Fermilab rmilab Pro roject ject-X X Ove verview rview
Shekhar Mishra
Project-X,
International Collaboration Coordinator Fermilab
Ove verview rview Shekhar Mishra Project-X, International - - PowerPoint PPT Presentation
Fermilab rmilab Pro roject ject-X X Ove verview rview Shekhar Mishra Project-X, International Collaboration Coordinator Fermilab Out utline line Fermilab Complex Fermilab Strategic Plan Energy Frontier Cosmic Frontier
International Collaboration Coordinator Fermilab
– Energy Frontier – Cosmic Frontier – Intensity Frontier
– Some Design Details – R&D and Project Status
– India Collaboration
The Fermilab Tevatron has now passed on the energy frontier to LHC, following 25 years as the highest energy particle collider in the world. Fermilab operates the highest power long baseline neutrino beam in the world. But will face stiff competition from J-PARC
coming decades has been developed by the DOE’s High Energy Physics Advisory Panel (HEPAP).
– Fermilab is fully aligned with this strategy.
– Dominated by LHC. – Upgrades to LHC machine and detectors
– What follows the LHC? Depends on results and at what energy results occur
– Physics exploitation and upgrades of LHC. – R&D on future machines:
colliders at ultra-LHC energies
Tevatron LHC LHC LHC ILC, CLIC or Muon Collider Now 2016 LHC Upgrades ILC?? 2013 2019
1 2 3 4 5 6 7 8 9 10 11 12 13
Green curve: same rates as 09
2022
– The nature of dark matter and dark energy
– Get to ―zero—background‖ technology.
– Establishment of time evolution of the acceleration:
– Establish scalable ―zero-background‖ technology for dark matter. – Participate in future ground and space telescopes (the principal agencies are NSF and NASA, not DOE)
Now 2016 2013 2019 DM: ~10 kg DE: SDSS
DM: ~100 kg DE: DES
Holometer? DM: ~1 ton DE: LSST WFIRST?? BigBOSS?? DE: LSST WFIRST?? 2022
– Proton super-beams to study neutrinos and rare decays – Quark factories: in e+e- and LHCb
– The understanding of neutrino – The observation of rare decays coupled to new physics processes
– Develop the most powerful set of facilities in the world for the study of neutrinos and rare processes, way beyond the present state of the art. – Complementary to LHC.
MINOS MiniBooNE MINERvA SeaQuest NOvA MicroBooNE g-2? SeaQuest Now 2016 LBNE Mu2e Project X+LBNE m, K, nuclear, … n Factory ?? 2013 2019 2022
Collaborations for our programs
many particle experiments, …
27 countries 16 countries 23 countries
325 & 650 MHZ 1300 MHz
rare processes, nuclear and energy programs
– ~3 MW; flexible provision for beam requirements supporting multiple users – < 5% of beam is sent to the Main Injector
– Linac would be 1300 MHz with <5% duty cycle
– A continuous wave (CW), very high power, superconducting 3 GeV linac.
– Greatly enhances the capability for rare decays of kaons, muons
– Standard Model tests with nuclei (ISOL targets), – Possible energy and transmutation applications, – Cold neutrons
Main Injector
– the most intense beams of neutrinos at high energy (LBNE) and low energy (for the successors to Mini and MicroBooNE)
experiments run simultaneously
– scope would be difficult to reproduce elsewhere
3 GeV CW linac 3-8 GeV pulsed linac 8-120 GeV existing machines
15
a Nuclear Energy program, including transmutation
– Multi MW CW beam at 1-2 GeV (similar to Fermilab Project-X) could be the accelerator and target technology demonstration project.
experiments
– 2 MW proton source at 60-120 GeV
for kaon and muon based precision experiments
– Operations simultaneous with the neutrino program
– Requires ~4 MW at ~5-15 GeV .
– Nuclear physics – Nuclear energy applications (Demonstration: Accelerator and Transmutation)
isional Siting
CW Linac Pulsed Linac
18 PX Briefing to OHEP
3 Gev cw linac 8 Gev beam transport 3 Gev beam transport 3-8 Gev pulsed linac
MeV, 1/10mA avg/peak
– Pulsed RFQ under test at Fermilab
– High Bandwidth Chopper – RT bunching cavities, P < 5 kW each – Triplet (RT) optics (keep round beam)
MEBT RFQ
H-gun
Room Temp (RT) (~15m)
SSR0 SSR1 SSR2 LE HE ILC #Cavities 18 18 40 48 152 224 #Solenoids 18 18 20 #Quadrupoles 32 46 28 #Cryomodules 1 2 4 8 19 28 Length, m 11.38 15.2 33.6 157.05 330.51 353.27 Position, m 11.38 26.58 60.18 157.11 487.62 Period Length, m 0.61 0.8 1.6 6.06 13.76 25.23 #Periods 18 18 10 16 19 14 Transition Energy, MeV 10.79 35.17 153.7 537.32 3038 8319 Transition Beta 0.150 0.266 0.511 0.771 0.972 0.995
SSR0 SSR1 SSR2 β=0.6 β=0.9 325 MHz 2.5-160 MeV 650 MHz 0.16-3 GeV ILC 3-8 GeV
Cavity ity Gradien ient
Cavity ity Power er
Energy rgy Gain pe per Ca Cavity ty
Project-X is a compact SRF Accelerator: Design enhances capabilities and reduces cost.
