Paper | Title | Other Keywords | Page |
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MOZBA2 | Operational Experience with Superconducting Undulators at APS | operation, undulator, photon, vacuum | 57 |
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Funding: Work supported by U. S. Department of Energy, Office of Science, under Contract No. DE-AC02-06CH11357. APS has been developing superconducting undulators for over a decade. Presently, two planar and one helical device are in operation in the APS storage ring, and a number of devices will be installed in the APS Upgrade ring. All superconducting devices perform with very high reliability and have very minor effect on the storage ring operation. To achieve this, a number of storage ring modifications had to be done, such as introduction of the beam abort system to eliminate device quenches during beam dumps, and lattice and orbit modifications to allow for installation of the small horizontal aperture helical device with magnet coils in the plane of synchrotron radiation. |
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Slides MOZBA2 [3.424 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-MOZBA2 | ||
About • | paper received ※ 02 September 2019 paper accepted ※ 19 November 2019 issue date ※ 08 October 2019 | ||
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MOZBB2 | Experiments with Metamaterial-Based Metallic Accelerating Structures | experiment, wakefield, acceleration, GUI | 78 |
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Funding: U.S. Department of Energy, Office of Science, Office of High Energy Physics under Award No. DE-SC0015566 at MIT and No. DE-AC02-06CH11357 at ANL We present experimental studies of metamaterial (MTM) structures for wakefield acceleration. The MTM structure is an all-metal periodic structure with its period much smaller than the wavelength at X-band. The fundamental TM mode has a negative group velocity, so an electron beam traveling through the structure radiates by reversed Cherenkov radiation. Two experiments have been completed at the Argonne Wakefield Accelerator (AWA), namely the Stage-I and Stage-II experiments. Differences between the two experiments include: (1) Structure length (Stage-I 8 cm, Stage-II 20 cm); (2) Bunch number used to excite the structure (Stage-I up to 2 bunches, Stage-II up to 8 bunches). In the Stage-I experiment, two bunches with a total charge of 85 nC generated 80 MW of RF power in a 2 ns long pulse. In the Stage-II experiment, the highest peak power reached 380 MW in a 10 ns long pulse from a train of 8 bunches with a total charge of 224 nC. Acceleration of a witness bunch has not been demonstrated yet, but the extracted power can be transferred to a separate accelerator for two-beam acceleration or directly applied to a trailing witness bunch in the same structure for collinear acceleration. |
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Slides MOZBB2 [8.172 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-MOZBB2 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 04 September 2019 issue date ※ 08 October 2019 | ||
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MOPLM16 | Design of a 200 kV DC Cryocooled Photoemission Gun for Photocathode Investigations | cathode, gun, electron, emittance | 136 |
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Funding: This work was supported by the U.S. National Science Foundation under Award No. PHY-1549132, the Center for Bright Beams. Intrinsic emittance of photocathodes limits the brightness of electrons beams produced from photoemission guns. Recent advancements have shown that an order of magnitude improvement in intrinsic emittance over the commonly used polycrystalline metal and semiconductor cathodes is possible via use of single crystalline ordered surfaces of metals, semiconductors and other exotic materials at cryogenic temperatures as cathodes. However, due to practical design considerations, it is not trivial to test such cathodes in existing electron guns. Here we present the design of a 200kV DC electron gun being developed at the Arizona State University for this purpose. |
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Poster MOPLM16 [1.549 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-MOPLM16 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 12 September 2019 issue date ※ 08 October 2019 | ||
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MOPLS01 | Spectroscopic Correlations to Resistive Switching of Ion Beam Irradiated Films | ECR, experiment, scattering, laser | 160 |
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Researchers concentrated on resistive random access memories (RRAMs) due to excellent scalability, high integration density, quick switching, etc*,**. Intrinsic physical phenomenon of RRAMs is resistive switching. In this work, ion beam irradiation was used as a tool to modify resistive switching of pulsed laser deposited (PLD) Y0.95Ca0.05MnO3/Si films. Ion irradiation induced optimal resistive switching with spectroscopic correlations has been attributed to oxygen vacancy gradient. Resistive switching ratio is estimated to be increased for the film irradiated with fluence 1×1011 ions/cm2 due to irradiation induced strain and oxygen vacancies verified by X’ray diffraction (XRD), Raman, atomic force microscopy (AFM), Rutherford backscattering spectrometry (RBS) and near-edge X-ray absorption fine structure (NEXAFS) measurements. Strain relaxation and oxygen vacancy annihilation have been realized for higher fluence (1×1012 and 1×1013 ions/cm2) owing to local annealing effect. Present study suggests that the films understudy can be considered as emerging candidates for RRAMs.
