The CERN plan for the LHC upgrade

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Presentation transcript:

The CERN plan for the LHC upgrade Lucio Rossi CERN – TE dept Accelerator seminar @ Fermilab 29Jul2010

Content LHC today, performances and consolidation plan LHC upgrade: overview of the past work Phase 1 (+ Phase 2 ?) LHC-INJ upgrade The new plan HL-LHC Concept Hardware Preliminary plan The « definitive » upgrade: HE-LHC 29 July 2010 L Rossi @ Fermilab

Luminosity today scope 0.1 fb-1 by 2010 – 1 fb-1 by 2011 ca. 70 nb-1 in last fill! Work to have nominal bunch intensity of 1.1 e11 ppb Approach with high bunch intensity paid off (investment of commissioning time) 9e10 p per bunch up to 13 bunches (8 crossing pairs/IP) Record Lpeak= 1.6 1030 Trying to resume the ramp at 10A/s (today working at 2 A/s because of n-QPS/PS interaction Yesterday first multibuch injection (4 b/fill) Today first attempt to 25 b (16 Xing pairs/IP) 29 July 2010 L Rossi @ Fermilab

Also thanks to your magnets… 29 July 2010 L Rossi @ Fermilab

The two problems of LHC for reaching nominal performance Beam Energy: IC joints limits to 3.5 TeV/beam We do not have anymore bad SC splice: the worst is 3 nΩ (specs is 0.6 nΩ, the one that melt away was 220 nΩ) However we have left behind us many unstabilized joints… Beam Intensity: collimation limits lumi to 0.05-0.2 1034 Today all so called phase 1 collimation is installed Phase 2 collimation has changed dramatically 1 years ago: studies pointed to the need of collimators in the COLD regions (DS). 29 July 2010 L Rossi @ Fermilab

We recovers from here… M3 line 29 July 2010 L Rossi @ Fermilab

And here… 29 July 2010 L Rossi @ Fermilab

Looking back… LHC Interconnection joints 0.2 nOhm 220 nOhm Most likely reconstruction of the one that melted away 29 July 2010 L Rossi @ Fermilab

A78.RB: Normalized Bus Segment Resistance Every single sc splice were measured in 2009 29 July 2010 L Rossi @ Fermilab

The problem still left Unstabilized joint (silent killer) Existance of unfilled gap was known during IC work in 2006 and reported. No problem for 1-2 mm gap… End february 2009 an empty bus bar (20 m or more) discovered in a spare quadrupole through -ray The picture above discovered in the tunnel in sector 3-4 in April 2009. It is 30 cnm long and it shows an extra resistance at room temperature of about 35 µΩ 29 July 2010 L Rossi @ Fermilab

29 July 2010 L Rossi @ Fermilab

situation We know we left behing unstabilzed length of 40 mm (50 microOhm) We measured well only 4 sector warm On the 4 sectors left cold (100 K) measurements are noisy. A statistical analysis showed that a 90 microOhm (70 mm lenght unstabilized) could not be excluded  run at 3.5 TeV/beam Plan 2012 – 2013 (April): open all 3 M lines/IC containing bus bars; re-solder the 10-15% defective joint ones (experience) fix the stability on ALL IC joint by means of a copper shunt 29 July 2010 L Rossi @ Fermilab

The fix to cure unstability Making the shunt (reduntant!) Making a box for lateral restraint and vertical containment) 29 July 2010 L Rossi @ Fermilab

Will we reach 7 TeV ? Dipole training… In principle 4 quenches/day with 2-4 sectors going in parallel was foreseen for training in the design: say at least 10 quench/day for HWC. We might have expected less than 100 quenches to reach nominal based on best prototypes + preseries dipoles (2000-2002) Analysis done experience7 TeV based on analysis of 2005-07 indicated that we should have expected 250 Re-analysis (see (E. Todesco at Chamonx 2010), of the same acceptance test data, points to 400: about 40 days of HWC. However HWC data, extrapolated from one sector only indicates about 800 ! 29 July 2010 L Rossi @ Fermilab

Actual resutls in single test (all) and in the LHC HWC for sector 5-6 only 100 quenches to 6.5 TeV 250 quenches to 6.75 TeV 500-800 to 7 TeV ! 29 July 2010 L Rossi @ Fermilab

