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TOMAS, R.; FISCHER, W.
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/SC (United States)2005
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/SC (United States)2005
AbstractAbstract
[en] The authors consider a scenario of having two identical Interaction Points (IPs) in the Relativistic Heavy Ion Collider (RHIC). The strengths of beam-beam resonances strongly depend on the phase advance between these two IPs and therefore certain phase advances could improve beam life-time and luminosity. The authors compute the dynamic aperture (DA) as function of the phase advance between these IPs to find the optimum settings.The beam-beam interaction is treated in the weak-strong approximation and a non-linear model of the lattice is used. For the current RHIC proton working point (0.69.0.685) [1] the design lattice is found to have the optimum phase advance. However this is not the case for other working points
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16 May 2005; 5 p; PAC 2005; Knoxville, TN (United States); 16-20 May 2005; KB--0202011; AC--02-98CH10886; Available from PURL: https://www.osti.gov/servlets/purl/15016132-cwIuXW/native/
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CALAGA, R.; TOMAS, R.
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/OFFICE OF SCIENCE (United States)2004
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/OFFICE OF SCIENCE (United States)2004
AbstractAbstract
[en] Identification of malfunctioning beam position monitors (BPMs) play an important role in any orbit or turn-by-turn analysis. Singular value decomposition (SVD) and Fourier transform methods were recently employed to identify malfunctioning BPMs at RHIC. A detailed statistical comparison between the two methods for Run 2003 was in good agreement and proved to be a robust method to identify faulty BPMs. We evaluate detailed BPM performance for different upgrades of BPM low-level software during Run 2003 and 2004
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5 Jul 2004; 5 p; 9. European Particle Accelerator Conference (EPAC-04); Lucerne (Switzerland); 5-9 Jul 2004; KB020204; AC02-98CH10886; Available from PURL: https://www.osti.gov/servlets/purl/15007986-bcXgGr/native/
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AbstractAbstract
[en] Principle scheme and method of chemical cleaning of steam generators are given without formulae of the solutions used. Quantitative data on sludge composition, corrosion effect on on structural materials and removed sludge quantity during steam generators cleaning at the Millstone-Point-2 NPP are presented
Original Title
Primenenie khimicheskogo sposoba ochistki trubnykh dosok parogeneratorov ot shlama
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Translated from English Nuclear Engineering International, 1987, v. 32, N 390, p. 39-41.
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Calaga, R.; Tomas, R.; Zimmermann, F.
Brookhaven National Laboratory (United States). Funding organisation: DOE - Office Of Science (United States)2010
Brookhaven National Laboratory (United States). Funding organisation: DOE - Office Of Science (United States)2010
AbstractAbstract
[en] The 3rd LHC Crab Cavity workshop (LHC-CC09) took place at CERN in October 2009. It reviewed the current status and identified a clear strategy towards a future crab-cavity implementation. Following the success of crab cavities in KEK-B and the strong potential for luminosity gain and leveling, CERN will pursue crab crossing for the LHC upgrade. We present a summary and outcome of the variousworkshop sessions which have led to the LHC crab-cavity strategy, covering topics like layout, cavity design, integration, machine protection, and a potential validation test in the SPS.
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23 May 2010; 5 p; IPAC'10: 1. International Particle Accelerator Conference; Kyoto (Japan); 23-28 May 2010; KB0202011; AC02-98CH10886; Available from http://www.bnl.gov/isd/documents/71532.pdf; PURL: https://www.osti.gov/servlets/purl/1013483-MJnDIv/
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FISCHER, W.; SATOGATA, T.; TOMAS, R.
