“…I will not look into this general question here. It suffices to point out that many numerical studies [76,75] support the assumption that a 9-th order Taylor map is adequate for the stability studies in an electron machine. In the LER ring example, a 9-th order Taylor map has been used to generate tracking data and compare with the numerical fits.…”
“…I will not look into this general question here. It suffices to point out that many numerical studies [76,75] support the assumption that a 9-th order Taylor map is adequate for the stability studies in an electron machine. In the LER ring example, a 9-th order Taylor map has been used to generate tracking data and compare with the numerical fits.…”
“…A Vps truncated at an order of Q can be mathematically written as [1] [5] O=(J that is, each component of the Vps is a Tps represented the last section. For example, the Zth component would…”
Section: Vector Truncated Power Series -Vpsmentioning
confidence: 99%
“…where again iOSIP and j OSIP are One-Step Index Pointers and in the double loop, the inner one is vectorized while the outer one is parallelized. It was this fast computational process that allowed the fast Taylor-map tracking for the SSC to high orders (11-or 12-th order) with a computational speed two orders of magnitude faster than the conventional element-by-element tracking [5].…”
“…Such inaccuracy and nonsymplecticity have been controversial in the use of one-turn maps for long-term tracking. However, it is well under stood that the required accuracy and symplecticity depend on circumstances [7]. For the PEP-II lattice dynamic aper ture studies (only 1024 turns), through numerous testing we have concluded that a map of 10 th order in Hamiltonian (9" 1 order in Taylor expansion) is accurate enough and 3 Poisson bracket expansion of the Lie transformation is ac curate and symplectic enough.…”
Section: Reliability Of the Npb Trackingmentioning
confidence: 98%
“…The nPB tracking provides a fac tor of 100 in tracking speed and also offers insight into the underlying physics. Map tracking for proton accelera tors [6] [7] [8] is a different problem since there is no signifi cant synchrotron radiation damping.…”
With a newly developed algorithm using resonance ba sis Lie generators and their evaluation with action-angle Poisson bracket maps (nPB tracking) we have been able Lo perform fasl tracking for dynamic aperture studies of PEP-II lattices as well as incorporate lattice n on linearities in beam-beam studies [l]. We have been able to better un derstand the relationship between dynamic apertures and the tune shift and resonance coefficients in the generators of the one-turn rr»aps [2]. To obtain swamp plots (dynamic aperture vs. working point) of the PEP-II lattices, we firsL compute a one-turn resonance basis map for a nominal working point and then perform nPB tracking by switch ing the working point while holding fixed all other terms in the map. Results have been spot-checked by comparing with element-by-element tracking.
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