Nonlinear optics from off-energy closed orbits

This paper describes a novel scheme for correcting the second order (chromatic sextupole) magnet lattice and its deployment on a fourth generation multibend achromat electron storage ring. The method is analogous to the well-established linear optics from closed orbits scheme, but uses an off-energy...

Full description

Bibliographic Details
Main Authors: David K. Olsson, Åke Andersson, Magnus Sjöström
Format: Article
Language:English
Published: American Physical Society 2020-10-01
Series:Physical Review Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevAccelBeams.23.102803
id doaj-c971c4de74484b9f9be3b734675204bf
record_format Article
spelling doaj-c971c4de74484b9f9be3b734675204bf2020-11-25T03:36:56ZengAmerican Physical SocietyPhysical Review Accelerators and Beams2469-98882020-10-01231010280310.1103/PhysRevAccelBeams.23.102803Nonlinear optics from off-energy closed orbitsDavid K. OlssonÅke AnderssonMagnus SjöströmThis paper describes a novel scheme for correcting the second order (chromatic sextupole) magnet lattice and its deployment on a fourth generation multibend achromat electron storage ring. The method is analogous to the well-established linear optics from closed orbits scheme, but uses an off-energy orbit response matrix to characterize the second order optics of a lattice. The matrix is constructed from the difference between two orbit response matrices measured at off-nominal energy, and is approximately linear with chromatic sextupole field strengths. This is utilized in a least squares minimization to find a model which minimizes the difference between the measured and model off-energy orbit response matrix. From this model corrections to the chromatic sextupoles of the machine can be calculated. In effect, for the MAX IV 3 GeV ring, the proposed scheme, NOECO (nonlinear optics from off-energy closed orbits), brings initial sextupole strength variations between achromats in the order of ±8% down to the order of ±1%. The chromatic machine functions were symmetrized, the measured chromaticities approached the nominal values, and the lifetime of the beam at delivery conditions, with the same level of emittance coupling, increased to 19 h from 11 h at previously used sextupole settings.http://doi.org/10.1103/PhysRevAccelBeams.23.102803
collection DOAJ
language English
format Article
sources DOAJ
author David K. Olsson
Åke Andersson
Magnus Sjöström
spellingShingle David K. Olsson
Åke Andersson
Magnus Sjöström
Nonlinear optics from off-energy closed orbits
Physical Review Accelerators and Beams
author_facet David K. Olsson
Åke Andersson
Magnus Sjöström
author_sort David K. Olsson
title Nonlinear optics from off-energy closed orbits
title_short Nonlinear optics from off-energy closed orbits
title_full Nonlinear optics from off-energy closed orbits
title_fullStr Nonlinear optics from off-energy closed orbits
title_full_unstemmed Nonlinear optics from off-energy closed orbits
title_sort nonlinear optics from off-energy closed orbits
publisher American Physical Society
series Physical Review Accelerators and Beams
issn 2469-9888
publishDate 2020-10-01
description This paper describes a novel scheme for correcting the second order (chromatic sextupole) magnet lattice and its deployment on a fourth generation multibend achromat electron storage ring. The method is analogous to the well-established linear optics from closed orbits scheme, but uses an off-energy orbit response matrix to characterize the second order optics of a lattice. The matrix is constructed from the difference between two orbit response matrices measured at off-nominal energy, and is approximately linear with chromatic sextupole field strengths. This is utilized in a least squares minimization to find a model which minimizes the difference between the measured and model off-energy orbit response matrix. From this model corrections to the chromatic sextupoles of the machine can be calculated. In effect, for the MAX IV 3 GeV ring, the proposed scheme, NOECO (nonlinear optics from off-energy closed orbits), brings initial sextupole strength variations between achromats in the order of ±8% down to the order of ±1%. The chromatic machine functions were symmetrized, the measured chromaticities approached the nominal values, and the lifetime of the beam at delivery conditions, with the same level of emittance coupling, increased to 19 h from 11 h at previously used sextupole settings.
url http://doi.org/10.1103/PhysRevAccelBeams.23.102803
work_keys_str_mv AT davidkolsson nonlinearopticsfromoffenergyclosedorbits
AT akeandersson nonlinearopticsfromoffenergyclosedorbits
AT magnussjostrom nonlinearopticsfromoffenergyclosedorbits
_version_ 1724548061478256640