FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W4226164754> ?p ?o ?g. }

• W4226164754 abstract "For some synchrotron light source beamline applications, a round beam is preferable to a flat one. A conventional method of obtaining round beam in an electron storage ring is to shift its tune close to a linear difference resonance. The linearly coupled beam dynamics is analyzed with perturbation theories, which have certain limitations. In this paper, we adopt the Solution by LInear Matrices (SLIM) analysis to calculate exact beam sizes to design round beam lattices. The SLIM analysis can deal with a generally linearly coupled accelerator lattice. The effects of various coupling sources on beam emittances and sizes can be studied within a self-consistent frame. Both the on- and off-resonance schemes to obtain round beams are explained with examples. The SLIM formalism for two widely used magnet models: combined-function bending magnets, and planar wigglers and undulators, is also derived." @default.
• W4226164754 created "2022-05-05" @default.
• W4226164754 creator A5033463275 @default.
• W4226164754 creator A5041801417 @default.
• W4226164754 date "2022-04-21" @default.
• W4226164754 modified "2023-10-17" @default.
• W4226164754 title "Designing linear lattices for round beam in electron storage rings using the solution by linear matrices analysis" @default.
• W4226164754 cites W1969363675 @default.
• W4226164754 cites W1980630290 @default.
• W4226164754 cites W1983103920 @default.
• W4226164754 cites W1988374183 @default.
• W4226164754 cites W1991167392 @default.
• W4226164754 cites W2013729931 @default.
• W4226164754 cites W2020886704 @default.
• W4226164754 cites W2032705227 @default.
• W4226164754 cites W2037630267 @default.
• W4226164754 cites W2067634029 @default.
• W4226164754 cites W2069324604 @default.
• W4226164754 cites W2075265848 @default.
• W4226164754 cites W2076398340 @default.
• W4226164754 cites W2115278974 @default.
• W4226164754 cites W2133292567 @default.
• W4226164754 cites W2152527765 @default.
• W4226164754 cites W2163257413 @default.
• W4226164754 cites W2217051974 @default.
• W4226164754 cites W3102090394 @default.
• W4226164754 cites W3120108967 @default.
• W4226164754 cites W3200571729 @default.
• W4226164754 doi "https://doi.org/10.1103/physrevaccelbeams.25.040702" @default.
• W4226164754 hasPublicationYear "2022" @default.
• W4226164754 type Work @default.
• W4226164754 citedByCount "2" @default.
• W4226164754 countsByYear W42261647542023 @default.
• W4226164754 crossrefType "journal-article" @default.
• W4226164754 hasAuthorship W4226164754A5033463275 @default.
• W4226164754 hasAuthorship W4226164754A5041801417 @default.
• W4226164754 hasBestOaLocation W42261647541 @default.
• W4226164754 hasConcept C120665830 @default.
• W4226164754 hasConcept C121332964 @default.
• W4226164754 hasConcept C121684516 @default.
• W4226164754 hasConcept C134786449 @default.
• W4226164754 hasConcept C136959337 @default.
• W4226164754 hasConcept C142362112 @default.
• W4226164754 hasConcept C147120987 @default.
• W4226164754 hasConcept C153349607 @default.
• W4226164754 hasConcept C16332341 @default.
• W4226164754 hasConcept C16389437 @default.
• W4226164754 hasConcept C168834538 @default.
• W4226164754 hasConcept C180048950 @default.
• W4226164754 hasConcept C189166818 @default.
• W4226164754 hasConcept C21368211 @default.
• W4226164754 hasConcept C24890656 @default.
• W4226164754 hasConcept C2776595292 @default.
• W4226164754 hasConcept C2781204021 @default.
• W4226164754 hasConcept C30475298 @default.
• W4226164754 hasConcept C41008148 @default.
• W4226164754 hasConcept C558565934 @default.
• W4226164754 hasConcept C62520636 @default.
• W4226164754 hasConcept C73301696 @default.
• W4226164754 hasConcept C95312477 @default.
• W4226164754 hasConceptScore W4226164754C120665830 @default.
• W4226164754 hasConceptScore W4226164754C121332964 @default.
• W4226164754 hasConceptScore W4226164754C121684516 @default.
• W4226164754 hasConceptScore W4226164754C134786449 @default.
• W4226164754 hasConceptScore W4226164754C136959337 @default.
• W4226164754 hasConceptScore W4226164754C142362112 @default.
• W4226164754 hasConceptScore W4226164754C147120987 @default.
• W4226164754 hasConceptScore W4226164754C153349607 @default.
• W4226164754 hasConceptScore W4226164754C16332341 @default.
• W4226164754 hasConceptScore W4226164754C16389437 @default.
• W4226164754 hasConceptScore W4226164754C168834538 @default.
• W4226164754 hasConceptScore W4226164754C180048950 @default.
• W4226164754 hasConceptScore W4226164754C189166818 @default.
• W4226164754 hasConceptScore W4226164754C21368211 @default.
• W4226164754 hasConceptScore W4226164754C24890656 @default.
• W4226164754 hasConceptScore W4226164754C2776595292 @default.
• W4226164754 hasConceptScore W4226164754C2781204021 @default.
• W4226164754 hasConceptScore W4226164754C30475298 @default.
• W4226164754 hasConceptScore W4226164754C41008148 @default.
• W4226164754 hasConceptScore W4226164754C558565934 @default.
• W4226164754 hasConceptScore W4226164754C62520636 @default.
• W4226164754 hasConceptScore W4226164754C73301696 @default.
• W4226164754 hasConceptScore W4226164754C95312477 @default.
• W4226164754 hasFunder F4320306084 @default.
• W4226164754 hasFunder F4320308507 @default.
• W4226164754 hasFunder F4320322392 @default.
• W4226164754 hasFunder F4320338289 @default.
• W4226164754 hasIssue "4" @default.
• W4226164754 hasLocation W42261647541 @default.
• W4226164754 hasLocation W42261647542 @default.
• W4226164754 hasLocation W42261647543 @default.
• W4226164754 hasLocation W42261647544 @default.
• W4226164754 hasLocation W42261647545 @default.
• W4226164754 hasLocation W42261647546 @default.
• W4226164754 hasOpenAccess W4226164754 @default.
• W4226164754 hasPrimaryLocation W42261647541 @default.
• W4226164754 hasRelatedWork W1480216049 @default.
• W4226164754 hasRelatedWork W1585693316 @default.
• W4226164754 hasRelatedWork W1983514793 @default.
• W4226164754 hasRelatedWork W2043680884 @default.

• next