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master_lattice.py
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master_lattice.py
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import numpy as np
import math
########### INPUT ###########
#Design of the machine#
arc_number = 8 #number of arcs in the ring
arc_cells = 28 #number of cells per arc
straight_sections = 8 #number of straight sections in the ring
straight_cells = 4 #number of cells per straight section
total_cells = (arc_number*arc_cells)+(straight_sections*straight_cells) #total number of cells in the ring
print 'total number of cells in the ring = '
print total_cells
print '\n'
cell_length = 100
circumference = total_cells*cell_length
print 'circumference = '
print circumference
print '\n'
m = 60.1 #phase advance per cell. Choose close to 60, but not exactly 60! (otherwise resonances...)
tune = (m*total_cells)/360
cell_dipoles = 2 #number of dipoles per cell
no_dipoles = (straight_cells + 2)*straight_sections*cell_dipoles #number of cells with no dipoles
total_dipoles = (total_cells*cell_dipoles) - no_dipoles #number of dipoles in the ring
#sextupole strength
ksf =3.17441e-04
ksd =-4.07306e-04
#tune
Qpx = 43.0
Qpy = 43.0
frac_q_x = 0.11 #Give slightly different fractional numbers to avoid coupling
frac_q_y = 0.21
Qx_total = Qpx+frac_q_x
Qy_total = Qpy+frac_q_y
#number of turns for tracking
TURNS=1000
#Define chromaticities. Usual values are up to 40 (maximum!)
Qx = []
Qy = []
f = open('chromaticities.txt','r')
for line in f:
chromaticity=line.split()
Qx.append(float(chromaticity[0]))
Qy.append(float(chromaticity[1]))
DQ1 = Qx[0] #give values from 0-9. These correspond to chromaticities = 0,1,5,10,15,20,25,30,35,40.
DQ2 = Qy[0]
#Define dipoles, quadrupoles and sextupoles as multipoles
elements = """
MBS:multipole, knl:={d_angle};
qfType:multipole, knl:={0,kf};
qdType:multipole, knl:={0,kd};
sfType:multipole, knl:={0,0,ksf};
sdType:multipole, knl:={0,0,ksd};
CAV: RFCAVITY, L := 0.;
"""
fodo = """
fodo:SEQUENCE, REFER=entry, L=circumference;
"""
con = """
beam, particle=proton, sequence=fodo, energy=6500;
use, sequence=fodo;
"""
matching_begin= """
match, sequence = fodo;
"""
matching_end = """
vary, name = kf, step=0.00001;
vary, name = kd, step=0.00001;
vary, name = ksf, step=0.00001;
vary, name = ksd, step=0.00001;
lmdif, calls=50, tolerance=1e-6; //method adopted
ENDMATCH;
"""
twiss = """
twiss,save,centre,file=twiss_master.out;
"""
plots = """
survey,file=survey_master.cas;
"""
#Tracking here!
