R. Ostojic
CERN
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Featured researches published by R. Ostojic.
IEEE Transactions on Applied Superconductivity | 1997
A. Yamamoto; K. Tsuchiya; Norio Higashi; Tatsushi Nakamoto; T. Ogitsu; N. Ohuchi; T. Shintomi; A. Terashima; G. Kirby; R. Ostojic; T.M. Taylor
The conceptual design study of a high gradient superconducting insertion quadrupole magnet has been carried out in collaboration between KEK and CERN for the Large Hadron Collider (LHC) to be built at CERN. A model magnet design has been optimized to provide a nominal design field gradient of 240 T/m with a bore aperture of 70 mm and an operational field gradient of 225 T/m at 1.9 K under radiation environment with a deposition of several watts per meter in the superconducting coils. The design and its process are discussed.
IEEE Transactions on Magnetics | 1994
R. Ostojic; T.M. Taylor; G.A. Kirby
In order to achieve high field quality and low current rating of the 250 T/m quadrupoles for the LHC low-/spl beta/ insertions, a design based on a graded four-layer coil with an aperture of 70 mm, wound from NbTi conductor cooled at 1.8 K, has been proposed. Its mechanical structure is based on the collar-spacer concept, where a thin collar serves for coil assembly only. The iron yoke has both important magnetic and structural functions, since the magnetic forces are taken by the rigidity of the iron lamination pack. The coil and cable parameters are derived for this particular structure, and the results of the structural analysis of the magnet are presented. A one-metre model of the quadrupole is presently under construction; its features are described and some initial cable tests reported. >
IEEE Transactions on Applied Superconductivity | 2002
R. Ostojic
The Large Hadron Collider comprises eight insertions, four of which are dedicated to the LHC experiments while the others are used for the major collider systems. The various functions of the insertions are fulfilled by a variety of magnet systems, most of them based on the technology of NbTi superconductors cooled by superfluid helium at 1.9 K. A number of stand-alone magnets in the matching sections are operated at 4.5 K, while in the high radiation areas specialized resistive magnets are used. In this paper, we review the concepts underlying the design of the LHC insertions, and report on the design, procurement and testing of the various specialized magnet systems.
IEEE Transactions on Applied Superconductivity | 2004
R. Ostojic
The LHC comprises eight insertions, four of which are dedicated to the experiments while the others are used for major collider systems. The various functions of the insertions are fulfilled by a variety of magnet systems, most of them based on the technology of NbTi superconductors cooled by superfluid helium at 1.9 K. In this paper, we review the concepts underlying the design of the LHC insertions, and describe the corresponding design of the various specialized magnet systems. A status of the procurement of the magnets is given, and plans for their installation and commissioning reviewed.
IEEE Transactions on Applied Superconductivity | 2014
M. L. Lopes; Giorgio Ambrosio; M. Buehler; R. Coleman; D. Evbota; S. Feher; V.V. Kashikhin; M.J. Lamm; J. P. Miller; G. Moretti; R. Ostojic; T. Page; J. Popp; M. Tartaglia
The muon-to-electron conversion experiment at Fermilab is designed to explore charged lepton flavor violation. It is composed of three large superconducting solenoids, namely, the production solenoid, the transport solenoid, and the detector solenoid. Each subsystem has a set of field requirements. Tolerance sensitivity studies of the magnet system were performed with the objective of demonstrating that the present magnet design meets all the field requirements. Systematic and random errors were considered on the position and alignment of the coils. The study helps to identify the critical sources of errors and which are translated to coil manufacturing and mechanical support tolerances.
IEEE Transactions on Applied Superconductivity | 2014
S. Feher; N. Andreev; J. Brandt; Sergey Cheban; R. Coleman; N. Dhanaraj; I. Fang; M.J. Lamm; V. Lombardo; M. L. Lopes; J. P. Miller; R. Ostojic; D. Orris; T. Page; T. Peterson; Z. Tang; R. Wands
The Mu2e experiment at Fermilab has been approved by the Department of Energy to proceed with the development of the preliminary design. Integral to the success of Mu2e is the superconducting solenoid system. One of the three major solenoids is the detector solenoid that houses the stopping target and the detectors. The goal of the detector solenoid team is to produce detailed design specifications that are sufficient for vendors to produce the final design drawings, tooling and fabrication procedures and proceed to production. In this paper we summarize the reference design of the detector solenoid.
IEEE Transactions on Applied Superconductivity | 1999
Tatsushi Nakamoto; K. Tanaka; Akira Yamamoto; K. Tsuchiya; E. Barkhardt; Norio Higashi; N. Kimura; T. Ogitsu; N. Ohuchi; K. Sasaki; T. Shintomi; A. Terashima; G. Kirby; R. Ostojic; T.M. Taylor
A one meter model of the high gradient 70 mm aperture superconducting low-/spl beta/ quadrupole has been developed at KEK. The design field gradient is 240 T/m at a current 7677 A with a superconducting load line ratio of 92% and peak field of 9.64 T in the coil. A first series of training tests of the magnet was carried out at 1.9 K including a full thermal cycle to room temperature. The highest quench current was 8007 A corresponding to a field gradient of 250 T/m. The magnet was subsequently reassembled to improve its longitudinal mechanical structure. In this paper, quench characteristics and mechanical behavior of the first model magnet are presented.
IEEE Transactions on Applied Superconductivity | 1993
R. Ostojic; T.M. Taylor
Due to their detrimental effect on the Large Hadron Collider (LHC) dynamic aperture, the random multipole errors of the LHC insertion quadrupoles need to be lower by a factor of five than the corresponding errors in the lattice. For achieving this level of random errors, the authors propose to increase the aperture of the insertion quadrupoles. A novel approach for achieving a quadrupole strength of 250 T/m in an aperture of 70 mm, based on a graded multilayer coil wound from NbTi conductor cooled at 1.8 K, has been investigated. The design concept of the coil, which incorporates a shell-like structure composed of a high current density block imbedded in a low density shell, is developed. The coil design, parameters of the superconducting cable, and the yoke and collar design are described, both for a two-in-one and a single quadrupole geometries.<<ETX>>
IEEE Transactions on Applied Superconductivity | 2001
J. Lucas; R. Ostojic; L. Bottura; R. Bussjaeger; H. Dariol; A. Hobl; D. Krischel; G. Kirby; V. Remondino; S. Sanfilippo; M. Schillo; A. Siemko; F. Sonnemann; D. Tommasini; I. Vanenkov; W. Venturini Delsolaro
The LHC dispersion suppressors and matching sections will be equipped with individually powered superconducting quadrupoles with an aperture of 56 mm. In order to optimise the parameters and cost of the magnets and of their powering, the quadrupole has been designed on the basis of an 8.2 mm wide Rutherford-type cable for a nominal current of 5300 A, corresponding to a gradient of 200 T/m at 1.9 K. In order to validate the design two 1-m single-aperture quadrupoles and one twin-aperture quadrupole have been built and tested. In this report we describe the construction features of the magnets and present the results of the magnet tests.
IEEE Transactions on Applied Superconductivity | 2000
G. Kirby; J. Lucas; R. Ostojic; F. Rodriguez-Mateos; D. Krischel; M. Schillo
About one hundred individually powered low current superconducting quadrupoles will be installed in the LHC insertions. One of the design requirements was to keep the excitation current of the magnet below 6 kA in view of minimizing the costs of the powering circuits. The design of the quadrupole is based on a 8.2 mm NbTi cable, and is designed for a nominal gradient of 200 T/m at 1.9 K. In this paper we present the design of the quadrupole and discuss the construction details of the 1 m single aperture model which has been recently completed.