SNuMI (>1MW) SNuMI 1 Motivations for SNuMI The neutrino experimental program for the next decade –NOνA (long baseline νμ→νe search) –MINERνA (Main Injector.

Slides:



Advertisements
Similar presentations
Electron Cooling in the Accumulator McGinnis Electron Cooling in the Accumulator Dave McGinnis.
Advertisements

Muon Coalescing 101 Chuck Ankenbrandt Chandra Bhat Milorad Popovic Fermilab NFMCC IIT March 14, 2006.
1 Proton Upgrades at Fermilab Robert Zwaska Fermilab March 12, 2007 Midwest Accelerator Physics Collaboration Meeting Indiana University Cyclotron Facility.
 An h=4 (30 MHz) RF system will be used for electron operation. For protons, this would correspond to h=56, and the 1 kV maximum gap voltage would only.
Nufact09-IIT 107/24/2009 Project X and a Muon Facility at Fermilab Milorad Popovic FNAL.
Re-commissioning the Recycler Storage Ring at Fermilab Martin Murphy, Fermilab Presented August 10, 2012 at SLAC National Laboratory for the Workshop on.
NOvA meeting PIP Update W. Pellico. PIP Goals and Scope (Provided in 2011 – Directorate S. H. / DOE Talk ) Goals: Specific to the issues surrounding the.
Eric Prebys Representing the “Mu2e Task Force”: Steve Werkema Jim Morgan Vladimir Nagaslaev Chuck Ankenbrandt Vladimir Shiltsev Ioanis Kourbanis *Mu2e-doc-1911.
Paul Derwent 30 Nov 00 1 The Fermilab Accelerator Complex o Series of presentations  Overview of FNAL Accelerator Complex  Antiprotons: Stochastic Cooling.
(ISS) Topics Studied at RAL G H Rees, RAL, UK. ISS Work Areas 1. Bunch train patterns for the acceleration and storage of μ ± beams. 2. A 50Hz, 1.2 MW,
1 Electron Cloud Measurements at the Fermilab Main Injector Bob Zwaska Fermilab ECloud07 Workshop April 9, 2007.
A U.S. Department of Energy Office of Science Laboratory Operated by The University of Chicago Argonne National Laboratory Office of Science U.S. Department.
Fermilab 1 AP Dept. Activities Report September 20, 2006Dixon Bogert AP Dept. - Activities Report Dixon Bogert - AP Dept. Meeting September 20 th, 2006.
3 GeV,1.2 MW, Booster for Proton Driver G H Rees, RAL.
Proton Plans at Fermilab Robert Zwaska - Fermilab Science and Engineering at Henderson- DUSEL Capstone Workshop Stony Brook University May 5, 2006 Outline.
SNuMI: Phase I & Phase II Nancy Grossman Phase I: $33.4M FY06$ (no contingency, no G&A) 41% contingency Phase II: $53.7M FY06$ (no contingency, no G&A)
F MI High Power Operation and Future Plans Ioanis Kourbanis (presented by Bruce Brown) HB2008 August 25, 2008.
Antiproton Source Capabilities and Issues Keith Gollwitzer & Valeri Lebedev Accelerator Division Fermilab 1.
Brookhaven Science Associates U.S. Department of Energy AGS Upgrade and Super Neutrino Beam DOE Annual HEP Program Review April 27-28, 2005 Derek I. Lowenstein.
INTRODUCTION  RECYCLER BPM – Original system not adequate to measure beam position precisely. It is being upgraded to meet the required physics precision.
Proton Driver: Status and Plans C.R. Prior ASTeC Intense Beams Group, Rutherford Appleton Laboratory.
AAC February 4-6, 2003 Protons on Target Ioanis Kourbanis MI/Beams.
F Overview of the SuperNuMI Plan A. Marchionni, Fermilab AD/MID Accelerator Advisory Committee, May 10-12, 2006.
F Project X Overview Dave McGinnis October 12, 2007.
Proton Study Meeting 4/19/05 Eric Prebys 1 Proton Plan Stage I Eric Prebys.
Recent RF Development at Fermilab Weiren Chou and Akira Takagi Fermilab, U.S.A. July 7, 2003 Presentation to the FFAG03 Workshop July 7-12, 2003, KEK.
F Project-X Related Issues in Recycler A.Burov, C.Gattuso, V.Lebedev, A.Leveling, A.Valishev, L.Vorobiev Fermilab AAC Review 8/8/2007.
F 1 MW Proton Beam for Neutrinos Dave McGinnis AAC Meeting May 10, 2006.
F Proton Plan Eric Prebys, FNAL Accelerator Division.
Overview of Booster PIP II upgrades and plans C.Y. Tan for Proton Source group PIP II Collaboration Meeting 03 June 2014.
Accelerator Issues Fermilab Antiproton Experiment Keith Gollwitzer Antiproton Source Department Accelerator Division Fermilab.
Mu2e, August 15, 2007 E Prebys 1 The Steering Group and mu2e Eric Prebys.
Accumulator Stacktail Cooling Paul Derwent December 18, 2015.