* X.J. Zhu et al., Front. Mater. Sci. 6 (2012) 183, 206. ** D.S. Jeong et al., Rep. Prog. Phys. 75 (2012) 076502:1,31. |
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Poster MOPLS01 [0.745 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-MOPLS01 | ||
About • | paper received ※ 26 August 2019 paper accepted ※ 16 November 2020 issue date ※ 08 October 2019 | ||
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MOPLS09 | Engineering Design of Gallium-Nickel Target in Niobium Capsule, with a Major Focus on Determining the Thermal Properties of Gallium-Nickel Through Thermal Testing and FEA, for Irradiation at BLIP | target, proton, niobium, experiment | 170 |
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Funding: Funding:This abstract is authored by BSA operated under contract number DE-SC0012704. This research is supported by the U.S. DOE Isotope Program, managed by the Office of Science for Nuclear Physics. The Brookhaven Linac Isotope Producer (BLIP) produces several radioisotopes using a variable energy and current proton beam. The targets irradiated at BLIP are cooled by water and required to be isolated in a target capsule. During the design stage, thermal analysis of the target and cladding is carried out to determine the maximum beam power a target can handle during irradiation without destruction. In this work we designed a capsule for Gallium-Nickel (Ga 80%, Ni 20%) alloy target material and irradiated the target at the BLIP to produce the radioisotope Ge-68. Since no literature data is available on Ga4Ni’s thermal conductivity (K) and specific heat (C), measurements were carried out using thermal testing in conjunction with Finite Element Analysis (FEA). Steady-state one dimensional heat conduction method was used to determine the thermal conductivity. Transient method was used to calculate the specific heat. The test setup with same methodologies can be used to assess other targets in the future. Here, we will detail these studies and discuss the improved design and fabrication of this target. |
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Poster MOPLS09 [0.751 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-MOPLS09 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 03 September 2019 issue date ※ 08 October 2019 | ||
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TUXBA3 | Robust Thermoacoustic Range Verification for Pulsed Ion Beam Therapy | proton, target, simulation, experiment | 294 |
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Funding: * Supported by the U.S D.O.E., Office of Nuclear Physics, under Contract No. DE-AC02-06CH11357. Measurements were performed at ANL’s ATLAS facility, which is a DOE Office of Science User Facility. Lack of online range verification generally limits application of proton therapy to cancers in the brain, spine, and to pediatric patients. Previously, thermoacoustic range verification (TARV) has been demonstrated in weakly scattering media with known sound speed [1]. At ATLAS, we demonstrated the accuracy and robustness of TARV relative to ultrasound (US) images despite acoustic heterogeneity and sound speed errors representing in vivo conditions [2]. 250 ns pulses deposited 0.26 Gy of 16 MeV protons and 2.3 Gy of 60 MeV helium ions into liquid targets. TA signals were detected by an US array that also generated US images. An air gap phantom displaced the Bragg peak by 6.5 mm and the scanner’s propagation speed setting was altered by ±5%. Weak and strong scatterers were placed between the Bragg peak and US array. Estimated Bragg peak locations were translated 6.5 mm by the air gap phantom and agreed with TRIM simulations to within 0.3 mm, even when TA emissions traveled through a strong acoustic scatterer. Soundspeed errors dilated, and acoustic heterogeneities deformed both US images and TA range estimates, confirming that TARV is accurate relative to US images. [1] Hickling, et al, Med Phys, 45(7), 2018. (review article) [2] S. Patch, D. Santiago, & B. Mustapha, Med Phys, 46(1), 2019. |
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Slides TUXBA3 [4.449 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUXBA3 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 31 August 2019 issue date ※ 08 October 2019 | ||
