1 / 6

Post-merge Guggenheim stage 12 R.C. Fernow BNL AAG Thursday Meeting 27 December 2012

Post-merge Guggenheim stage 12 R.C. Fernow BNL AAG Thursday Meeting 27 December 2012. Introduction. we have been working on post-merge Guggenheim channel ring simulations curved lattice cells dipole fields from tipping the solenoids

tad
Download Presentation

Post-merge Guggenheim stage 12 R.C. Fernow BNL AAG Thursday Meeting 27 December 2012

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Post-merge Guggenheim stage 12 R.C. Fernow BNL AAG Thursday Meeting 27 December 2012

  2. Introduction • we have been working on post-merge Guggenheim channel ring simulations • curved lattice cells • dipole fields from tipping the solenoids • generate Icool field maps in cylindrical coordinates • emittance exchange by tracking thru wedges • uses RF Be windows scaled from Study 2 • we have working files for all the (11) flip stages • now looking at first non-flip stage

  3. Small ring • first tried small ring (ρ = 1.53 m), similar to last flip lattice • could not find a reasonable closed orbit • tried varying starting parameters for orbit finder by hand • computed 2D beta functions were not reasonable • transmission thru cooling cell was very small

  4. Larger ring • looked at larger ring with ρ = 5.47 m • found a good closed orbit solution • 2D beta functions still bad ( β ~ 2 mm, should be ~5.9 cm) • dispersion was small D = 3.3 cm • for 120o wedge • met reference emittance goals for this stage • εTN = 0.432 mm, εLN = 2.37 mm after 12 cells • but transmission was very poor ~0.476

  5. Still larger ring • looked at even larger ring with ρ = 10.95 m • found a good closed orbit • beta functions were still bad ( β ~ 2 mm) • dispersion was very small D = 1.7 cm • for 120o wedge • not able to meet both reference emittance goals for this stage • εTN = 0.452 mm, εLN = 2.68 mm after 39 cells • transmission increased, but was still poor ~0.707 • tried wedge angles up to 140o • but was unable to reach the longitudinal emittance goal

  6. Eigenvalue analysis • currently looking with Scott at eigenvalues of the one-cell transport matrix • trying to find evidence for the source of poor performance • for ∞ case, both eigenvalues must be the same • possible trouble with • intrinsic design of the lattice ? • errors or bad approximations in the simulation ? • methods used in the analysis program ?

More Related