Interim Collimation 2013 Collimation upgrade in IR3 dispersion suppressors to capture p losses due to single-diffractive scattering and to capture ion losses (removes highest predicted and highest measured loss). Collimation upgrade in IR3 warm insertion (10 vertical collimators added) to add flexibility for relocating losses from IR7 to IR3 (SEE limitations). Prepare work for 2015/16 collimation upgrades. Gain: Hope to reach nominal intensity and up to half nominal luminosity. Lower complexity. Smaller horizontal impedance. Higher cleaning efficiency. Price to pay: Twice larger vertical impedance, additional loss spike in IR5 and higher losses at tertiary collimators. IR3 upgrade is an excellent step forward but no miracle solution. Ralph Assmann

Not discussed today! Full Collimation 2016 Collimation upgrade in IR7 and IR2 dispersion suppressors to capture p losses due to SD scattering and to capture ion losses. Installation of advanced collimators (mostly into prepared empty slots) to allow non-destructive and very fast collimator setup, compatible with LHC stability and small b* (0.55m). SLAC very motivated to participate to construction, “regardless of the technology chosen for the secondary collimators to be installed” (e-mail associate lab director B. Hettel). Collimation upgrade in IR1 and IR5 for luminosity-induced losses from collisions (install 4 already produced Cu collimators). Collimation upgrade in IR2 for ZDC acceptance issue. EARLIER??? Remote handling and air bypass operational in IR7. Additional tungsten absorbers in IR6 dump protection system to improve local cleaning. Not discussed today! Ralph Assmann

Dispersion Suppressor Work Addresses a very basic limitation of the LHC collimation system: protons lose energy when hitting matter, ions dissociate and fragment! Could not be addressed before: collimation started very late in the game and SC areas of LHC were frozen. Note that this is nothing exotic: other accelerators had this (e.g. LEP2 added collimators into dispersion suppressors). A solution without new SC magnets was proposed: allows collimation readiness for nominal and ultimate beams by 2015/6 at latest (if we start). Other solutions are nice but would come much later (e.g. shorter magnets with collimator in front).  What – Where – Why Ralph Assmann

TCRYO Upgrade Scenario Downstream of IR7 b-cleaning NEW concept halo Halo Loss Map Losses of off-momentum protons from single-diffractive scattering in TCP cryo-collimators Upgrade Scenario Note: now in front of Q10 transversely shifted by 3 cm NEW concept halo without new magnets and civil engineering -3 m shifted in s +3 m shifted in s

The LHC upgrade: LHC and EU Particle Physics - Lisbona 2006 The European strategy for particle physics … Scientific activities 3. The LHC will be the energy frontier machine for the foreseeable future, maintaining European leadership in the field; the highest priority is to fully exploit the physics potential of the LHC, resources for completion of the initial programme have to be secured such that machine and experiments can operate optimally at their design performance. A subsequent major luminosity upgrade (SLHC), motivated by physics results and operation experience, will be enabled by focussed R&D; to this end, R&D for machine and detectors has to be vigorously pursued now and centrally organized towards a luminosity upgrade by around 2015. Statement is perfectly actual and valid However the date must be shifted 5 years 1 y of delay in LHC and detector commissioning 2 y for the incident and for next splice consolidation 2 y more of operation to reach ~500 fb-1 (Int. Lumi per year ~ 50 fb-1, not 100 !) 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

L. Rossi - HL-LHC Design Study @ ESGARD The baseline in 2003-2006 Radiation damage limit ~700 fb-1 Paper of J. Strait et al. PAC2003 Need of change in 2013 -15. Main hardware: HF Quadrupole magnets for 13-15 T New program (in // to LHC construction) US-LARP in US in 2003 (6 MCHF/y 2006-13) – based on a Nb3Sn DOE program 1998-2010 FP6-CARE : NED JRA to develop EU Nb3Sn in 2004-08 . Its positive effects NOW! FP7 EuCard IA: WP on HFM 2009-2012 In 2007 new – anticipated – scenario : Nb3Sn not ready before 2015-17 Decision to target a first upgrade in 2012-13 Phase 1 based on Nb-Ti Ø=120 mm FP7 SLHC-PP launched for 2008-2010 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

Updated LHC lumi vs. (end of) year 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD Courtesy of M. Lamont, spring 2010

L. Rossi - HL-LHC Design Study @ ESGARD Intensity Limits Intensity Limitations (1011 protons per bunch)   Present SPL-PS2 2GeV in PS Linac2/LINAC4 4.0 PSB or SPL 3.6 PS or PS2 1.7 3.0 SPS 1.2 >1.7? LHC 1.7-2.3? Reminder design = 1.15 (for 1034); Ultimate = 1.7 (for 2.3x1034) From S. Myers Conclusion: We continue (as planned) and terminate the study for LP-SPL/PS2 and study in parallel the PS Booster energy upgrade Decision can be taken when we have the results of these studies and experience with the LHC operation 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