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TUYBB5 | Design and Analysis of a Halo-Measurement Diagnostics | electron, diagnostics, optics, experiment | 322 |
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Funding: This material is based upon work supported by the U.S. Department of Energy, Office of Science, Office of Nuclear physics under contract DE-AC05-06OR23177 and DE-AC02-07CH11359. A large dynamical-range diagnostics (LDRD) design at Jefferson Lab will be used at the FAST-IOTA injector to measure the transverse distribution of halo associated with a high-charge electron beam. One important aspect of this work is to explore the halo distribution when the beam has significant angular momentum (i.e. is magnetized). The beam distribution is measured by recording radiation produced as the beam impinges a YAG:Ce screen. The optical radiation is split with a fraction directed to a charged-couple device (CCD) camera. The other part of the radiation is reflected by a digital micromirror device (DMD) that masks the core of the beam distribution. Combining the images recorded by the two cameras provides a measurement of the transverse distribution with over a large dynamical range. The design and analysis of the optical system will be discussed including optical simulation using SRW and the result of a mockup experiment to test the performances of the system will be presented. |
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Slides TUYBB5 [3.013 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUYBB5 | ||
About • | paper received ※ 02 September 2019 paper accepted ※ 13 September 2019 issue date ※ 08 October 2019 | ||
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TUPLM21 | Optical Stochastic Cooling Program at Fermilab’s Integrable Optics Test Accelerator | experiment, lattice, electron, optics | 418 |
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Funding: Fermi National Accelerator Laboratory is operated by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the United States Department of Energy. Beam cooling enables an increase of peak and average luminosities and significantly expands the discovery potential of colliders. Optical Stochastic Cooling (OSC) is a high-bandwidth cooling technique that will advance the present state-of-the-art, stochastic-cooling rate by more than three orders of magnitude. A proof-of-principle demonstration with protons or heavy ions involves prohibitive costs, risks and technological challenges; however, exploration of OSC with electrons is a cost-effective alternative for studying the beam-cooling physics, optical systems and diagnostics. The ability to demonstrate OSC was a key requirement in the design of Fermilab’s Integrable Optics Test Accelerator (IOTA) ring. The IOTA program will explore the physics and technology of OSC in amplified and non-amplified configurations. We also plan to investigate the cooling and manipulation of a single electron stored in the ring. The OSC apparatus is currently being fabricated, and installation will begin in the fall of 2019. In this contribution, we will describe the IOTA OSC program, the upcoming passive-OSC experimental runs and ongoing preparations for an amplified-OSC experiment |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLM21 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 06 September 2019 issue date ※ 08 October 2019 | ||
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TUPLM24 | Electron Heating by Ions in Cooling Rings | electron, proton, scattering, damping | 426 |
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Hadron beam cooling at high energy is a critical technique for Electron-Ion Colliders (EIC). We consider using an electron storage ring for the EIC at BNL. For such a cooler, the electron beam quality plays an important role since it directly determines the cooling rate. Besides the effects of IBS, space charge and synchrotron damping, which are calculable with well known methods, the heating effect by ions also needs to be carefully considered in electron beam dynamics. In this paper, we present an analytical model to calculate the heating rate by ions and give some example calculations. In addition, this model was benchmarked by applying it on the IBS calculation.