track = """
start, x= 2e-3, px=0, y= 2e-3, py=0, t= 0, pt = 1e-6;
start, x= 3e-3, px=0, y= 3e-3, py=0, t= 0, pt = 3e-5;
start, x= 4e-3, px=0, y= 4e-3, py=0, t= 0, pt = 6e-5;
start, x= 5e-3, px=0, y= 5e-3, py=0, t= 0, pt = 8e-5;
start, x= 6e-3, px=0, y= 6e-3, py=0, t= 0, pt = 1e-4;
start, x= 7e-3, px=0, y= 7e-3, py=0, t= 0, pt = 1.3e-4;
start, x= 8e-3, px=0, y= 8e-3, py=0, t= 0, pt = 1.6e-4;
start, x= 9e-3, px=0, y= 9e-3, py=0, t= 0, pt = 1.8e-4;
start, x= 10e-3, px=0, y= 10e-3, py=0, t= 0, pt = 2.1e-4;
start, x= 11e-3, px=0, y= 11e-3, py=0, t= 0, pt = 3e-4;
"""
#Generate MADX file
fname = 'madx_master_lattice.txt'
#WRITE IN MADX FILE
with open(fname, 'w') as fid:
fid.write('arc_number = %f;\n'%(float(arc_number)))
fid.write('arc_cells = %d;\n'%(int(arc_cells)))
fid.write('straight_sections = %f;\n'%(float(straight_sections)))
fid.write('straight_cells = %d;\n'%(int(straight_cells)))
fid.write('total_cells = (arc_number*arc_cells)+(straight_sections*straight_cells);\n')
fid.write('cell_length = %f;\n'%(float(cell_length)))
fid.write('circumference = total_cells*cell_length;\n')
fid.write('\n')
fid.write('m = %f;\n'%(float(m)))
fid.write('tune = %f;\n'%(float(tune)))
fid.write('cell_dipoles = %f;\n'%(float(cell_dipoles)))
fid.write('no_dipoles = %f;\n'%(float(no_dipoles)))
fid.write('total_dipoles = %f;\n'%(float(total_dipoles)))
fid.write('d_angle := 2*pi/total_dipoles;\n')
fid.write('\n')
fid.write('kf := (4*sin(m/2))/cell_length;\n')
fid.write('kd := -(4*sin(m/2))/cell_length;\n')
fid.write('\n')
fid.write('ksf := %f;\n'%(float(ksf)))
fid.write('ksd := %f;\n'%(float(ksd)))
fid.write(elements)
fid.write(fodo)
#build lattice
loc=0.0 #position of the 1st element
dip=1 #dipole counter
drift = float(cell_dipoles + 2)*total_cells #number of drift spaces
print 'Number of drift spaces = '
print drift
print '\n'
space = float(circumference/drift)
print 'space = '
print space
print '\n'
full_cells = abs((arc_cells*arc_number/straight_sections)-4) #full cells in a row
print 'full cells in a row = '
print full_cells
print '\n'
half_dipoles = (cell_dipoles/2)
straight_drift = float(half_dipoles+1) #in straight sections space between F and D is different due to the missing dipoles. N dipoles result in N+1 drifts
print 'straight drifts = '
print straight_drift
print '\n'
fid.write('CAV1:CAV, at=0.;\n')
offset = 1
#lattice begins in the middle of a straight section
for jj in xrange (straight_sections):
########################################################################################################################################
print 'Last half straight section'
print '\n'
for rr in xrange (straight_cells/2):
fid.write('/*cell%d*/\n'%(int(rr+offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(rr+offset), float(loc)))
#defocus
loc=loc+(straight_drift*space)
fid.write('qd%d:qdType, at=%f;\n'%(int(rr+offset), float(loc)))
loc=loc+(straight_drift*space)
fid.write('\n')
offset = offset+rr+1
print 'offset rr = %d= '%int(rr)
print offset
print '\n'
########################################################################################################################################
######## Dispersion suppressor ########
print 'Begin dispersion suppressor'
print '\n'
fid.write('/*cell%d*/\n'%(int(offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(offset), float(loc)))
for kk in xrange (int(half_dipoles)):
#bend
loc=loc+space
fid.write('DIP%d:MBS, at=%f;\n'%(int(dip), float(loc)))
dip=dip+1
#defocus
loc=loc+space
fid.write('qd%d:qdType, at=%f;\n'%(int(offset), float(loc)))
for kk in xrange (int(half_dipoles)):
#bend
loc=loc+space
fid.write('DIP%d:MBS, at=%f;\n'%(int(dip), float(loc)))
dip=dip+1
loc=loc+space
fid.write('\n')
###############################################################
offset = offset+1
print 'offset kk = %d= '%int(kk)
print offset
print '\n'
fid.write('/*cell%d*/\n'%(int(offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(offset), float(loc)))
#defocus
loc=loc+(straight_drift*space)