Fermilab Proton Driver and Muons David Johnson Fermilab Neutrino Factory Muon Collider Collaboration Meeting March 14, 2006.
Overview of the Project X RD&D Plan Sergei Nagaitsev AAC Meeting February 3, 2009.
F All Experimenters' Mtg - 2 Jun 03 Weeks in Review: 05/19/03 –06/02/03 Keith Gollwitzer – FNAL Stores and Operations Summary Standard Plots.
Fermilab 1 SNUMI Civil Issues September 18, 2006Dixon Bogert SNUMI Civil Design & Site Considerations; Issues and FESS work Dixon Bogert SNUMI Meeting,
Updated Overview of Run II Upgrade Plan Beam Instrumentation Bob Webber Run II Luminosity Upgrade Review February 2004.
Proton Intensity Upgrades  Present operation of Main Injector and NuMI  NuMI designed for 400 kW, achieved a max beam power of 270 kW  Present Proton.
Early Beam Injection in the Fermilab Booster & its Implementation Plan Chandra Bhat Todd’s Operation Meeting /12/2015 Chandra Bhat Abstract:
Doug Michael Sep. 16, GeV protons 1.9 second cycle time 4x10 13 protons/pulse 0.4 MW! Single turn extraction (10  s) 4x10 20 protons/year 700.
Proton Plan Expectations Eric Prebys AD/Proton Source.
 A model of beam line built with G4Beamline (scripting tool for GEANT4)  Simulated performance downstream of the AC Dipole for core of beam using  x.
Status of the Accelerator Complex Keith Gollwitzer Antiproton Source Accelerator Division Fermilab 2009 Fermilab Users’ Meeting.
SNuMI: WBS 1.1 Booster Upgrades Eric Prebys $642K FY06$ (no contingency, no G&A) xx% contingency Main Injector & Recycler BNB NuMI Tunnel Booster Ring.
F A Fermilab Roadmap Dave McGinnis May 28, f Fermilab Roadmap - McGinnis Timelines  Divide the road map into three parallel paths  ILC - Energy.
Barrier RF Stacking Weiren Chou and Dave Wildman Fermilab, U.S.A. October 20, 2004 Presentation at the Proton Driver Session ICFA-HB2004, Bensheim, Germany,
Early Beam Injection Scheme for the Fermilab Booster: A Path for Intensity Upgrade Chandra Bhat Fermi National Accelerator Laboratory DPF2015, ANN ARBOR,
Status of Project X Keith Gollwitzer Accelerator Division Fermilab MAP Winter Meeting - March 1, 2011.
F Possible Proton Capabilities at Fermilab Dave McGinnis April 16, 2007.
Robert R. Wilson Prize Talk John Peoples April APS Meeting: February 14,
Beam time structures 1 At any particular instance of time there will be only one kind of beam in the MI. It will be either protons or anti-protons. The.
NuFACT06 Muon Source at Fermilab David Neuffer Fermilab.
LER Workshop, Oct 11, 2006Intensity Increase in the LER – T. Sen1 LHC Accelerator Research Program bnl-fnal-lbnl-slac  Motivation  Slip stacking in the.
Run II Status Keith Gollwitzer Temple Review July 1, 2003.
Proton Drivers & Muon Sources at Fermilab David Neuffer Fermilab.
Steering Group Meeting 10:30 – 12:30 am CDT Monday, July 23, 2007 Y2K.
Limitations to Total Booster Flux Total protons per batch: 4E12 with decent beam loss, 5E12 max. Average rep rate of the machine: –Injection bump magnets.
F Project X: Recycler 8.9 GeV/c Extraction D. Johnson, E. Prebys, M. Martens, J. Johnstone Fermilab Accelerator Advisory Committee August 8, 2007 D. Johnson.
MI/RR Operation Status Ioanis Kourbanis August 21, 2014.
Overview of Project X ICD and RD&D Plans David Neuffer material from Paul Derwent & Sergei Nagaitsev (AAC Meeting, February 3, 2009)
Proton Driver Keith Gollwitzer Accelerator Division Fermilab MAP Collaboration Meeting June 20, 2013.
Proton Source Reference Notes for mu2e at Fermilab 1 Section 1: Compilation of parameters describing the existing Fermilab accelerator complex and the.
Proton Plan 1/10/07 E Prebys 1 Proton Plan Meeting Agenda:  Project/campaign reorganization: Prebys  Status updates: all  Booster Water Proposal: Cooper.
F Sergei Nagaitsev (FNAL) Aug Project X ICD2 Briefing.
HP-PS beam acceleration and machine circumference A.LachaizeLAGUNA-LBNO General meeting Paris 18/09/13 On behalf of HP-PS design team.
8 GeV Linac (Project X) and mu2e Chuck Ankenbrandt Fermilab Mu2e Collaboration Meeting August 1, 2007 My Preferred title: Linac & Recycler & Accumulator.
Jeffrey Eldred, Sasha Valishev AAC Workshop 2016
A. Al-khateeb, O. Chorniy, R. Hasse, V. Kornilov, O. Boine-F
JLEIC Ion Integration Goals
Presentation transcript:

