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Linac Beams for Fixed Target Experiments Presentation by Roger Erickson SLAC Operations Review SLAC, June 15-16, 2004
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06/16/04 Accelerator Operations Review Outline Linac and sources Interleaved beams A-Line and End Station A (ESA) Final Focus Test Beam (FFTB) Secondary Test Beams Summary
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06/16/04 Accelerator Operations Review Linac Beam Lines LCLS will add an electron injector downstream of the positron source. Fixed target experiments can be carried out in End Station A (ESA) or the Final Focus Test Beam (FFTB) facility.
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06/16/04 Accelerator Operations Review The Two-mile Linac 50 GeV Linac with multiple pulsed extraction points. 120 pulses per second max; now running 30. Up to 6e11 electrons per pulse. Polarized electrons available up to full intensity. 4e10 positrons per pulse, interleaved with electron pulses. Long pulses (undamped) or short pulses (damped). Typically running two programs simultaneously: PEP-II Fixed target in ESA or FFTB Flexibility for interleaved beams: e+, e-, damped and undamped, different energies, intensities and rates.
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06/16/04 Accelerator Operations Review Typical (Recent) Running Mode Linac runs well at 30 pulses/sec (half the ac line frequency). 9 GeV electrons to HER: on demand for trickling, up to 10 Hz. 3.1 GeV positrons to LER: on demand for trickling, up to 10 Hz. 28.5 GeV “scavenger” electrons to Sector 19 (to make more positrons for the next cycle). 28.5 GeV electrons to FFTB: 10 Hz for fixed target programs (interleaved with PEP injection pulses). At the push of a button, Electrons and Positrons to PEP-II for rapid filling at 15 Hz each (with no rate to FFTB).
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06/16/04 Accelerator Operations Review Research Yard Experimental Facilities ESA FFTB
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06/16/04 Accelerator Operations Review A-Line to ESA SLAC’s original experimental hall, site of parton discovery and parity violation in eP scattering. Recent E-158 success: first observation of parity violation in polarized e-e- Moller scattering. E-158 had three production runs at 120 Hz in 2002-2003; once with PEP-II and twice alone. High power (500 kW) beam capability. ESA is convenient for staging fixed target experiments Large, massively shielded building. Power, LCW, and cryogenic facilities. Easy truck access. Crane coverage. Counting house with DAQ facilities. Strong bends and weak focusing preclude “FFTB beams” with small emittance and compressed bunch length.
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06/16/04 Accelerator Operations Review Energy dithering region BPM ~2 microns energy ~1 MeV Agreement (MeV) BPM24 X (MeV) BPM12 X (MeV) toroid ~30 ppm A-Line Beam Monitoring Devices
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06/16/04 Accelerator Operations Review ParameterE-158NLC-500 Charge/Train5 x 10 11 14.4 x 10 11 Repetition Rate120 Hz Energy45 GeV250 GeV e - Polarization85% Train Length270ns267ns Microbunch spacing0.3ns1.4ns Beam Loading13%22% Energy Spread0.15%0.16% E-158 Beam Comparison with 500 GeV Linear Collider Design.
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06/16/04 Accelerator Operations Review End Station A Photo Shows E-158 Spectrometer Magnets.
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06/16/04 Accelerator Operations Review Pending Programs in ESA Calibration of GLAST detector components with secondary hadrons (to be scheduled to accommodate GLAST requirements). A Letter of Intent submitted to the EPAC: Beam Instrumentation Tests for the Linear Collider using the SLAC A-Line and End Station A
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06/16/04 Accelerator Operations Review Final Focus Test Beam The FFTB was originally built to demonstrate technology for focusing and measuring sub-micron electron beams suitable for a future linear collider. Recent on-going programs include: Plasma Wakefield Acceleration – a series of experiments that have recently demonstrated high-gradient acceleration in a lithium plasma. SPPS – A new facility that uses compressed electron bunches to generate intense x-ray pulses. Technology applicable to the LCLS: Extreme bunch compression. Beam control and feedback for stability. Instrumentation for characterizing extremely short x-ray pulses.
