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\newacronym{linac}{LINAC}{Linear Accelerator}
\newacronym{cnpem}{CNPEM}{Brazilian Center for Research in Energy and Materials}
\newacronym{lnls}{LNLS}{Brazilian Synchrotron Light Laboratory}
\newacronym{3gls}{3$^\text{rd}$ GLS}{Third Generation Light Sources}
\newacronym{4gls}{4$^\text{th}$ GLS}{Fourth Generation Light Sources}
\newacronym{esrf}{ESRF}{European Synchrotron Radiation Facility}
\newacronym{mba}{MBA}{Multi-Bend-Achromat}
\newacronym{sofb}{SOFB}{Slow Orbit Feedback System}
\newacronym{fofb}{FOFB}{Fast Orbit Feedback System}
\newacronym{rms}{rms}{root-mean-square}
\newacronym{ie}{IE}{Injection Efficiency}
\newacronym{loco}{LOCO}{Linear Optics from Closed Orbits}
\newacronym{std}{std}{standard deviation}
\newacronym{svd}{SVD}{Singular Value Decomposition}
\newacronym{bba}{BBA}{Beam-Based Alignment}
\newacronym{rf}{RF}{radio-frequency}
\newacronym{DA}{DA}{Dynamic Aperture}
\newacronym{tbt}{TbT}{Turn-by-Turn}
\newacronym{pca}{PCA}{Principal Component Analysis}
\newacronym{nlk}{NLK}{nonlinear kicker}
\newacronym{dpk}{DipK}{dipolar kicker}
\newacronym{RCDS}{RCDS}{Robust Conjugate Direction Search}
\newacronym{sr}{SR}{Synchrotron radiation}
\newacronym{desy}{DESY}{Deutsches Elektronen-Synchrotron}
\newacronym{doris}{DORIS}{Double-Ring Storage Facility}
\newacronym{ada}{ADA}{Anello Di Accumulazione}
\newacronym{bessy}{BESSY}{Berliner Elektronenspeicherring-Gesellschaft für Synchrotronstrahlung}
\newacronym{elsa}{ELSA}{Electron Stretcher Accelerator}
\newglossaryentry{SuperACO}
{
name={SuperACO},
description={$800~\unit{MeV}$ positron accelerator at \acrshort*{lure}}
}
\newacronym{lure}{LURE}{Laboratorie pour l'Utilisation du Rayonnement Electromagnétique}
\newacronym{nsls}{NSLS}{National Synchrotron Light Source}
\newacronym{spear}{SPEAR}{Stanford Positron Electron Accelerating Ring}
\newglossaryentry{kek}
{
name={KEK},
description={Japanese High Energy Accelerator Research Organization}
}
\newglossaryentry{SOR-Ring}
{
name={SOR-Ring},
description={$300~\unit{M eV}$ spectroscopy-dedicated synchrotron radiation source in the Institute for Nuclear Study of the University of Tokyo}
}
\newglossaryentry{alba}
{
name={ALBA},
description={"Sunrise" in Catalan and in Spanish. A third-generation synchrotron light source facility in the Barcelona Synchrotron Park in Cerdanyola del Vallès, near Barcelona}
}
\newacronym{soleil}{SOLEIL}{Source Optimisée de Lumière d´Energie Intermédiaire du LURE}
\newacronym{ESRF}{ESRF}{European Synchrotron Radiation Facility}
\newglossaryentry{ELETTRA}
{
name={ELETTRA},
description={Third-generation electron storage ring of the Elettra Sincrotrone Trieste research center, in Trieste, Italy}
}
\newacronym{APS}{APS}{Advanced Photon Source}
\newacronym{ALS}{ALS}{Advanced Light Source}
\newglossaryentry{UVX}
{
name={UVX},
description={LNLS' first synchrotron light-source, based on a second-generation $1.37\unit{G eV}$ storage ring}
}
\newglossaryentry{orm}
{
name={ORM},
description={Orbit Response Matrix},
first={\glsentrydesc{orm} (\glsentrytext{orm})},
plural={ORMs},
descriptionplural={Orbit Response Matrices},
firstplural={\glsentrydescplural{orm} (\glsentryplural{rom})}
}
\newacronym{AS}{AS}{Australian Synchrotron}
\newacronym{CLS}{CLS}{Canadian Light Source}
\newacronym{TPS}{TPS}{Taiwan Photon Source}
\newacronym{PLS}{PLS}{Pohang Light Source}
\newacronym{Spring-8}{Spring-8}{Super Photon ring-8 GeV}
\newacronym{SSRF}{SSRF}{Shanghai Synchrotron Radiation Facility}
\newacronym{bpm}{BPM}{Beam Position Monitor}
\newacronym{id}{ID}{insertion device}
\newacronym{4gsr}{4GSR}{4{th} generation storage ring}
\newacronym{5ba}{5BA}{five-bend-achromat}
\newacronym{dcct}{DCCT}{Direct-Current Current Transformer}
\newacronym{ICT}{ICT}{Integrated Current Transformer}
\newglossaryentry{WP1}{
name={WP1},
description={Machine Working Point 1, with tunes $(\nu_x, \nu_y)=(49.08, 14.14)$}
}
\newglossaryentry{WP2}{
name={WP2},
description={Machine Working Point 2, with tunes $(\nu_x, \nu_y)=(49.20, 14.25)$}
}
\newglossaryentry{WP3}{
name={WP3},
description={Machine Working Point 3, with tunes $(\nu_x, \nu_y)=(49.16, 14.22)$}
}