Heavy ion operation from run 2 to HL-LHC

The nuclear collision programme of the LHC will continue with Pb-Pb and p-Pb collisions in Run 2 and beyond. Extrapolating from the performance at lower energies in Run 1, it is already clear that Run 2 will substantially exceed design performance. Beyond that, future high-luminosity heavy ion operation of LHC depends on a somewhat different set of (more modest) upgrades to the collider and its injectors from p-p. The high-luminosity phase will start sooner, in Run 3, when necessary upgrades to detectors should be completed. It follows that the upgrades for heavy-ion operation need high priority in LS2.

[1]  M. Blaskiewicz,et al.  POTENTIAL OF STOCHASTIC COOLING OF HEAVY IONS IN THE LHC , 2013 .

[2]  Hans-Heinrich Braun,et al.  Hadronic and electromagnetic fragmentation of ultrarelativistic heavy ions at LHC , 2014 .

[3]  W. Fischer,et al.  Time evolution of the luminosity of colliding heavy-ion beams in BNL Relativistic Heavy Ion Collider and CERN Large Hadron Collider , 2010 .

[4]  A. Ferrari,et al.  COLLIMATION OF HEAVY ION BEAMS IN LHC , 2004 .

[5]  Rhoades-Brown,et al.  Heavy-ion partial beam lifetimes due to Coulomb induced processes. , 1996, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[6]  S. Redaelli,et al.  ALICE spectrometer polarity reversal , 2012 .

[7]  M. Blaskiewicz,et al.  Three-dimensional stochastic cooling in the relativistic heavy ion collider. , 2010, Physical review letters.

[8]  Z. Vilakazi,et al.  Measurement of electromagnetic cross sections in heavy ion interactions and its consequences for luminosity lifetimes in ion colliders , 1999, Proceedings of the 1999 Particle Accelerator Conference (Cat. No.99CH36366).

[9]  J. Jowett,et al.  Heavy ion beams in the LHC , 2003, Proceedings of the 2003 Particle Accelerator Conference.

[10]  C. Oppedisano,et al.  Measurement of the electromagnetic dissociation cross section of Pb nuclei at = 2.76 TeV , 2011, 1107.1985.

[11]  C. Carli THE LHC AS A PROTON-NUCLEUS COLLIDER , 2006 .

[12]  R. Bruce,et al.  Quench tests at the Large Hadron Collider with collimation losses at 3.5 Z TeV , 2012 .

[13]  P. Cochat,et al.  Et al , 2008, Archives de pediatrie : organe officiel de la Societe francaise de pediatrie.

[14]  Elena Shaposhnikova,et al.  LIMITS TO THE PERFORMANCE OF THE LHC WITH ION BEAMS , 2004 .

[15]  J. Borburgh,et al.  Ions for LHC: Status of the injector chain , 2007 .

[16]  A. Morsch,et al.  Proton–nucleus collisions at the LHC: scientific opportunities and requirements , 2011, 1105.3919.

[17]  R. Bruce,et al.  OPERATING THE LHC OFF-MOMENTUM FOR p-Pb COLLISIONS , 2013 .

[18]  Kain,et al.  First proton-nucleus collisions in the LHC: the p-Pb pilot physics , 2012 .

[19]  T. Weiler,et al.  Measurements of heavy ion beam losses from collimation , 2009, 0908.2553.

[20]  Z. L. Matthews,et al.  The ALICE experiment at the CERN LHC , 2008 .

[21]  S. Fartoukh,et al.  Achromatic telescopic squeezing scheme and application to the LHC and its luminosity upgrade , 2013 .

[22]  Daniel Valuch,et al.  p-Pb Feasibility Test and Modifications of LHC Sequence and Interlocking , 2012 .

[23]  Bunch-by-Bunch Analysis of the LHC Heavy-Ion Luminosity , 2013 .

[24]  R. Bruce,et al.  LUMINOSITY AND BEAM PARAMETER EVOLUTION FOR LEAD ION BEAMS IN THE LHC , 2011 .

[25]  S. A. Sadovsky,et al.  The physics of ultraperipheral collisions at the LHC , 2007, 0706.3356.

[26]  R. Bruce,et al.  Beam losses from ultra-peripheral nuclear collisions between 208Pb82+ ions in the Large Hadron Collider and their alleviation , 2009, 0908.2527.

[27]  J. Wenninger,et al.  THE LHC BEAM POSITION SYSTEM: PERFORMANCE DURING 2010 AND OUTLOOK FOR 2011 , 2011 .