A good field quality is always requested to achieve for the low- beta quadrupole magnet being used in the accelerator projects. To meet the requirement, people are always managing to reduce the field errors from its magnetic design and construction. In order to obtain a basic understanding for various known multipolar field errors, some calculation evaluations have been performed. Based on the results, the possible origins and corresponding correction methods of the deviation were briefly discussed in the paper. (6 refs)
Two 1-m model magnets for the LHC low- beta quadrupoles were constructed and tested in KEK. They wer...
The dynamic aperture of LHC in collision is determined by the multipole field errors of the low-beta...
The Fermilab Main Injector ramps from 8 GeV to 120 GeV in about half a second. The rapidly changing ...
The magnetic field of superconducting accelerator magnets is mainly determined by the current distri...
The U.S. large hadron collider (LHC) Accelerator Research Program, in close collaboration with The E...
Fermilab, Lawrence Berkeley National Laboratory and Brookhaven National Laboratory have formed a con...
The first two short models of the MQXB quadrupole magnets for the LHC interaction regions have been ...
As part of the collaboration program between CERN and KEK for the LHC, we have been developing a hig...
Fermilab, Lawrence Berkeley National Laboratory and Brookhaven National Laboratory have formed a con...
Mathematical foundations of field computation and magnetic measurements for accelerator magnets Mag...
The paper describes the recent efforts in establishing a consistent basis for beam physics simulatio...
Estimates of random field-shape errors induced by cable mispositioning in superconducting magnets ar...
Abstract—The inner triplet quadrupole magnets (MQXA) for the LHC low-beta insertion have been develo...
A group of codes has been developed using a new method for designing the pole profile of a quadrupol...
Today's best magnetic materials show almost analytic behavior. This is used here todevelop a formali...
Two 1-m model magnets for the LHC low- beta quadrupoles were constructed and tested in KEK. They wer...
The dynamic aperture of LHC in collision is determined by the multipole field errors of the low-beta...
The Fermilab Main Injector ramps from 8 GeV to 120 GeV in about half a second. The rapidly changing ...
The magnetic field of superconducting accelerator magnets is mainly determined by the current distri...
The U.S. large hadron collider (LHC) Accelerator Research Program, in close collaboration with The E...
Fermilab, Lawrence Berkeley National Laboratory and Brookhaven National Laboratory have formed a con...
The first two short models of the MQXB quadrupole magnets for the LHC interaction regions have been ...
As part of the collaboration program between CERN and KEK for the LHC, we have been developing a hig...
Fermilab, Lawrence Berkeley National Laboratory and Brookhaven National Laboratory have formed a con...
Mathematical foundations of field computation and magnetic measurements for accelerator magnets Mag...
The paper describes the recent efforts in establishing a consistent basis for beam physics simulatio...
Estimates of random field-shape errors induced by cable mispositioning in superconducting magnets ar...
Abstract—The inner triplet quadrupole magnets (MQXA) for the LHC low-beta insertion have been develo...
A group of codes has been developed using a new method for designing the pole profile of a quadrupol...
Today's best magnetic materials show almost analytic behavior. This is used here todevelop a formali...
Two 1-m model magnets for the LHC low- beta quadrupoles were constructed and tested in KEK. They wer...
The dynamic aperture of LHC in collision is determined by the multipole field errors of the low-beta...
The Fermilab Main Injector ramps from 8 GeV to 120 GeV in about half a second. The rapidly changing ...