| dc.contributor | Universidade Estadual Paulista (UNESP) | |
| dc.creator | Kassab, LRP | |
| dc.creator | Gouffon, P. | |
| dc.creator | Martins, M. N. | |
| dc.date | 2014-05-20T15:25:56Z | |
| dc.date | 2016-10-25T18:00:32Z | |
| dc.date | 2014-05-20T15:25:56Z | |
| dc.date | 2016-10-25T18:00:32Z | |
| dc.date | 1999-01-01 | |
| dc.date.accessioned | 2017-04-05T23:54:57Z | |
| dc.date.available | 2017-04-05T23:54:57Z | |
| dc.identifier | Particle Accelerators. Reading: Gordon Breach Sci Publ Ltd, v. 63, n. 1, p. 21-36, 1999. | |
| dc.identifier | 0031-2460 | |
| dc.identifier | http://hdl.handle.net/11449/36254 | |
| dc.identifier | http://acervodigital.unesp.br/handle/11449/36254 | |
| dc.identifier | WOS:000080164800002 | |
| dc.identifier | http://cds.cern.ch/record/1120321/files/p21.pdf | |
| dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/879815 | |
| dc.description | We will present measurements and calculations related to the antisymmetric perturbations, and comparisons with the symmetric ones, of the IFUSP race-track microtron booster accelerator end magnets. These perturbations were measured in planes situated at +/-12 mm of the middle plane, in a gap height of 4 cm, for a field distribution of about 0.1 T. The measurements were done in 1170 points, separated by a distance of 8 mm, using an automated system with a +/-1.5 mu T differential Hall probe. The race-track microtron booster is the second stage of the 30.0 MeV electron accelerator under construction at the Linear Accelerator Laboratory in which the required uniformity for the magnetic field is of about 10(-3). The method of correction employed to homogenize the IFUSP race-track microtron booster accelerator magnets assures uniformity of 10(-5) in an average field of 0.1 T, over an area of 700 cm(2). This method uses the principle of attaching to the pole pieces correction coils produced by etching techniques, with copper leads shaped like the isofield lines of the normal component of the magnetic field measured. The ideal planes, in which these measurements are done, are calculated and depend on the behavior of the magnetic field perturbations: symmetric or antisymmetric with reference to the middle plane of the magnet gap. These calculations are presented in this work and show that for antisymmetric perturbations there is no ideal plane for the correction of the magnetic field; for the symmetric one, these planes are at +/-60% of the half gap height, from the middle plane. So this method of correction is not feasible for antisymmetric perturbations, as will be shown. Besides, the correction of the symmetric portion of the field distribution does not influence the antisymmetric one, which almost does not change, and corroborates the theoretical predictions. We found antisymmetric perturbations of small intensity only in one of the two end magnets. However, they are not detected at +/- 1 mm of the middle plane and will not damage the electron beam. | |
| dc.language | eng | |
| dc.publisher | Gordon Breach Sci Publ Ltd | |
| dc.relation | Particle Accelerators | |
| dc.rights | info:eu-repo/semantics/closedAccess | |
| dc.subject | magnetic fields | |
| dc.subject | magnetic measurements | |
| dc.subject | magnets | |
| dc.subject | microtrons | |
| dc.title | The IFUSP race-track microtron booster accelerator end magnets antisymmetric perturbations | |
| dc.type | Otro | |
