Paper | Title | Page |
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TUPOB04 | A More Compact Design for the JLEIC Ion Pre-Booster Ring | 483 |
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Funding: This work was supported by the U.S. Department of Energy, Office of Nuclear Physics, under Contract No. DE-AC02-06CH11357 for ANL The original design of the JLEIC pre-booster was a 3-GeV figure-8 shaped synchrotron with a circumference of about 240 m. In the current baseline design, the 3-GeV pre-booster was converted into an 8-GeV booster of the same shape and size but using super-ferric magnets with fields up to 3 Tesla. In order to limit the foot-print of the JLEIC ion complex and reduce its total cost, we have designed a more compact and cost-effective octagonal 3-GeV ring about half the size of the original one. At 3 GeV, the figure-8 shape is not required to preserve ion polarization; Siberian snakes with reasonable magnetic fields can be used for spin correction. As the ion collider ring requires an injection energy of at least 8 GeV, we propose to use the existing electron storage ring, which is part of the electron complex, as a large booster for the ions up to 11 GeV. The design optimization of the pre-booster ring will be presented leading to the final octagonal ring design. Preliminary beam simulations will also be presented and discussed. |
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DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-TUPOB04 | |
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TUPOB14 | An Accurate and Efficient Numerical Integrator for Pair-Wise Interaction | 514 |
SUPO01 | use link to see paper's listing under its alternate paper code | |
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We are developing a new numerical integrator based on Picard iteration method for Coulomb collisions. The aim is to achieve a given prescribed accuracy most efficiently. The integrator is designed to have adaptive time stepping, variable order, and dense output. It also has an automatic selection of the order and the time step. We show that with a good estimation of the radius of convergence of the expansion, we can obtain the optimal time step size. We also show how the optimal order of the integration is chosen to maintain the required accuracy. For efficiency, particles are distributed over time bins and propagated accordingly. | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-TUPOB14 | |
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TUPOB15 | Implementing the Fast Multipole Boundary Element Method With High-Order Elements | 518 |
SUPO13 | use link to see paper's listing under its alternate paper code | |
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The next generation of beam applications will require high-intensity beams with unprecedented control. For the new system designs, simulations that model collective effects must achieve greater accuracies and scales than conventional methods allow. The fast multipole method is a strong candidate for modeling collective effects due to its linear scaling. It is well known the boundary effects become important for such intense beams. We implemented a constant element fast boundary element method (FMBEM) * as our first step in studying the boundary effects. To reduce the number of elements and discretization error, our next step is to allow for curvilinear elements. In this paper we will present our study on a quadratic and a cubic parametric method to model the surface.
* A.Gee and B.Erdelyi, "A Differential Algebraic Framework for the Fast Indirect Boundary Element Method," in Proc. IPAC'16. Busan, South Korea. |
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Poster TUPOB15 [1.727 MB] | |
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-TUPOB15 | |
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THPOA68 | The First Particle-Based Proof of Principle Numerical Simulation of Electron Cooling | 1241 |
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Envisioned particle accelerators such as JLEIC demand unprecedented luminosities of 1034 cm -2 s -1 and small emittances are key to achieve them. Electron cooling, where a 'cold' electron beam and the 'hot' proton or ion beam co-propagate in the cooling section of the accelerator, can be used to reduce the emittance growth. It is required to precisely calculate the cooling force among particles to estimate accurately the cooling time. There are different methods to simulate electron cooling. We have developed a novel code, Particles' High-order Adaptive Dynamics (PHAD), for electron cooling. This code differs from other established methods since it is the first particle-based simulation method employing full particle nonlinear dynamics. In this paper we present the first results obtained that establish electron cooling of heavy ions. | ||
DOI • | reference for this paper ※ https://doi.org/10.18429/JACoW-NAPAC2016-THPOA68 | |
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