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Search indexed NASA NTRS and DOE OSTI research on propulsion, heat transfer, battery materials and energy systems. Follow report and document links to the original sources.

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At least 325 records · Page 18
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DOE OSTI2021

Dynamic Aperture Evaluation for the Hadron Storage Ring in the Electron-Ion Collider

The Electron-Ion Collider (EIC) is aiming at a design luminosity of 1e34 cm⁻²s⁻¹. To maintain such a high luminosity, both beams in the EIC need an acceptable beam lifetime in the presence of the beam-beam interaction. For this purpose, we carried out weak-strong element-by-element particle tracking to evaluate the long-term dynamic aperture for the hadron ring lattice design. We improved our simulation code SimTrack to treat some new lattice design features, such as radially offset on-momentum orbits, coordinate transformations in the interaction region, etc. In this article, we will present the preliminary dynamic aperture calculation results with β^{*}- function scan, radial orbit shift, crossing angle collision, and magnetic field errors.

Luo, Y.↗
DOE OSTI2022

COOLING PERFORMANCE IN A DUAL ENERGY STORAGE RING COOLER*

The lon­gi­tu­di­nal and trans­verse emit­tance growth in hadron beams due to in­tra-beam scat­ter­ing (IBS) and other heat­ing sources de­te­ri­o­rate the lu­mi­nos­ity in a col­lider. Hence, a strong hadron beam cool­ing is re­quired to re­duce and pre­serve the emit­tance. The cool­ing of high en­ergy hadron beam is chal­leng­ing. We pro­pose a dual en­ergy stor­age ring-based elec­tron cooler that uses an elec­tron beam to ex­tract heat away from hadron beam in the cooler ring while the elec­tron beam is cooled by syn­chro­tron ra­di­a­tion damp­ing in the high en­ergy damp­ing ring. In this paper, we pre­sent a de­sign of a dual en­ergy stor­age ring-based elec­tron cooler. Fi­nally, the cool­ing per­for­mance is sim­u­lated using Jef­fer­son Lab Sim­u­la­tion Pack­age for Elec­tron Cool­ing (JSPEC) for pro­ton beams at the top en­ergy of 275 GeV for Elec­tron-Ion Col­lider.

Dhital, B.↗
DOE OSTI2022

Modeling of the Optical Stochastic Cooling at the IOTA Storage Ring Using ELEGANT

In support of the Optical Stochastic Cooling (OSC) experiment at IOTA, we implemented a high-fidelity model of OSC in ELEGANT. The element is generalizable to any OSC experiment and captures three main behaviors; (i) the longitudinal time of flight OSC, (ii) the effects between the transverse motion of particles in the beam and the transverse distribution of undulator radiation, and (iii) the incoherent contributions of neighboring particles. Together these produce a highly accurate model of OSC and were benchmarked using the results from the IOTA OSC experiment.

43 PARTICLE ACCELERATORS↗
DOE OSTI2017

Status of the Development of Superconducting Undulators for Storage Rings and Free Electron Lasers at the Advanced Photon Source

Development of superconducting undulator (SCU) technology continues at the Advanced Photon Source (APS). The experience of building and successful operating the first short-length, 16-mm period length superconducting undulator SCU0 paved the way for a 1-m long, 18-mm period device— SCU18-1— which has been in operation since May 2015. The APS SCU team has also built and tested a 1.5-m long, 21-mm period length undulator as a part of the LCLS SCU R&D program, aimed at demonstration of SCU technology availability for free electron lasers. This undulator successfully achieved all the requirements including a phase error of 5° RMS. Our team has recently completed one more 1-m long, 18-mm period length undulator— SCU18-2— that is replacing the SCU0. We are also working on a helical SCU for the APS. The status of these projects will be presented.

Ivanyushenkov, Y.↗
DOE OSTI2017

ACCELERATOR PHYSICS CHALLENGES IN THE DESIGN OF MULTI-BEND-ACHROMAT-BASED STORAGE RINGS

With the recent success in commissioning of MAX IV, the multi-bend achromat (MBA) lattice has begun to deliver on its promise to usher in a new generation of higher-brightness synchrotron light sources. In this paper, we begin by reviewing the challenges, recent success, and lessons learned of the MAX-IV project. Drawing on these lessons, we then describe the physics challenges in even more ambitious rings and how these can be met. In addition, we touch on engineering issues and choices that are tightly linked with the physics design.