SNuMI (>1MW) SNuMI 1 Motivations for SNuMI The neutrino experimental program for the next decade –NOνA (long baseline νμ→νe search) –MINERνA (Main Injector ν-A interactions) –Liquid Argonne detector? NOvA largely statistics limited – comparing 6 full years (44 weeks) –1.2MW should improve sensitivities by 30% versus 700kW –A liquid Ar detector would greatly benefit from a 1.2MW beam –If unexpected signals/results, then 1.2MW could be a bigger benefit – won’t know for a while though

SNuMI (>1MW) SNuMI 2 SNuMI Concepts Use the Accumulator in the Anti-proton Source as a proton ring: –After acceleration in the Booster, beam transferred to the Accumulator –Accumulator was designed for momentum stacking Momentum stack 3 Booster batches (4.7×10 12 p/batch) every 200 ms No need to cog in the Booster when injecting into the Accumulator Longitudinal emittance dilution of ~ 20% instead of ~ 80% as in slip-stacking – Box Car stack in the Recycler Load in a new Accumulator batch every 200 ms Place 6 Accumulator batches sequentially around the Recycler – Load the Main Injector in a single turn – 8.3×10 13 ppp in MI every s  1.2 MW

SNuMI (>1MW) SNuMI 3 Operating Scenarios * NuMI values are given for mixed-mode cycles * *

SNuMI (>1MW) SNuMI 4 AP-4 Line (may not need) AP-5 Line Original SNuMI Connections Euclid: “The shortest distance between two points is a straight line.”

SNuMI (>1MW) SNuMI 5 “B->R->AS” Proposal Booster to Recycler to Antiproton Source (accumulator/debuncher) “B->R->AS” – (suggest BRAD instead) Transporting 8-GeV protons from the Booster via the Recycler to the Antiproton Source (Chuck Ankenbrandt et. al.) “A way to deliver 8-GeV protons from the Booster to the Antiproton Source via existing enclosures and beam lines is described. By using the existing 8-GeV line and most of the Recycler as parts of the beam path, the scheme avoids the need for new civil construction and new beam transport lines. In this way, as soon as the Tevatron Collider era is over, the Antiproton Source can be rapidly transformed into a very useful pair of proton storage rings for various applications.”