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/SC (United States)2005
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/SC (United States)2005
AbstractAbstract
[en] Beam echoes are a very sensitive method to measure diffusion, and longitudinal echo measurements were performed in a number of machines. In RHIC, for the first time, a transverse beam echo was observed after applying a dipole kick followed by a quadrupole .kick. After application of the dipole kick, the dipole moment decohered completely due to lattice nonlinearities. When a quadrupole kick is applied at time τ after the dipole kick, the beam re-cohered at time 2τ thus showing an echo response. We describe the experimental setup and measurement results. In the measurements the dipole and quadrupole kick amplitudes, amplitude dependent tune shift, and the time between dipole and quadrupole kick were varied. In addition, measurements were taken with gold bunches of different intensities. These should exhibit different transverse diffusion rates due to intra-beam scattering
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16 May 2005; 5 p; Particle Accelerator Conference PAC-05; Knoxville, TN (United States); 16-20 May 2005; KB-0202011; AC02-98CH10886; Available from PURL: https://www.osti.gov/servlets/purl/15016281-NR09It/native/
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CALAGA, R.; FRANCHI, A., TOMAS, R.; CERN)
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/SC (United States)2006
BROOKHAVEN NATIONAL LABORATORY (United States). Funding organisation: DOE/SC (United States)2006
AbstractAbstract
[en] Compensation of transverse coupling during the RHIC energy ramp has been proven to be non-trivial and tedious. The lack of accurate knowledge of the coupling sources has initiated several efforts to develop fast techniques using turn-by-turn BPM data to identify and compensate these sources. This paper aims to summarize the beam experiments performed to measure the coupling, matrix and resonance driving terms with the aid of RHIC ac dipoles at injection energy
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26 Jun 2006; 5 p; EPAC'06 - 10. Biennial European Particle Accelerator Conference; Edinburgh (United Kingdom); 26-30 Jun 2006; KB0202011; AC02-98CH10886; Available from http://www.pubs.bnl.gov/documents/32804.pdf; PURL: https://www.osti.gov/servlets/purl/895874-1oMRfs/
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[en] Linear coupling is one of the factors that determine beam lifetime in RHIC. The traditional method of measuring the minimum tune separation requires a tune scan and can't be done parasitically or during the acceleration ramp. A new technique of using ac dipoles to measure linear coupling resonance has been developed at RHIC. This method measures the degree of coupling by comparing the amplitude of the horizontal coherent excitation with the amplitude of the vertical coherent excitation if the beam is excited by the vertical AC dipole and vice versa. One advantage of this method is that it can be done without changing tunes from the normal machine working points. In principle, this method can also localize the coupling source by mapping out the coupling driving terms throughout the ring. This is very useful for local decoupling the interaction regions in RHIC. A beam experiment of measuring linear coupling has been performed in RHIC during its 2003 run, and the analysis of the experimental data is discussed in this paper
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12 May 2002; 3 p; 2003 PARTICLE ACCELERATOR CONFERENCE; PORTLAND, OR (United States); 12-16 May 2003; KB02022011; AC02-98CH10886; Available from PURL: https://www.osti.gov/servlets/purl/15006721-uVhWOJ/native/
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Miyamoto, R.; Cattin, M.; Serrano, J.; Tomas, R.
Brookhaven National Laboratory, Relativistic Heavy Ion Collider (United States). Funding organisation: Doe - Office Of Science (United States)2010
Brookhaven National Laboratory, Relativistic Heavy Ion Collider (United States). Funding organisation: Doe - Office Of Science (United States)2010
AbstractAbstract
[en] The adiabaticity of the AC dipole might be compromised by noise or unwanted frequency components in its signal. An effort has been put to characterize and optimize the signal quality of the LHC AC dipoles. The measured signal is used in realistic simulations in order to evaluate its impact on beam dynamics and to ultimately establish safe margins for the operation of the LHC AC dipoles.
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23 May 2010; 5 p; IPAC'10: 1. International Particle Accelerator Conference; Kyoto (Japan); 23-28 May 2010; KB0202011; AC02-98CH10886; Available from http://www.bnl.gov/isd/documents/71544.pdf; PURL: https://www.osti.gov/servlets/purl/984417-3q3wQA/
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[en] Recently resonance driving terms were successfully measured in the CERN SPS and the BNL RHIC from the Fourier spectrum of BPM data. Based on these measurements a new analysis has been derived to extract multipole strengths. In this paper we present experimental measurements of sextupolar and skew quadrupolar strengths carried out at RHIC. A non-destructive measurement using an AC dipole is also presented
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5 Jul 2004; 5 p; 9. European Particle Accelerator Conference (EPAC-04); Lucerne (Switzerland); 5-9 Jul 2004; KB020204; AC02-98CH10886; Available from PURL: https://www.osti.gov/servlets/purl/15008005-68kjYD/native/
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Aiba, M.; Calaga, R.; Tomas, R.; Vanbavinkove, G.
Brookhaven National Laboratory Relativistic Heavy Ion Collider (United States). Funding organisation: DOE - Office Of Science (United States)2010
Brookhaven National Laboratory Relativistic Heavy Ion Collider (United States). Funding organisation: DOE - Office Of Science (United States)2010
AbstractAbstract
[en] Measurements of chromatic beta-beating were carried out for the first time in the RHIC accelerator during Run 2009. The analysis package developed for the LHC was used to extract the off-momentum optics for injection and top energy. Results from the beam experiments and compassion to the optics model are presented. The primary goal of the RHIC experiments were execute an on-line measurement of the optics using the tools developed for the LHC. Turn-by-turn BPM trajectories (typically 1000 turns) acquired immediately after an external dipole kick are numerically analyzed to determine the optical parameters at the location of the beam position monitors (BPMs). For chromatic optics, a similar analysis, but on a beam with finite momentum offset(s). Each optical measurement typically is calculated from multiple data sets to capture statistical variations and ensure reproducibility. The procedure of measurement and analysis is detailed in ref (1, 2). Two dedicated experiments were performed at RHIC with protons during Run 2009. The first at injection energy and optics and the other at 250 GeV and squeezed optics. The basic RHIC parameters relevant for the two experiments are listed in Table 1.
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23 May 2010; 5 p; IPAC'10: 1. International Particle Accelerator Conference; Kyoto (Japan); 23-28 May 2010; KB0202011; AC02-98CH10886; Available from http://www.bnl.gov/isd/documents/71530.pdf; PURL: https://www.osti.gov/servlets/purl/1013482-S70Kyf/
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