| Energy [GeV] | 2.085 |
| Wiggler[T] | 2.1 |
| Qx | 10.57 |
| Qy | 9.62 |
| Qz [6.88 MV] | 0.089 |
| Emittance [nm] | 7.5nm |
| Bunch length | 12.3mm |
- linear lattice constraints
- non linear lattice constraints energy offset +- 0.006 and disp
- lattice file
- Optical parameters and orbits
- table
- Lattice gif and ps
(including orbit)
- Lattice gif and ps (without orbit)
- RF voltage = 6.88, Qs=-0.089, Bunch length = 12mm
Tune scan
Tune scan gif and (initialization)
with Qz = -0.089
Dynamic aperture
The dynamic aperture gif ( ps )
and (initialization) 20080706-1 .Qx=10.57 Qy=9.6,Qz=-0.089.
The horizontal and vertical tunes are
shifted in order to avoid the synchrobetatron line that shifts with the lower synchrotron tune. (See tune scans)
Dynamic aperture is computed for fractional energy
offset of 0%, 0.5% and 1%. Tracking is based on symplectic integration through the same wiggler
map as for CESR-c calculations.
Particles are considered lost
if their amplitude >> the real physical aperture. (This seems to be the
way linear collider damping ring people report dynamic aperture.)
Analyzer output
Synchrotron radiation data
chamber profile: (near L3) and table for ring
&synrad_params
sr_param%lat_file = "/home/dlr/lat/bmad_6wig_nosol_8nm_2085.lat" ! Input lattice.
sr_param%i_beam = 0.1 ! Beam current.
sr_param%epsilon_y = 10e-12 ! Vertical emittance.
seg_len = 0.01 ! Segment length for calculation.
beam_direction = -1 ! -1 = track backwards only,
! 0 = track both directions, 1 = forward.
wall_file = "wall.dat" ! "NONE" => Use a wall with a fixed offset from the beam.
wall_offset = 0.0448 ! Used when wall_file is set to "NONE"
forward_beam = "POSITRON" ! "POSITRON" or "ELECTRON"
backward_beam = "ELECTRON" ! This is important if there are elsep elements.
/
Electrostatic separators are off
(Tabulated data includes details of power, twiss parameters, and magnetic element where photons are incident on the chamber)
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