cavity type β G Freq MHz Beam pipe ø, mm Va, max MeV Emax MV/m Bmax mT R/Q, Ω G, Ω *Q0,2K 109 Pmax,2K W SSR0
β=0.115 325 30 0.6 32 39 108 50 6.5 0.5
SSR1
β=0.215 325 30 1.47 28 43 242 84 11.0 0.8
SSR2
β=0.42 325 40 3.34 32 60 292 109 13.0 2.9 Parameters of the single-spoke cavities
SSR0 - design SSR1 – prototyping, testing SSR2 - design
Parameter LE650 HE650 ILC β_geomet eometri ric 0.61 0.61 0.9 0.9 1 Cavity vity Length th = ncell
ll∙βgeom/2
mm 703 703 1038 1038 1038 1038 R/Q Ohm 378 378 638 638 1036 1036 G-facto actor Ohm 191 191 255 255 270 270
/cavity vity (on
st) MeV 11.7 11.7 19.2/17 2/17.7 .7* 17.2 17.2
ient MV/m 16.6 16.6 18.5 5 / 17 16.9 16.9 Max surf
tric field ld MV/m 37.5 37.5 37.3 3 / 34 34 34 Max surf
etic field eld, mT 70 70 70 / 61.5 72 72 Q0 @ @ 2°K 1010 1.5 1.5 2.0 2.0 1.5 1.5 P2K max [W] 24 24 29 / 24 20 20
1.3 GHz ILC
650 MHz: β=0.61 650 MHz: β=0.9
Most t Recent ent 9-cell, ell, 1.3 GHz Cavity ty Results lts
6 cavitie ities buil ilt by ACCEL L and 6 by AES
Courtesy of R Geng
ILC
PX PX
Final Assembly HTS VTS
String Assembly
MP9 Clean Room
VTS
ANL/FNAL EP
1st U.S. built ILC/PX Cryomodule 1st
st Dressed
ed Cavity
Ion Source and RFQ 325 MHz Spoke Cavity Test Facility 1.3 GHz HTS HINS Linac enclosure for 10 MEV Source of cryogenics Scale: Square blocks are 3ft x 3ft
27 27
Cryomodule-1 (CM1) (Type III+) Capture Cavity 2 (CC2) CC2 RF System 5 MW RF System for CM1
28 28
Cryomodules Capture Cavity 1 (CC1) 5MW RF System for Gun CC1 & CC2 RF Systems RF Gun 5MW RF System for Cryomodules Future 10MW RF System CC2 Future 3.9/Crab Cavity Test Beamlines
– Detailed Lattice designed – New gun system being installed
– CC2 (single 9-cell cavity) operational - 10/09
– CM1 installed, aligned, and under vacuum – Cooled, Under RF Power
cost range documentation for CD-0, Feb 2011
Department of Energy briefing on November 16-17, 2010
technical questions
– Baseline concept for the chopper – Concept for marrying the 3-8 GeV pulsed linac to CW front end – Injection into the Recycler – SRF and RF development at all relevant frequencies
construction start is FY2016
– We are receiving very significant R&D support for Project X and SRF development (~$40M in FY11, not including ARRA (stimulus))
Project X could be up and running in ~2020
Indian Institutions: BARC/Mumbai IUAC/Delhi RRCAT/Indore VECC/Kolkata
to execute the Project X RD&D Program.
– Being organized as a ―national project with international participation‖.
established through bi-lateral MOUs.
sub-system design, development, and construction. – National Collaboration MOU signatories:
ANL ORNL/SNS BNL MSU Cornell TJNAF Fermilab SLAC LBNL ILC/ART
Project-X accelerator and Physics programs
– Accelerator collaboration:
– Physics Collaboration:
while enhancing in new physics and application areas
– All aspects of CW Linac – Plan is to jointly develop accelerators at Fermilab and in India
– Dzero (Energy Frontier) – MINOS, NOvA, LBNE, MIPP (Intensity Frontier) – LHC-CMS Center at Fermilab – Exploring collaboration in
– World leading programs in neutrinos and rare processes; – Potential applications beyond elementary particle physics;
– Aligned with ILC and Muon Accelerators
with the requirements of the physics program:
– 3 GeV CW linac operating at 1 mA: 3 MW beam power – 3-8 GeV pulsed linac injecting into the Recycler/Main Injector complex
2020 http://projectx.fnal.gov/
Proton Energy (kinetic) Beam Power Beam Timing Rare Muon decays 2-3 GeV >500 kW 1 kHz – 160 MHz (g-2) measurement 8 GeV 20-50 kW 30- 100 Hz. Rare Kaon decays 2.6 – 4 GeV >500 kW 20 – 160 MHz. (<50 psec pings) Precision K0 studies 2.6 – 3 GeV > 100 mA (internal target) 20 – 160 MHz. (<50 psec pings) Neutron and exotic nuclei EDMs 1.5-2.5 GeV >500 kW > 100 Hz
Working groups established to outline experimental needs in five areas: http://www.fnal.gov/directorate/Longrange/Steering_Public/work shop-physics-5th.html
excluded but very unlikely
there are crucial long term advantages to Project X
experiments and neutrinos simultaneously. At JPARC the 50 GeV synchrotron is used for neutrinos and rare decays – requiring sharing
land for expansion