SNuMI (>1MW) SNuMI 6 Proposed B->R->AS Path (for Mu2e experiment, plus others?) B->R->AS: Commissioning of momentum staking in the Accumulator Motivate mitigation of radiation issues in the Accumulator. Modifications for SNuMI era: AP-5 line or equivalent will still be needed Need a fast extraction system for Recycler to P150 line. Only two “free” Booster batches will remain for other programs. Eliminate the need for the AP-4 line? AP-5 line

SNuMI (>1MW) SNuMI 7 Responses to Director’s Review Recommendations about SNuMI (8) We recommend that emittance growth at transition as a function of beam brightness be re-examined in light of the Phase II requirements. If machine studies can be done with relevant bunch parameters then they should be given high priority. Extensive simulations of transition crossing in MI were performed for bunch intensities of 1.0E11 (Phase I, now NOvA), 1.8E1; (Phase II, now SNuMI) and different longitudinal emittances Without a gamma-t jump and intensities of 1.0E11 per bunch the maximum longitudinal emittance that can be accelerated through transition is 0.4 eV- sec. For intensities of 1.8E11 the maximum longitudinal emittance that can accelerated trough transition is limited to 0.3 eV-sec. By using a gamma-t jump we can accelerate trough transition longitudinal emittances up to 0.6 eV-sec with minimal emittance growth. The use of a longitudinal quad damper can greatly reduce the emittance growth during the transition crossing. See ProtonPlan2-doc-136-v1

SNuMI (>1MW) SNuMI 8 Responses to Director’s Review Recommendations about SNuMI (21) More detailed calculations will be needed to better understand the beam losses in advance of the full development of the Phase II design. Booster to Recycler to Antiproton Source (accumulator/debuncher) “B->R->AS” proposal would help in this area. (22)The project should consider a study of the possible use of collimation and local shielding inside the Accumulator beam enclosure to better control the prompt radiation hazard passively. B->R->AS proposal would help in this area.

SNuMI (>1MW) SNuMI 9 Responses to Director’s Review Recommendations about SNuMI (38) Study alternative stacking schemes that are less sensitive to beam instabilities and have better efficiency. Unfortunately we do not know of any stacking scheme that is both less sensitive to instabilities and has better stacking efficiency. The possibility of using slip-stacking to stack 18 Booster batches in the Recycler was investigated. See “Using Slip Stacking for SNuMI” by I. Kourbanis ProtonPlan-doc-272. We also doing experimenting with fast barrier bucket stacking in MI.

SNuMI (>1MW) SNuMI 10 Responses to Director’s Review Recommendations about SNuMI (37) Estimate the beam loss instability thresholds during the beam stacking processes, in particular during debunching and rebunching of the high intensity beam in the Accumulator and the Recycler, with simulations and/or beam studies. Currently we can routinely achieve Accumulator intensities of 1E12 and 15 eV-sec with no sign of instabilities. For SNuMI (>1MW) most of the Accumulator impedance sources will be removed (stochastic cooling arrays, 2.5MHz and 1.2MHz cavities) and the 53MHz impedance will be reduced by a factor of 20 with rf feedback. The debunching in the Recycler can be avoided. The impedance threshold required for self-bunching in the Accumulator was studied. See “Self-Bunching of a Coasting Beam in the Accumulator” by D. McGinnis ProtonPlan-doc-198.

SNuMI (>1MW) SNuMI 11 Conclusion Momentum Stacking in the Accumulator Paper: –“For the projected SNUMI intensity of 14.1x10 12 particles in the Accumulator at a 95% momentum spread of 15.9MeV, and an RF feedback gain of 14dB, the beam should be stable with a factor of two margin. This result can be tested by cooling 100mA of antiproton beam on the stacking lattice (h=0.10) to a frequency width of 7.9 Hz.” B->R->AS would enable commissioning of momentum stacking in the Accumulator and perhaps eliminate need for AP4 line construction The steering committee needs to consider SNuMI as part of the lab’s long term plan If the lab plans to do SNuMI, it is a large commitment It is imperative that the laboratory make a decision one way or the other within the next year, given the timescale and size of the project

SNuMI (>1MW) SNuMI 12 Backup of schedule – very rough…. Comparison to timeline shown at November 2006 Director’s Review for SNuMI Ph II: This schedule shows end of conceptual design in F08 (CD-1 complete), then 5 years to operations Prior slide shows construction funds available FY11, which combined with Nov 06 timeline puts start of operations in 2014 Prior slide also shows very compressed and optimistic construction period, likely unrealistic Shift of completion due to when prior slide shows construction funds are available