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06/16/04 Accelerator Operations Review FFTB Experimental Area
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06/16/04 Accelerator Operations Review RTL DAMPING RING SLAC LINAC 9 ps0.4 ps 50 ps 1 GeV28.5 GeV 14-meter chicane compressor in linac at 1/3 point (9 GeV) CHICANE BENDING MAGNETS LONGER PATH TAKEN BY HEAD OF THE BUNCH Energy e- Energy Time ELECTRON BUNCH WITH HIGHER ENERGY TAIL TAIL BEGINS TO CATCH UP FULLY COMPRESSED FFTB Short Bunches in FFTB
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06/16/04 Accelerator Operations Review Plasma Wakefield Acceleration e-e- N=1.8 10 10 z =20-12µm E=28.5 GeV Optical Transition Radiators Li Plasma Gas Cell: H 2, Xe, NO n e ≈0-10 18 cm -3 L≈2.5-20 cm Plasma light X-Ray Diagnostic, e-/e + Production Cherenkov Radiator Dump ∫Cdt Imaging Spectrometer Energy Spectrum “X-ray” 25m Coherent Transition Radiation and Interferometer 0+5-5 n e =2.5x10 17 No Plasma Gain Loss 0+5-5 7.9 GeV ≈3 GeV! n e =2.5x10 17 0+5-5 Pyro=48 4 0+5 -5 +1.5 GeV n e =3.5x10 17 No Plasma Min. Gain Min. Loss 0+5-5 Relative Energy (GeV)
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06/16/04 Accelerator Operations Review SPPS in FFTB
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06/16/04 Accelerator Operations Review Photon beam line Electron beam line Experimental Area Beam dump FFTB Dump Line Experimental Area
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06/16/04 Accelerator Operations Review Pending Programs in FFTB SPPS Ongoing program of technology development involving extremely short x- ray pulses. Plasma Wakefield Acceleration Ongoing program to develop exotic new methods for achieving very high accelerating gradients, strong plasma focusing, and related technology. Experiment E-165 Flourescence in Air from Showers (FLASH) A continuing program to quantitatively understand the production of light by cosmic rays in the upper amosphere, using controlled laboratory conditions. Experiment E166 A Proposal to Test Production of Polarized Positrons with the SLAC 50-GeV Beam in the FFTB An undulator-based technique applicable to a future linear collider.
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06/16/04 Accelerator Operations Review Test Beam Facilities Primary electron or positron beams to ESA or FFTB. Secondary electron or positron beams to ESA or FFTB. Produced by double conversion (e- to gammas to e+ or e-). One or a few particles/pulse. Energy easily selectable with transport line magnets. Secondary hadron beam to ESA. Primary electrons to beryllium target near end of linac. Secondary particles scattered at 0.5 deg into A-Line. Positrons, pions, kaons, and protons tagged with time-of-flight and Cerenkov detectors. One tagged particle/pulse was delivered to GLAST detector development test.
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06/16/04 Accelerator Operations Review Test Beam Scheduling The approval and scheduling process is designed to minimize effort for outside users and minimize cost and impact for SLAC. Proposals are submitted to Experimental Facilities Department. EFD staff provide technical and administrative support for users. “Test Request” summary is circulated to: Radiation physicist Chairman, Safety Oversight Committee FFTB (or ESA) Area Manager Accelerator Department physicist Research Division Program Coordinator Test Request is submitted to Accelerator Department Operations Section for scheduling. Beam Authorization Sheet is prepared by Radiation Physics Department. Most test beam experiments are carried out with no significant adverse impact on other programs. Many are done in 1 to 3 days.
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06/16/04 Accelerator Operations Review Test Beam Experiments in FFTB T-447Single Pulse Damage in Materials (Sept 2000) T-448Magnified Optical Transition Radiation Test (Oct 2000) T-450Damage Test in Diamond for LCLS (Oct 2000) T-451High Energy Neutron Spectra Measurement (March 2001) T-452STAR Endcap Calorimeter Detector Prototype Test (Jan 2001) T-453Radiation Damage in Diamond for LCLS (April 2001) T-454Measurement of Neutron Spectra (June 2001) T-455Measurement of the Calorimeter for the Local Polarimeter at Phenix/RHIC (Aug 2001) T-456Magnetization Dynamics in Magnetic Films (Sept 2001) T-457Measurement of Neutron Energy Spectra Using Bonner Multi-Sphere Spectrometer (June 2002) T-460Characterization of Askaryan Effect in Rock Salt (June 2002) T-461 High Atmosphere Air Fluorescence (June 2002) T-462 Magnetization Dynamics of Soft-Magnetic Films (June 2002) T-464 Correlation of Linac Transverse Deflection Cavity with FFTB Streak Camera (June 2002) T-465 Magnetization Dynamics in the Sub-picosecond Time Scale (May 2003) T-466 UCLA Electromagnetic Calorimeter (EMC) Prototype (May 2003) T-467Measurement of FFTB Backgrounds for E166 (Jan 2004) T-468Diamond Detector Response (July 2003) Experiments not yet run: T-469DIRC R&D Program T-470DASH: Diamond Detectors for FLASH T-471Incoherent Radio Emission from Showers
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06/16/04 Accelerator Operations Review Conclusions Extra linac pulses, not needed for PEP-II injection, can be delivered to End Station A or the FFTB facility for use by fixed target or “test beam” experiments. We have seen a constant demand for these beams from a wide variety of users. Small experiments can be set up and run with no adverse impact on the PEP-II program and with very little additional cost to SLAC. Significant new physics results have been achieved, and a large number of detector technology development tests have been carried out. The FFTB will be dismantled in 2006 to make room for the Linac Coherent Light Source (LCLS). We are exploring possible replacement options. The requests for test beams keep coming!
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