Borland, M.↗
DOE OSTI2013

Analysis of localized beam losses in the Booster extraction straight section and the Booster to Storage Ring Transfer Line

The NSLS-II accelerators are installed within radiation shielding walls that are designed to attenuate the radiation generated from an assumed beam loss power (current multiplied by the assumed energy) within the beam channel to a level of <0.5mrem/h at the outer surface of the bulk shield walls of the accelerator. This Bulk Shielding Power assumes that the beam current is intercepted by a thick target (i.e., 30 cm of copper or steel) along the Booster or transport line beam axis and the dose rate level is calculated transverse to the beam axis. Any operational losses greater than this BSP level are expected to be addressed by installing supplemental shielding near that loss point in order to attenuate this radiation level outside the shield wall to the design level of <0.5mrem/hr.

43 PARTICLE ACCELERATORS↗
DOE OSTI2018

Electron Storage Ring Development for ICS Sources

The purpose of the Fast-Track SBIR was to enhance the performance of the Compact Light Source (CLS) by a factor of 10 in flux and brightness. This was accomplished in collaboration with the SLAC National Accelerator Laboratory by increasing the intensity of the stored electron beam, by decreasing the emittance of the stored beam, and by decreasing the spot size at the interaction point of the CLS. In addition, the CLS feedbacks and software were developed further to enhance the operational stability and reliability. SLAC National Accelerator Laboratory participated at the 30% level of funding and effort.

43 PARTICLE ACCELERATORS↗
DOE OSTI2018

Lattice Element Error Solver for Modeling of Accelerators, Storage Ring, Transport Systems, and Insertion Devices

The goals of CRADA 350 were achieved in this Phase I SBIR work. Specifically, a software environment was developed which included a nonlinear solver, OASIS. During the Phase I work, we applied the algorithm to a number of nonlinear-solver benchmark problems, including SLAC accelerator problems. By searching over only two optimization-control parameters, this Phase I work has enabled the development of a systematic procedure to facilitate the finding of a “best-guessed” global minimum solution for various types of non-linear problems with different size and complexity. This set of rules was codified and led to a versatile nonlinear program, IMIGO.

43 PARTICLE ACCELERATORS↗
DOE OSTI2018

An Online Beam Loss Monitor for NSLS-II Storage Ring

Reliable beam loss monitors are important tools for the safe operation of the accelerators. Beam loss monitors provide valuable information on the magnitude and location of the particle beam loss inside the accelerator enclosures. In the synchrotron radiation facilities, the electron accelerator enclosures experience a mixed radiation environment, consisting of low energy x-ray background along with bremsstrahlung and photoneutrons.

36 MATERIALS SCIENCE↗
DOE OSTI2018

NSLS-II Storage Ring Injection Using a Nonlinear Injection Kicker

The NSLS-II has been operating successfully with top off injection since September 2015. Measurements of the stored beam show a transient of 200 μm in the long straight sections during top off injections. This transient is not desirable for some users, particularly those who specialized in imaging or are otherwise sensitive to beam motion. Users are provided with a signal with which they can gate their detectors, but it is desirable to reduce or eliminate this motion all together. Studies have been performed to reduce the transients, and it is clear that the power supplies require more tunability in the pulse shape in order to reduce the transient across the entire bunch train. Other light sources have explored the possibility of using pulsed quadrupoles and sextupoles as the injection magnet. The stored beam receives no kick as the on-axis fields in these magnets is zero, but the injected beam would see a kick as it is off-center. One drawback of the pulsed quadrupole is that the stored beam experiences a size oscillation. Another issue with a nonlinear kicker is the gradient seen by the injected beam. The transport line needs to be tuned for this gradient, and depending on the strength of the nonlinearity, this gradient may change greatly with injected beam position. Therefore, other facilities have explored other magnet configurations that are nonlinear but have a gradient with less positional dependence. The prospect of using a sextupole kicker was investigated during the design phase of the NSLS-II. It was decided that the idea would not be pursued for several reasons. In particular, the design that was studied the most in depth was not compatible with the standard four bump injection design and the tolerances required were deemed too tight at the time. Other ideas were discussed as well and ultimately none were accepted into the design. In this report we discuss the possibility of placing a nonlinear kicker in the first straight section after the injection straight instead of using the injection bumps. The design of the kicker is based on a design that has been used successfully at BESSY and MAX IV. Our conceptual kicker design is compatible with the existing ring optics and power supply requirements. We show that the transport line is capable of being matched to the required optics. The design does not have restrictive tolerances and is a viable option for a facility upgrade.

36 MATERIALS SCIENCE↗