fid.write('qd%d:qdType, at=%f;\n'%(int(offset), float(loc)))
loc=loc+(straight_drift*space)
offset = offset+1
fid.write('\n')
print 'End dispersion suppressor'
print '\n'
######## End of dispersion suppressor ########
########################################################################################################################################
for ii in xrange(int(full_cells)):
fid.write('/*cell%d*/\n'%(int(ii+offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(ii+offset), float(loc)))
#add sextupole next to quadrupole
fid.write('sf%d:sfType, at=%f;\n'%(int(ii+offset), float(loc)))
for kk in xrange (int(half_dipoles)):
#bend
loc=loc+space
fid.write('DIP%d:MBS, at=%f;\n'%(int(dip), float(loc)))
dip=dip+1
#defocus
loc=loc+space
fid.write('qd%d:qdType, at=%f;\n'%(int(ii+offset), float(loc)))
#add sextupole next to quadrupole
fid.write('sd%d:sdType, at=%f;\n'%(int(ii+offset), float(loc)))
for kk in xrange (int(half_dipoles)):
#bend
loc=loc+space
fid.write('DIP%d:MBS, at=%f;\n'%(int(dip), float(loc)))
dip=dip+1
loc=loc+space
fid.write('\n')
print 'offset jj = %d ii = %d= '%(int(jj),int(ii))
print offset
print '\n'
########################################################################################################################################
######## Dispersion suppressor ########
print 'Begin dispersion suppressor'
print '\n'
offset = offset+ii+1
print 'offset jj = %d ii = %d= '%(int(jj),int(ii))
print offset
print '\n'
fid.write('/*cell%d*/\n'%(int(offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(offset), float(loc)))
#defocus
loc=loc+(straight_drift*space)
fid.write('qd%d:qdType, at=%f;\n'%(int(offset), float(loc)))
loc=loc+(straight_drift*space)
fid.write('\n')
###############################################################
offset = offset+1
print 'offset jj = %d ii = %d= '%(int(jj),int(ii))
print offset
print '\n'
fid.write('/*cell%d*/\n'%(int(offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(offset), float(loc)))
for kk in xrange (int(half_dipoles)):
#bend
loc=loc+space
fid.write('DIP%d:MBS, at=%f;\n'%(int(dip), float(loc)))
dip=dip+1
#defocus
loc=loc+space
fid.write('qd%d:qdType, at=%f;\n'%(int(offset), float(loc)))
for kk in xrange (int(half_dipoles)):
#bend
loc=loc+space
fid.write('DIP%d:MBS, at=%f;\n'%(int(dip), float(loc)))
dip=dip+1
loc=loc+space
fid.write('\n')
print 'End dispersion suppressor'
print '\n'
######## End of dispersion suppressor ########
########################################################################################################################################
print 'Begin half straight section '
print '\n'
#first half of the drift space
offset = offset+1
print 'offset jj = %d ii = %d= '%(int(jj),int(ii))
print offset
print '\n'
for rr in xrange(straight_cells/2):
fid.write('/*cell%d*/\n'%(int(rr+offset)))
#focus
fid.write('qf%d:qfType, at=%f;\n'%(int(rr+offset), float(loc)))
#defocus
loc=loc+(straight_drift*space)
fid.write('qd%d:qdType, at=%f;\n'%(int(rr+offset), float(loc)))
loc=loc+(straight_drift*space)
fid.write('\n')
offset = offset+rr+1
print 'offset rr = %d= '%int(rr)
print offset
print '\n'
########################################################################################################################################
fid.write('ENDSEQUENCE;\n')
#Set RF cavities
fid.write('CAV1, volt=0.1, lag=0.5, harmon=35000;\n')
fid.write(con)
fid.write(matching_begin)
fid.write('global, sequence = fodo, DQ1 =%f;\n'%(float(DQ1)))
fid.write('global, sequence = fodo, DQ2 =%f;\n'%(float(DQ2)))
fid.write('global, sequence = fodo, Q1 =%f;\n'%(float(Qx_total)))
fid.write('global, sequence = fodo, Q2 =%f;'%(float(Qy_total)))
fid.write(matching_end)
fid.write(plots)
fid.write(twiss)
#change voltage!
fid.write('CAV1, volt=10, lag=0.5, harmon=35000;\n')
#tracking
fid.write('track,file=track_master%d.out,dump;'%(DQ1))
fid.write(track)
fid.write('run,turns=%d;\n'%(TURNS))
fid.write('endtrack;\n')
fid.write('stop;\n')