002750280 001__ 2750280
002750280 003__ SzGeCERN
002750280 005__ 20210511151824.0
002750280 0248_ $$aoai:inspirehep.net:1842527$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT$$pcerncds:CERN$$qINSPIRE:HEP$$qForCDS
002750280 035__ $$9http://old.inspirehep.net/oai2d$$aoai:inspirehep.net:1842527$$d2021-01-25T19:53:38Z$$h2021-01-26T05:00:08Z$$mmarcxml
002750280 035__ $$9Inspire$$a1842527
002750280 041__ $$aeng
002750280 100__ $$aFerlin, G$$uCERN
002750280 245__ $$aCryogenics Experience during Run 2 and impact of LS2 on next run
002750280 260__ $$c2019
002750280 300__ $$a6 p
002750280 520__ $$9Grobid$$aThe first part of the presentation will summarize the overall cryogenic
performance and availability for Run 2. Main evolutions and effects on the
cryogenic system during Run 2 will be presented. The second part will focus on
the LS2, in particular the main maintenance and evolutions engaged. We will
present their expected effects on the global availability on one hand and their
expected influence on the cryogenic limitations with respect to the required
cooling power during Run 3 on the other hand. Finally, we re-formulate the
expected cooling power limitations taking into account the balance between 1.9 K
cooling power used for Inner Triplet and 4.5-20 K non-isothermal cooling power
used for Beam Screens.
002750280 690C_ $$aCERN
002750280 693__ $$aCERN LHC
002750280 700__ $$aBradu, B$$uCERN
002750280 700__ $$aBrodzinski, K$$uCERN
002750280 700__ $$aDelprat, L$$uCERN
002750280 700__ $$aPezzetti, M$$uCERN
002750280 773__ $$01835544$$c85-90$$wC19-01-30.1
002750280 8564_ $$82274879$$s769386$$uhttps://cds.cern.ch/record/2750280/files/1835544_85-90.pdf$$yFulltext
002750280 962__ $$b2706427$$k85-90$$nevian les bains20190130
002750280 960__ $$a13
002750280 980__ $$aARTICLE
002750280 980__ $$aConferencePaper