* Work supported by States Department of Energy |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLM24 | ||
About • | paper received ※ 26 August 2019 paper accepted ※ 02 September 2019 issue date ※ 08 October 2019 | ||
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TUPLM26 | Progress Toward a Laser Amplifier for Optical Stochastic Cooling | laser, undulator, experiment, synchrotron-radiation | 434 |
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Optical Stochastic Cooling (OSC) is a method of beam cooling using optical frequencies which compresses the phase space of the beam by correcting the deviation of each particle’s momentum. A particle bunch passing through an undulator produces radiation which is amplified and provides the corrective energy kick. In this project, we are testing a method of amplifying synchrotron radiation (SR) for the eventual use in OSC. The SR is amplified by passing through a highly-doped Chromium:Zinc Selenide (Cr:ZnSe) crystal which is pumped by a Thulium fiber laser. The SR will be produced by one of the bending magnets of the Advanced Photon Source. The first step is to detect and measure the power of SR using a photo-diode. The gain is then determined by measuring the radiation amplified after the single-pass through the crystal. This serves as a preliminary step to investigate the performance of the amplification of beam-induced radiation fields. The planned experiment is an important step towards achieving active OSC in a proof-of-principle demonstration in IOTA. | |||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLM26 | ||
About • | paper received ※ 02 September 2019 paper accepted ※ 13 September 2019 issue date ※ 08 October 2019 | ||
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TUPLS11 | NEG-Coated Copper Vacuum Chambers for the APS-Upgrade Storage Ring Vacuum System | vacuum, storage-ring, photon, operation | 477 |
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Funding: Argonne National Laboratory’s work was supported by the U.S. Department of Energy, Office of Science under contract DE-AC02-06CH11357. The APS-Upgrade (APS-U) storage ring features a diverse group of vacuum chambers including seven distinctive, non-evaporable getter (NEG)-coated copper vacuum chambers per each of the 40 sectors. These chambers feature a 22-millimeter diameter aperture along the electron-beam path, with two vacuum chambers permitting photon extraction through a keyhole-shaped extension to this aperture. The chambers range from 0.3-meters to 1.7-meters in length and fit within the narrow envelope of quadrupole and sextupole magnets. Six of the seven copper vacuum chambers intercept significant heat loads from synchrotron radiation; five of these designs are fabricated entirely from OFS copper extrusions and are equipped with a compact Glidcop® photon absorber. A hybrid vacuum chamber, fabricated from OFS copper extrusion and a copper chromium zirconium (CuCrZr) keyhole transition, also intercepts synchrotron radiation. The seventh vacuum chamber design features a keyhole aperture across its length and is entirely fabricated from CuCrZr. This paper details the careful balance of vacuum chamber functionality, manufacturability, and the overall design process followed to achieve the final designs. |
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Poster TUPLS11 [4.941 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLS11 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 02 September 2019 issue date ※ 08 October 2019 | ||
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TUPLS12 | Final Design of NEG-Coated Aluminum Vacuum Chambers & Stainless Steel Keyhole Vacuum Chambers for the APS-U Storage Ring | vacuum, storage-ring, photon, quadrupole | 480 |
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Funding: Argonne National Laboratory’s work was supported by the U.S. Department of Energy, Office of Science under contract DE-AC02-06CH11357. The APS-Upgrade storage ring features a diverse group of vacuum chambers which includes eight NEG (non-evaporable getter) coated aluminum chambers and two copper coated stainless steel keyhole-shaped chambers per sector (40 total). Each chamber contains a 22 mm diameter electron beam aperture; the keyhole chambers also include a photon extraction antechamber. The chambers vary in length of approximately 289 ’ 792 mm and fit within the narrow envelope of quadrupole and sextupole magnets. Each design is a balance of functionality, manufacturability, and installation space. An innovative CAD skeleton model system and ray tracing layout accurately determined synchrotron radiation heat loads on built-in photon absorbers and the internal envelope of the keyhole antechamber. Chamber designs were optimized using thermal-structural FEA for operating and bakeout conditions. The group of chambers require complex manufacturing processes including EDM, explosion-bonded metals, furnace brazing, and welding with minimal space. This paper describes the design process and manufacturing plan for these vacuum chambers including details about FEA, fabrication plans, and cooling/bakeout strategies. |