MTP “Observations from the DG” Thus, the MTP assumes the feasibility of the energy upgrade of the PS Booster and does not include the start of the LP-SPL and PS2 construction as of 2013 In order to optimize the strategy towards the HL-LHC, with the goal of maximizing the integrated luminosity useful for physics, Management has set up a task force. A preliminary recommendation from this task force is to delay the inner triplet replacement to a single HL-LHC upgrade around 2020. From S. Myers 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

Phase 1 assessment: summary from taskforce @ LMC-10Mar2010 - 2a Disadvantage of the Phase 1. Optics much more rigid; requires special scheme. Aberration sat the limit of LHC correction capability. Longer magnets (same technology) does not help. 30 cm  is more difficult than 55 cm of the present LHC. Better solution found with  = 40 cm offering a 3 sigma margin per beam (which was part of the initial goal) but only 1.2 gain in lumi over nominal. Today we are limited by a single element. IR upgrade will use all the margins in the whole ring. To change this: modification in MS positions and replacement of a few magnets, additional IR collimators to catch higher losses in IR matching section (lower aperture due to higher beta* in the not-changed magnets Use ultimate strength in the sextupoles, NEW powering scheme of MQT corrector families. Logistics is hard: The logistic for ancillary equipment is hard. A solution NOT fully satisfactory has been found for IP1; more difficult for IP5. A real long term solution devised (see S. Weisz in Chamonix and SC links by A. Ballarino). This solution should be integrated in a more global study for R2E radiation protection of electronics 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

Phase 1 assessment: summary from taskforce @ LMC-10Mar2010 - 2b Disadvantage of the Phase 1 The use of the same refrigerator for RF and Arc-IT in 4-5 makes 5L (CMS) weaker in term of cryo-power for high luminosity. The new schedule of LHC: we will not be at nominal before 2014-15 at the very best, and the 300-400 fb-1 are foreseen well beyond 2020. Because of past and future delay (splice consolidation) the IT phase 1 cannot be installed anyway before 2016/17. 1 year optimistic installation time + needed time for a new commissioning of the machine The fairly long stop, and the relatively low gain factor: 2 at max, 1.2 at min) require 2.5 to 5 years just to catch up. Then other long stops will be required for L > 2-3 1034. 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

Phase 1 assessment: summary from taskforce @ LMC-10Mar2010 – 3 Recommendation about Phase 1 Stop the phase 1 project Keep going on the R&D of Phase 1 that is necessary because of long lead time development; Decision in 2013/2014, after LHC behaviour near nominal will be known, the best technology for upgrade. We can’t start construction before half 2013. Decision in 2014 to have it by 2018-2020. Put the IT upgrade in a global pictures, preceded by all consolidation or improvement needed to make it most effective and compatible with other equipment. 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

What needs for average lumi 5x1034 New lay-out of some part of LHC Improve some correctors Commissioning @ 600-650 A the lattice sextupoles New MQT corrector scheme using existing spare 600 A bus bars Re-commissioning DS quads at higher gradient Review MSs Change of New Q5/Q4 (larger aperture), with new stronger corrector orbit, displacements of few magnets Larger aperture D2 (may be other actions, more quads in points 6 and 7) Displacement of Power Converters & DFBs at least of Inner Triplets but also of OTHER equipment on surface by means of SC links. Cryo-plant for RF in point 4 : 5-7 kW @ 4.5 K 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

The main ingredient of the upgrade -1 IR Quads High Gradient/Large Aperture Quads, with Bpeak 13-15 T. Higher field quadrupoles translate in higher gradient/shorter length or larger aperture/same length or a mix . US-LARP engaged to produce proof by 2013. Construction is 1 year more than Nb-Ti : by 2018 is a prudent assumption.  as small as 22 cm are possible with a factor 2.5 in luminosity by itself, if coupled with a mechanism to compensate the geometrical reduction. If a new way of correcting chromatic aberration could be found,  as small as 10-12 cm can be eventually envisaged. 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

L. Rossi - HL-LHC Design Study @ ESGARD HF Nb3Sn Quad Nb3Sn is becoming a reality (first LQ long -3.6 m – quad 90 mm) This year we expect a second LQ and a 1 m long - 120 mm aperture model In 3 years: 4-6 m long magnets, 120 mm ap., G=180-200 T/m G= 200 T/m 160 T/m Gequiv LHC 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

