意外的成功
发表于 2025-3-23 12:09:20
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Audiometry
发表于 2025-3-23 16:19:39
Betatron,uced in the previous chapters, such FAISCEAU, FAISTORE. SR monitoring uses SRPRNT. INCLUDE allows simplifying the input data files. Graphs are part of data treatment and simulation outcomes, they are produced using . or gnuplot.
陈旧
发表于 2025-3-23 20:46:18
Microtron,FIT. SYSTEM is used to, mostly, resort to gnuplot so as to end simulations with some nice graphs (orbits, fields, or else) obtained by reading data from output files such as zgoubi.fai (resulting from the use of FAISTORE), zgoubi.plt (resulting from IL . 2), or other zgoubi.*.out files resulting
路标
发表于 2025-3-24 00:20:06
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Blasphemy
发表于 2025-3-24 06:26:22
Weak Focusing Synchrotron,ral brightness uses .. Particle monitoring requires keywords introduced in the previous chapters, including FAISCEAU, FAISTORE, PICKUPS, and some others. Spin motion computation and monitoring resort to SPNTRK, SPNPRT and FAISTORE. Optics matching and optimization use FIT. INCLUDE is used, mostly
一加就喷出
发表于 2025-3-24 08:26:01
Strong Focusing Synchrotron,using QUADRUPO or MULTIPOL. The latter can simulate higher order lenses, which can otherwise resort to SEXTUPOL, OCTUPOLE, etc. Acceleration uses CAVITE. Accounting for synchrotron radiation (SR) energy loss requires SRLOSS. Monte Carlo SR monitoring can use SRPRNT, which logs data in zgoubi.res. SR
Palpitation
发表于 2025-3-24 13:29:01
Beam Lines,d their data from output files filled up during the execution of the code, such as zgoubi.fai (resulting from the use of FAISTORE), zgoubi.plt (resulting from IL . 2 flag), or other zgoubi.*.out files resulting from a PRINT command.
亚当心理阴影
发表于 2025-3-24 18:34:21
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CALL
发表于 2025-3-24 19:00:27
François Méotories is addressed. The effect of the mechanical factors like ovality, creep, cranking of kiln, etc. on refractory performance and the checking method are discussed in details with diagrams. The effect of overheating, flame character, etc. is discussed in detail. The effect of thermal shock, abrasio
Locale
发表于 2025-3-25 02:52:47
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