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Poster TUPLS12 [2.581 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLS12 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 02 September 2019 issue date ※ 08 October 2019 | ||
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TUPLE05 | Optical System for Observation of FRIB Target | target, shielding, vacuum, neutron | 570 |
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Funding: Work supported by the U.S. Department of Energy Office of Science under Cooperative Agreement DE-SC0000661. Facility for Rare Isotope Beams (FRIB) is a next-generation rare-isotope research facility under construction at Michigan State University (MSU). FRIB will produce rare-isotope beams of unprecedented intensities by impinging a 400 kW heavy-ion beam on a production target and by collecting and purifying the rare isotopes of interest with a fragment separator. A thermal imaging system (TIS) has been developed to monitor the beam spot on the production target. The main features and characteristics of optical system is presented. The prototype of optical system has been tested. |
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Poster TUPLE05 [1.840 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLE05 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 06 November 2020 issue date ※ 08 October 2019 | ||
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TUPLE11 | Proposed Enhanced Imaging Station in the 6-GeV Booster-to-Storage Ring Transport Line for APS Upgrade | booster, emittance, linac, electron | 583 |
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Funding: This manuscript has been authored by FRA, LLC under Contract No.DE-AC02-07CH11359 with the U.S.DoE, Office of HEP. Work supported by U.S.DoE, Office of Science, under Contract No.DE-AC02-06CH11357. One of the challenges of the injector for the Advanced Photon Source Upgrade (APS-U) is the measurement and monitoring of the required high charge electron beam at 6 GeV between the Booster synchrotron and the storage ring in the transport line (BTS. In APS-U charges of up to 17 nC per micropulse are specified with a beam geometrical horizontal emittance of 60 nm rad. Vertical beam sizes at the imaging station of ~80 µm (σ) are expected so system resolutions of <30 µm are warranted. A phased approach to enhance the imaging station performance has been initiated. Recently, the 20-year-old Chromox screen oriented at 45 degrees to the beam was replaced by a 100-micron thick YAG:Ce screen which gave an improved screen resolution of <10 micron(σ. However, the optical magnification of the system still needs to be increased. In addition, the high areal charge densities are expected to exceed the scintillator mechanism’s saturation threshold so an optical transition radiation (OTR) screen will be added to the station for high-charge studies. A final phase would be the use of optical diffraction radiation (ODR) as a non-intercepting, beam-size monitor during top-up injections. |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-TUPLE11 | ||
About • | paper received ※ 22 August 2019 paper accepted ※ 02 September 2019 issue date ※ 08 October 2019 | ||
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WEXBA2 | Recent Results and Opportunities at the IOTA Facility | electron, experiment, undulator, proton | 599 |
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The Integrable Optics Test Accelerator (IOTA) was recently commissioned as part of the Fermilab Accelerator Science and Technology (FAST) facility. The IOTA ring was briefly operated with electrons at 47 MeV followed by a 6-months run with 100 MeV electrons. The main goal of the first run was to study beam dynamics in the integrable lattices with elliptical nonlinear magnets and in the quasi-integrable case with profiled octupole channel. The flexibility of the IOTA ring allowed a wide range of complementary studies, such as experiments with a single electron; studies of fluctuations in undulator radiation and operation with low emittance beams. Over the next year the proton injector will be installed and two runs carried out. One run will be dedicated to the refinement of nonlinear experiments and another will be dedicated to the proof-of-principle demonstration of Optical Stochastic Cooling. | |||
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Slides WEXBA2 [12.702 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEXBA2 | ||
About • | paper received ※ 31 August 2019 paper accepted ※ 05 September 2019 issue date ※ 08 October 2019 | ||
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WEXBA3 | CSR Phase Space Dilution in CBETA | simulation, linac, lattice, shielding | 605 |
