1. Roundtable Discussion on Future Machines – Quy Nhon, 14.08.2014 Participants: Roy Aleksan, CEA, Chair of ESGARD Alain Blondel, Professor of particle physics at U. Geneva Oliver Brüning, CERN, BE/ABP Group Leader, HL-LHC Deputy Project Leader Swapan Chattopadhyay, FNAL & NIU & CERN (former director of CI/UK) Serguei Ganjour, CEA Francois Le Diberder, CNRS/IN2P3/LAL Katsunobu Oide, KEK, Director of KEK Accelerator Laboratory Maxim Titov, CEA Kaoru Yokoya, KEK, ILC GDE Regional Leader for Asia Frank Zimmermann, CERN, convener Excused: Jie Gao, Yifang Wang, Nima Arkani-Hamed, IHEP Beijing; Tao Han, Pittsburgh

2. Roundtable Discussion on Future Machines – Quy Nhon, 14.08.2014 Introductory presentations (20’) Discussions (30’): 1. Do we need precision or/and high energy? How precisely do we need to measure various couplings? How many Higgs decays, how many Z decays should be produced? Which energy should we aim for? Which collider has the strongest physics case after the HL-LHC? 2. How can we make sure that the wishes of the physics community are synchronized with the technical developments in the accelerator sector? How mature are the technologies for hadron collider, circular or linear e+e-, and other colliders? 3. What risks do we have for reaching the announced performance levels for hadron collider, circular or linear e+e- collider (or gg or muon) collider? How long will the commissioning take? 5 4. Can one extrapolate the “LHC” collaboration models to the next machine? 5. To what extent should the choice of the next project be driven by a long- term strategy? Concluding remarks (5’)

3. Courtesy W. Fischer hadron-collider peak luminosity vs. year LHC run 1 (2012-13) accumulated more integrated luminosity than all previous hadron colliders together!

4. S. Henderson past, future & proposed e + e - colliders FCC-Z FCC-W FCC-H FCC-t ILC 500 ILC 250

5. e + e - luminosity vs energy additional ILC upgrades (Harrison, Ross, Walker, 2013) FCC-ee crab waist / improved optics (Bogomyagkov, Levichev, Piminov, Shatilov, 2014)

6. commissioning times & performance of circular e + e - colliders PEP-II KEKB DA  NE

7. commissioning time & performance of the first linear collider CERN-SL-2002- 009 (OP), SLAC–PUB–8042 [K. Oide, 2013] SLC LEP1 (per IP) SLC design SLC -½ design value reached after 11 years LEP1 design SLC total integrated luminosity ~2 pb -1 LEP1+2 total integrated luminosity ~1 fb -1 (x4 IPs)

8. “Of course, it should not be the size of an accelerator, but its costs which must be minimized.” Gustav-Adolf Voss, builder of PETRA at PAC1995 Dallas † 5. October 2013

9. Roundtable Discussion on Future Machines – Quy Nhon, 14.08.2014 Introductory presentations (20’) Discussions (30’): 1. Do we need precision or/and high energy? How precisely do we need to measure various couplings? How many Higgs decays, how many Z decays should be produced? Which energy should we aim for? Which collider has the strongest physics case after the HL-LHC? 2. How can we make sure that the wishes of the physics community are synchronized with the technical developments in the accelerator sector? How mature are the technologies for hadron collider, circular or linear e+e-, and other colliders? 3. What risks do we have for reaching the announced performance levels for hadron collider, circular or linear e+e- collider (or gg or muon) collider? How long will the commissioning take? 5 4. Can one extrapolate the “LHC” collaboration models to the next machine? 5. To what extent should the choice of the next project be driven by a long- term strategy? Concluding remarks (5’)

10. back up

11. LEP – largest circular e + e - collider so far R. Assmann, Chamonix 2001 1000 pb -1 from 1989 to 2000

12. ATF-21.280.000001(eff.) 0.005 (eff.)- [>4*] comparing commissioning times & performance beam energy [GeV] design luminosity [10 32 cm -2 s -1 ] peak luminosity /design time to achieve design [y] LEP1450.1325 SLC450.060.5- (>10 ) LEP260-104.50.263<0.5 DAFNE0.55.00.9- (>10) PEP-II9, 3.13041.5 KEKB8, 3.510023.5 * not counting the year of the earthquake; ATF-2 operating only for fraction of calendar time

13. parameterLEP2FCC-eeCepC ZZ (c.w.)WHtH E beam [GeV]10445 80120175120 circumference [km] 26.7100 54 current [mA]3.014501431152306.616.6 P SR,tot [MW]22100 no. bunches41670029791449013609850 N b [10 11 ]4.21.81.00.70.461.43.7  x [nm] 22290.143.30.9426.8  y [pm] 25060112220   x [m] 1.20.5 1.00.8   y [mm] 50111111.2   y [nm] 3500250321304445160  z,SR [mm] 11.51.642.71.010.811.162.3  z,tot [mm] (w beamstr.) 11.52.565.91.491.171.492.7 hourglass factor F hg 0.990.640.940.790.800.730.61 L/IP [10 34 cm -2 s -1 ] 0.01282121261.71.8  beam [min] 3002873972302340

14. Cms energy Luminosity parameterLHCHL-LHCFCC-hhSppC (May14) c.m. energy [TeV]1410063 dipole magnet field [T]8.3316 (20)20 circumference [km]26.7100 (83)50 luminosity [10 34 cm -2 s -1 ]155 [→20?]12 bunch spacing [ns]2525 (5)25 events / bunch crossing27135170 (34)373 bunch population [10 11 ]1.152.21 (0.2)2 norm. transverse emitt. [  m] 3.752.52.2 (0.44)3.3 IP beta-function [m]0.550.151.10.75 IP beam size [  m] 16.77.16.8 (3)8.5 synchrotron rad. [W/m/aperture] 0.170.3328 (44)46 critical energy [keV]0.0444.3 (5.5)2.2 total syn.rad. power [MW] 0.00720.01464.8 (5.8)3 longitudinal damping time [h] 12.90.54 (0.32)1.0

15. Lyn Evans, AWLC14