We are near… Test of LARP HQ – 120 mm Max critical current Goal HL-LHC (G=180 T/m) Goal Phase 1 (G=127 T/m) 29 July 2010 L Rossi @ Fermilab

The main ingredient of the upgrade - 2 RF Crab cavities Crab Cavities: this is the best candidate for exploiting small  (for  around nominal only +15%). However it should be underlined that today Crab Cavities are not validated for LHC , not even conceptually: the issue of machine protection should be addressed with priority. Global Scheme. 1 cavity in IP4, Proof on LHC, good for 1 X-ing. Semi-global; it may work!(JP Koutchouck) Local scheme; 1 cavity per IP side. Maybe local doglegs needed. Early Separation Scheme could be an alternative (or a complement) Both scheme, Crab Cavities and ESS provide a simple mean to do levelling 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

L. Rossi - HL-LHC Design Study @ ESGARD Crab Cavities qc Elliptical 800 MHz not far from being designed. Require 400 mm beam-beam 400 MHz small cavity under conceptual study, they can (?) fit in 194 mm beam-beam. Required for final solution Ref. : F. Zimmermann, Ed Ciapala 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

Collimation: need of room in DS of P7, P2… 11 T–11 m Twin Dipole for DS Shift in the magnet position requires to make room for collimators (red squares). Alternative option based on stronger and shorter magnets (blue rectangles). 2 dips/Point

Addressing R2E (upgrade +consolidation) 120 kA were already assembled at CERN last year. Sub-cables were tested at CERN at currents of up to 18 kA (@ 4.5 K and in self-field) 1.1 mm MgB2 wire

L. Rossi - HL-LHC Design Study @ ESGARD And more … New Cryoplants in IP1 & IP5: for power AND to make independent Arc- IR: 2.8 kW @ 1.8 K scales as 5.2 kW @ 2 K (for 1 set of cold compressor) Working at 4.2 K will be a plus (for IR magnets) Special dedicated collimation system (also for background) and Machine protection Robotics for remote manipulation Dismantling present Triplet Installation HL-LHC Maintenance Dismounting HL-LHC ??? 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

It is new entire project  we need a Design Study We will try to get a EU funded DS (design Study) in the FP7 The work of SLHC-PP (Phase 1) has been essential to arrive to thsi point and most of it will be used Scope of the HL-LHC DS: Carry out the study to produce a consistent design to reach 5 1034 with levelling, allow LHC to reach the goal of 3000 fb-1 by 2030(s) Exploring in details all solutions and paths for the upgrade, both in terms of LHC operational mode and hardware changes Producing by end 2013 a PDR (Preliminary Design Report) enabling the CERN management, to make a choice about the configuration of LHC upgrade in 2014. Producing by end of 2014/half 2015 a TDR (Technical Design Report) of the selected path for the upgrade defining the maximum goal for the LHC luminosity 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

Resources for the program 10 M€ total cost over 4 years: July 2011-2015 Reimbursment by EU 30-40% may be reimbursed by EU to EU Institution Total cost of the LHC upgrade : 500 M Cost of the R&D & Study : at least 50 M (teh contribution of EU is marginal… … However si important to get a structured organization in which project is governed by a collaboration… Possibility for US labs (and/or DOE , LARP) and KEK to be full partner of the governing board of the EU DS. Would the EU Ds not be approved we intend to promote the collaboration with MoUs very much like detectors. A first step for Design and R&D A second step for actual construction 28 June 2010 L. Rossi - HL-LHC Design Study @ ESGARD

R&D on enabling technologies CERN Council & DG Collaboration Board Advisory Committee FP7 Design Study framework Project Office: Resource manager Technical coordinators Project Coordinator Steering Committee R&D on enabling technologies Design Studies Technical Design WP2 WPn EuCARD I see the 11T dipoles as part of HL-LHC but outside the EU DS WP1 USLARP Organization model for HL-LHC Jpk 27/4/2010

with the iron yoke – Coils are in blue HE-LHC The High Luminosity LHC or HL-LHC is the route that will enable the way to the Farthest Energy Frontier : an HE-LHC based on 20 T magnets for a 33 TeV c.o.m. collider HE-LHC Workshop 14-16 October in Malta By 2035 ? Nb3Sn + HTS magnets Sketch of the double aperture magnet with the iron yoke – Coils are in blue transmission line magnets of new injector Field in the coil (one pole shown) at 20 T operational field