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CBETA, the Cornell BNL ERL Test Accelerator, will be the first multi-turn Energy Recovery Linac (ERL) with SRF accelerating cavities and Fixed Field Alternating gradient (FFA) beamline. While CBETA gives promise to deliver unprecedentedly high beam current with simultaneously small emittance, Coherent Synchrotron Radiation (CSR) can pose detrimental effect on the beam at high bunch charges and short bunch lengths. To investigate the CSR effects on CBETA, we used the established simulation code Bmad to track a bunch with different parameters. We found that CSR causes phase space dilution, and the effect becomes more significant as the bunch charge and recirculation pass increase. Potential ways to mitigate the effect involving varying phase advances are being investigated. | |||
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Slides WEXBA3 [6.121 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEXBA3 | ||
About • | paper received ※ 28 August 2019 paper accepted ※ 15 September 2019 issue date ※ 08 October 2019 | ||
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WEYBB6 | Design Considerations and Operational Features of the Collimators for the Fermilab Main Injector and Recycler | collimation, proton, controls, operation | 642 |
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Funding: This manuscript has been authored by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the U.S. Department of Energy, Office of Science, Office of High Energy Physics. The Fermilab Main Injector system delivers 700 kW of 120 GeV Proton beam for neutrino experiments. Since 2013 this has been achieved using slip stacking accumulation in the Recycler with up to 12 batches from the Fermilab Booster per Main Injector Ramp Cycle. To control activation from beam loss, collimation systems in the Booster to Recycler transfer line, in the Recycler and in the Main Injector are employed. Residual radiation measurements around the ring with detailed studies at the collimators are required to maintain adequate loss control. We will review design considerations, operational parameters and activation results for more than ten years of operation. Simulations with MARS15 are used to explore the activation rates and the isotopic composition of the resulting activation. |
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Slides WEYBB6 [12.713 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEYBB6 | ||
About • | paper received ※ 30 August 2019 paper accepted ※ 04 September 2019 issue date ※ 08 October 2019 | ||
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WEPLM02 | Finding Beam Loss Locations in a Linac with Oscillating Dipole Correctors | linac, dipole, DTL, betatron | 663 |
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Funding: This manuscript has been authored by Fermi Research Alliance, LLC under Contract No. DE-AC02-07CH11359 with the U.S. Department of Energy, Office of Science, Office of High Energy Physics The paper proposes a method of finding the beam loss locations in a linac. If the beam is scraped at an aperture limitation, moving its centroid with two dipole correctors located upstream and oscillating in sync produces a line at the corresponding frequency in spectra of current-sensitive devices downstream of the loss point. The phase of this signal contains information about the location of the beam loss. Similar lines appear also in the position signals of Beam Position Monitors (BPMs). The phases of the BPM position lines change monotonically (within each 2π) along the linac and can be used a reference system. The phase of the loss signal compared with this reference system pinpoints the beam loss location, assuming that longitudinal coordinates of the BPMs are known. If the correctors deflection amplitudes and the phase offset between their waveforms are chosen optimally and well calibrated, the same measurement provides values of the β-function and the betatron phase advance at the BPM locations. Optics measurements of this type can be made parasitically, with negligible effect on the emittance, if a long measurement time is acceptable. |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEPLM02 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 19 November 2019 issue date ※ 08 October 2019 | ||
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WEPLM23 | Updated Applications of Advanced Compact Accelerators | linac, electron, laser, site | 694 |
