Review section to be matched

We need to create versions of this module for Beam1 and Beam 2:

Tabulate optical functions at main markers to orient ourselves.  Note that E.CELL.12.B1 has the same β functions as S.DS.L2.B1.   This calculation covers a good part of the arcs beyond what was just defined as "IR2DS.B1", etc/  Any difference in dispersions at the first 3 markers  is because of the extra from the crossing bumps.

	NAME	s
	S.CELL.12.B1	1509.	168.7	3.737	1.961	35.09	3.439
	E.CELL.12.B1	1616.	168.7	4.001	1.961	35.09	3.683
	S.DS.L2.B1	2786.	168.7	6.893	1.961	35.09	6.326
	E.ARC.12.B1	2893.	162.4	7.149	2.035	41.55	6.56
	E.DS.L2.B1	3063.	90.18	7.712	0.04939	92.35	6.949
	LHCINJ.B1	3189.	57.44	7.995	-0.1103	67.37	7.265
	IP2	3332.	10.	8.437		10.	7.747
	S.DS.R2.B1	3602.	102.8	9.19	-0.1243	99.66	8.512
	S.ARC.23.B1	3772.	37.13	9.712	1.113	167.8	8.931
	E.DS.R2.B1	3879.	31.42	9.961	0.9958	172.2	9.2
	S.CELL.23.B1	4841.	31.42	12.33	0.9958	172.2	11.39
	E.CELL.23.B1	4948.	31.42	12.6	0.9958	172.2	11.63

	NAME	s
	S.CELL.12.B2	1509.	31.42	3.62	0.9958	172.2	3.552
	E.CELL.12.B2	1616.	31.42	3.884	0.9958	172.2	3.795
	S.DS.L2.B2	2786.	31.42	6.747	0.9958	172.2	6.463
	E.ARC.12.B2	2892.	38.92	6.998	1.113	165.6	6.705
	E.DS.L2.B2	3063.	100.0	7.511	-0.1183	159.5	7.372
	IP2	3332.	10.	8.256		10.	7.997
	S.DS.R2.B2	3602.	111.3	8.912	-0.01145	113.3	8.776
	S.ARC.23.B2	3772.	162.8	9.472	1.898	42.92	9.076
	E.DS.R2.B2	3879.	168.7	9.738	1.961	35.09	9.307
	S.CELL.23.B2	4841.	168.7	12.11	1.961	35.09	11.49
	E.CELL.23.B2	4948.	168.7	12.37	1.961	35.09	11.74

Check values at the IP

Values at the start of the insertion

Values at the end of a periodic arc cell

The sign change is due to the fact that the end marker of the cell is to the right of a QF whereas the start marker of the dispersion suppressor is to the left of a QF.  To get the same proper conditions at the start of the dispersion suppressor, we need

Strengths to be varied

Created by Wolfram Mathematica 6.0  (30 August 2007)