000625584 001__ 625584
000625584 005__ 20250328221321.0
000625584 020__ $$a978-3-95450-231-8
000625584 0247_ $$2doi$$a10.18429/JACoW-IPAC2023-WEPM100
000625584 0247_ $$2INSPIRETeX$$aGehlot:2023reu
000625584 0247_ $$2inspire$$ainspire:2717302
000625584 0247_ $$2datacite_doi$$a10.3204/PUBDB-2025-01137
000625584 037__ $$aPUBDB-2025-01137
000625584 041__ $$aEnglish
000625584 1001_ $$0P:(DE-H253)PIP1102383$$aGehlot, Mona$$b0$$eCorresponding author
000625584 1112_ $$a14th International Particle Accelerator Conference$$cVenice$$d2023-05-07 - 2023-05-12$$gIPAC'23$$wItaly
000625584 245__ $$aDesign of permanent magnet dipoles-quadrupoles with longitudinal gradient for the PETRA IV storage ring
000625584 260__ $$a[Geneva]$$bJACoW Publishing$$c2023
000625584 29510 $$a[Ebook] IPAC'23 : 14th International Particle Accelerator Conference, 7-12 May 2023, Venice, Italy : proceedings / hosting institutions: INFN, Elettra Sincotrone Trieste , [Geneva] : JACoW Publishing, [2023],
000625584 300__ $$a3798 - 3800
000625584 3367_ $$2ORCID$$aCONFERENCE_PAPER
000625584 3367_ $$033$$2EndNote$$aConference Paper
000625584 3367_ $$2BibTeX$$aINPROCEEDINGS
000625584 3367_ $$2DRIVER$$aconferenceObject
000625584 3367_ $$2DataCite$$aOutput Types/Conference Paper
000625584 3367_ $$0PUB:(DE-HGF)8$$2PUB:(DE-HGF)$$aContribution to a conference proceedings$$bcontrib$$mcontrib$$s1743155925_731526
000625584 3367_ $$0PUB:(DE-HGF)7$$2PUB:(DE-HGF)$$aContribution to a book$$mcontb
000625584 500__ $$aLiteraturangaben;
000625584 520__ $$aThe PETRA IV storage ring is a project planned to upgrade the synchrotron light source PETRA III at DESY. The main aim is to decrease the horizontal emittance as low as 20 pmrad. This nominal emittance will be achieved by a hybrid six bend achromat lattice (H6BA) and a series of damping wigglers. The magnets used in this lattice will be a combination of resistive quadrupole and higher multipole magnets and permanent dipole magnets.Three different types of permanent combined-function dipole-quadrupole magnets are presently developed, including one with an additional longitudinal gradient. The design structure is a further advancement of the well-proven ESRF-EBS dipoles with longitudinal gradient. Due to its moderate value, the transverse gradient can be implemented by a slanted pole design. This contribution presents the design status of these novel magnets, discusses the expected magnetic field characteristics, and outlines the mechanical design for a prototype.
000625584 536__ $$0G:(DE-HGF)POF4-621$$a621 - Accelerator Research and Development (POF4-621)$$cPOF4-621$$fPOF IV$$x0
000625584 588__ $$aDataset connected to DataCite, INSPIRE
000625584 650_7 $$2Other$$aAccelerator Physics
000625584 650_7 $$2Other$$amc7-accelerator-technology-and-sustainability - MC7: Accelerator Technology and Sustainability
000625584 650_7 $$2Other$$amc7-t34-permanent-magnets - MC7.T34: Permanent Magnets
000625584 650_7 $$2autogen$$adipole
000625584 650_7 $$2autogen$$alattice
000625584 650_7 $$2autogen$$aquadrupole
000625584 650_7 $$2autogen$$asimulation
000625584 650_7 $$2autogen$$aoperation
000625584 650_7 $$2autogen$$aacceleration
000625584 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000625584 7001_ $$0P:(DE-H253)PIP1095027$$aN'gotta, Patrick$$b1
000625584 7001_ $$0P:(DE-H253)PIP1004486$$aRamm, Torsten$$b2
000625584 7001_ $$0P:(DE-H253)PIP1001383$$aTischer, Markus$$b3
000625584 7001_ $$0P:(DE-H253)PIP1113578$$aChavanne, Joel$$b4
000625584 773__ $$a10.18429/JACoW-IPAC2023-WEPM100
000625584 8564_ $$uhttps://bib-pubdb1.desy.de/record/625584/files/WEPM100.pdf$$yOpenAccess
000625584 8564_ $$uhttps://bib-pubdb1.desy.de/record/625584/files/WEPM100.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000625584 909CO $$ooai:bib-pubdb1.desy.de:625584$$popenaire$$popen_access$$pVDB$$pdriver$$pdnbdelivery
000625584 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1102383$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000625584 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1095027$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
000625584 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1004486$$aDeutsches Elektronen-Synchrotron$$b2$$kDESY
000625584 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1001383$$aDeutsches Elektronen-Synchrotron$$b3$$kDESY
000625584 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1113578$$aExternal Institute$$b4$$kExtern
000625584 9131_ $$0G:(DE-HGF)POF4-621$$1G:(DE-HGF)POF4-620$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vAccelerator Research and Development$$x0
000625584 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000625584 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000625584 9201_ $$0I:(DE-H253)FS-US-20120731$$kFS-US$$lFS-Undulator Systeme$$x0
000625584 9201_ $$0I:(DE-H253)ZM1-20120731$$kZM1$$lKonstruktion$$x1
000625584 980__ $$acontrib
000625584 980__ $$aVDB
000625584 980__ $$aUNRESTRICTED
000625584 980__ $$acontb
000625584 980__ $$aI:(DE-H253)FS-US-20120731
000625584 980__ $$aI:(DE-H253)ZM1-20120731
000625584 9801_ $$aFullTexts