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We are working for downsizing of RF accelerators from room-size to portable and table-top sizes and applying them to industril and social uses. We have developed portable 950 keV / 3.95 MeV X-band (9.3 GHz) electron linac based X-ray/neutron sources and successfully applied to on-site nondestructive inspection of industrial and social infrastructures such as chemical reaction chambers and bridges following the radiation safety law and regulation in Japan. By using the portable 950 keV / 3.95 MeV X-band electron linac based X-ray sources for on-site actual bridge inspection, we visualize inner reinforcement iron structure. The information of of the iron states is used for the structural analysis of the a bridge in order to evaluate its residual strength and sustainability. Table-topμelectron / ion beam sources using laser dielectric accelerating techniques are under development. The beam energy is ~ 1 MeV, the beam size is ~1 micron. We aim to apply them to 3D dynamic observation of radiation-induced DNA damage / repair for basic research of radiation therapy and low dose effect. | |||
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Poster WEPLM23 [0.778 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEPLM23 | ||
About • | paper received ※ 30 August 2019 paper accepted ※ 19 November 2019 issue date ※ 08 October 2019 | ||
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WEPLS09 | Fast Two-Dimensional Calculation of Coherent Synchrotron Radiation in Relativistic Beams | synchrotron, electron, wakefield, synchrotron-radiation | 783 |
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Coherent Synchrotron Radiation(CSR) in a relavistic beam during compression can lead to longitudinal modulation of the bunch with wavelength smaller than bunch length and is regarded as one of the main sources of emittance growth in the bunch compressor. Current simulations containing CSR wake fields often utilize one-dimensional model assuming a line beam. Despite its good computation efficiency, 1D CSR model can be inaccurate in many cases because it ignores the so-called ’compression effect’. On the other hand, the existing 3D codes are often slow and have high demands on computational resources. In this paper we propose a new method for calculation of the three-dimensional CSR wakefields in relativistic beams with integrals of retarded potentials. It generalizes the 1D model and includes the transient effects at the entrance and the exit from the magnet. Within given magnetic lattice and initial beam distributions, the formalism reduces to 2D or 3D integration along the trajectory and therefore allows fast numerical calculations using 2D or 3D matrices. | |||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEPLS09 | ||
About • | paper received ※ 28 August 2019 paper accepted ※ 04 September 2019 issue date ※ 08 October 2019 | ||
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WEPLH11 | RHIC Quench Protection Diode Radiation Damage | kicker, experiment, detector, laser | 831 |
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Funding: Work supported by Brookhaven Science Associates, LLC under Contract No. DE-AC02-98CH10886 with the U.S. Department of Energy. Each of RHIC’s superconducting magnets is protected by a silicon quench protection diode (QPD). In total, RHIC has over 800 diodes installed inside the cryostat close to the vacuum pipe~[RHICconfig]. After years of operation with high energy heavy ion beams we experienced a first permanently damaged QPD in the middle of our FY2016 Au Au run and a second damaged diode in the following year. In 2016 the run had to be interrupted by 19 days to replace the diode, in 2017 RHIC could still operate with a reduced ramping speed of the superconducting magnets. Both diodes were replaced and examined "cold" as well as "warm". This paper reports on what we have learned so far about the conditions leading up to the damage as well as the damage itself. |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEPLH11 | ||
About • | paper received ※ 23 August 2019 paper accepted ※ 05 September 2019 issue date ※ 08 October 2019 | ||
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WEPLO18 | Numerical Study of Coherent Radiation from Induced Plasma Dipole Oscillation by Detuned Laser Pulses | plasma, laser, dipole, simulation | 874 |
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The study of intense laser-plasma interactions is a growing field of both theoretical and applied research. This research focuses on simulating the cross/self-interactions between high-intense short laser pulses and an initial target for preliminary ionization. Unlike our previous studies of laser-matter interaction over preformed plasma, we will explore the injection of laser pulses to induce background plasma driven by the self-guided laser wakefield mechanism, which is used to perturb the plasma for induced dipole oscillations followed by radiation. Inducing a cylindrical spatial plasma column within the laser beam radius regime, it is expected that a stable spatially localized plasma channel will result and the emitted radiation from the plasma dipole oscillation (PDO) will not be affected by surrounding absorption, resulting in effective radiation. We will depict the injection of laser pulses accounting for parameters such as field intensity, profile and phase difference defining the coordinated pulses to assess the potential of enhancing the efficiency and spectral properties of the transverse emitted radiation due to the counter-propagating pulses interaction in plasma. | |||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-WEPLO18 | ||
