rection. The parameters defined above are Xcen- rms=0.95 mm, Ycenrms=1.81 mm before correction and Xcenrms=0.87 mm, Ycenrms=0.70 mm after correction. To improve the accuracy several iterations are required though further studies are necessary. 6. CONCLUSION All the algorithms mentioned above are included to the application package. The method has been tested at a 100 MeV region and is planned to use in all the mea- suring areas of INR Linac. This application package is developed for interactive analysis and control of trans- verse beam parameters. Effective beam matching and correction are achieved in the first experiment. REFERENCES 1. B.P. Murin et al. Ion Linear Accelerators. M.: «At- omizdat», 1978. 2. I.N. Biryukov, A.N.Mirzojan et al. Investigation of Transverse Beam Dynamics at the INR Linac. INR Report, 1991. ИНТЕРАКТИВНАЯ ПРОЦЕДУРА ПОПЕРЕЧНОГО СОГЛАСОВАНИЯ И КОРРЕКЦИИ ПУЧКА НА ЛИНЕЙНОМ УСКОРИТЕЛЕ ИЯИ РАН С.Е. Брагин, А.В. Фещенко, О.В. Грехов, Н.Ф. Лебедева, В.Н. Михайлов, А.Н. Мирзоян, В.А. Моисеев, О.М. Володкевич Разработан пакет программ для проведения интерактивной процедуры поперечного согласования и кор- рекции пучка по результатам измерения профилей пучка на различных участках линейного ускорителя ИЯИ РАН. Определяются режимы включения корректирующих элементов для выведения пучка на ось ускорите- ля и градиенты полей квадрупольных линз для согласования пучка с фокусирующим каналом ускорителя. Разработанная процедура успешно используется при настройке режимов работы ускорителя. ІНТЕРАКТИВНА ПРОЦЕДУРА ПОПЕРЕЧНОГО УЗГОДЖЕННЯ І КОРЕКЦІЇ ПУЧКА НА ЛІНІЙНОМУ ПРИСКОРЮВАЧІ ІЯД РАН С.Є. Брагін, А.В. Фещенко, О.В. Грєхов, Н.Ф. Лебедева, В.Н. Міхайлов, А.Н. Мірзоян, В.А. Моисєєв, О.М. Володкевич Розроблено пакет програм для проведення інтерактивної процедури поперечного узгодження і корекції пучка за результатами виміру профілів пучка на різних ділянках лінійного прискорювача ІЯД РАН. Визначаються режими включення коригувальних елементів для виведення пучка на вісь прискорювача і градієнти полів квадрупольних лінз для узгодження пучка з фокусуючим каналом прискорювача. Розроблена процедура успішно використається при настроюванні режимів роботи прискорювача. 118 Интерактивная процедура поперечного согласования и коррекции пучка на линейном ускорителе ИЯИ РАН ІНТЕРАКТИВНА ПРОЦЕДУРА ПОПЕРЕЧНОГО УЗГОДЖЕННЯ І КОРЕКЦІЇ ПУЧКА НА ЛІНІЙНОМУ ПРИСКОРЮВАЧІ ІЯД РАН