About • | paper received ※ 27 August 2019 paper accepted ※ 05 September 2019 issue date ※ 08 October 2019 | ||
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THYBA1 | Status of the CBETA Cornell-BNL ERL Prototype | cavity, MMI, beam-loading, electron | 923 |
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CBETA, the Cornell-BNL ERL Test Accelerator, is an SRF multi-turn ERL which has been commissioned in the one-turn configuration from March to July 2019. During this time, the project has demonstrated an energy acceptance of 1.5 in the FFA arc, high-transmission energy recovery performance, and increased the CBETA energy-recovered maximum average current. | |||
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Slides THYBA1 [11.605 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-THYBA1 | ||
About • | paper received ※ 28 August 2019 paper accepted ※ 06 September 2019 issue date ※ 08 October 2019 | ||
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THYBA5 | Study of Fluctuations in Undulator Radiation in the IOTA Ring at Fermilab | experiment, electron, undulator, wiggler | 934 |
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We study turn-by-turn fluctuations in the number of emitted photons in an undulator, installed in the IOTA electron storage ring at Fermilab, with an InGaAs PIN photodiode and an integrating circuit. In this paper, we present a theoretical model for the experimental data from previous similar experiments and in our present experiment, we attempt to verify the model in an independent and a more systematic way. Moreover, in our experiment we consider the regime of very small fluctuation when the contribution from the photon shot noise is significant, whereas we believe it was negligible in the previous experiments. Accordingly, we present certain critical improvements in the experimental setup that let us measure such a small fluctuation. | |||
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Slides THYBA5 [8.048 MB] | ||
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Poster THYBA5 [3.079 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-THYBA5 | ||
About • | paper received ※ 24 August 2019 paper accepted ※ 05 September 2019 issue date ※ 08 October 2019 | ||
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THZBB4 | Beam Loss in the First Segment of the FRIB Linac | detector, linac, monitoring, beam-losses | 965 |
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Funding: Work supported by the U.S. Department of Energy Office of Science under Cooperative Agreement DE-SC0000661. Beam loss in accelerators is an unavoidable and often unwanted reality, but it is not without its use. Information from beam loss can be leveraged to optimize the tune and improve beam quality, in addition to monitoring for machine fault and failure conditions. The folded geometry at the Facility for Rare Isotope Beams (FRIB) presents a unique challenge in the detection of radiative losses, resulting in the introduction of non-traditional measurement schemes. In addition to neutron detectors and pressurized ionization chambers, FRIB will utilize halo ring monitors, fast thermometry within the cryomodules, and differential beam-current measurements. This paper will present an analysis of beam-loss measurements from commissioning the first segment of the FRIB accelerator, and a discussion of ways to evaluate and monitor the health of the beam loss monitoring system. |
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Slides THZBB4 [2.477 MB] | ||
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Poster THZBB4 [0.584 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-THZBB4 | ||
About • | paper received ※ 04 September 2019 paper accepted ※ 17 November 2020 issue date ※ 08 October 2019 | ||
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FRCHC2 | Possibilities for Future Synchrotron Radiation Sources | electron, laser, free-electron-laser, FEL | 1000 |
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The landscape of present accelerator based light sources is drawn. The photon beam brightness increases opens new areas of user applications, both with the arrival of low emittance rings getting closer to diffraction limit and the advent of X-ray Free Electron Lasers, providing agility in terms of performance (two colors, attosecond pulse…). Finally, the path towards light sources using alternate accelerator schemes, such as plasma acceleration is discussed. | |||
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Slides FRCHC2 [76.897 MB] | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2019-FRCHC2 | ||
About • | paper received ※ 04 September 2019 paper accepted ※ 16 November 2020 issue date ※ 08 October 2019 | ||
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