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TLEP ... Lattice Design & Beam Optics

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TLEP ... Lattice Design & Beam Optics. Parameter-List on TKLEP-WEB Page !! emittance !!. Reminder: TLEP . . . the very first steps. TLEP ... Lattice Design ... Version 1...2. Arc : 96 standard FoDo cells & 2 half bend cells at beginning and end length of arc: 2.8km - PowerPoint PPT Presentation
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TLEP ... Lattice Design & Beam Optics Parameter-List on TKLEP-WEB Page !! emittance !!
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Page 1: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design & Beam Optics

Parameter-List on TKLEP-WEB Page!! emittance !!

Page 2: TLEP   ... Lattice Design & Beam Optics

Reminder: TLEP ... the very first steps

Page 3: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design ... Version 1...2

Arc: 96 standard FoDo cells & 2 half bend cells at beginning and endlength of arc: 2.8kmlength of straight section: 0.45 km

Dx

Page 4: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design

Arc: the single FoDo cell

until now ... 2 dipoles / 2 quadrupoles to be optimised according to hardware engineering

short cell length: ≈ 30 m

advantage: small betas small dispersion small emittance

but: realistic hardware design ?

Page 5: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design

Arc: the single FoDo cellphase advance: 900 / 600

to be discussed ...900 horizontally: small dispersion & emittance600 vertically: small beam size (βy) and better orbit correction tolerance (LEP experience)

1 36.8 72.6 108.4 144.2 1800

6

12

18

24

3030

0

max ( )

min ( )

1801

Page 6: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design (175 GeV) not the very first steps anymore (... V9.e)

Text-Book like approach

still 80 km, standard FoDo structure fill factor, robustness, easy to handle & modifyeasy to understand & optimise analytically

Choice of single cell: compared to V.3 ...V.6 cell length increased to Lcell = 50m

ε = δpp

⎛ ⎝ ⎜

⎞ ⎠ ⎟2

γD2 + 2αD ′ D + β ′ D 2( )equilibrium emittance

scaling of dispersion in a FoDo

ˆ D = l 2

ρ*

(1+ 12

sinψ cell

2)

sin2 ψ cell

20 30 60 90 120 150 180

0

2

4

6

8

1010

0.5

D max ( )

D min ( )

1801

Main modifications wrt. previous versions: longer cells to achieve higher dispersion values

Page 7: TLEP   ... Lattice Design & Beam Optics

TLEP ... single cell

Lcell=50m

Dipole: Ndipole = 2932 Ldipole = 21.3 m

due to techn. reasons: 2 * 11 m bending angle = 2.14 mrad B0 = 580 Γ

Quadrupole (arc):Lquadrupole = 1.5 mk=3.55*10-2 m-2 g=20.7 T/maperture: r0=30σ =11mm

Btip= 0.23 Tβ ≈ 100m, Dx= 15.3 cm

FoDo CellAt present the dipole length is “symbolic”. Due to technical reasons we think of putting 2 dipoles of 11m length each between the quads

Page 8: TLEP   ... Lattice Design & Beam Optics

TLEP ... mini beta hardwareL*= 4m

Quadrupole (mini-β):Lquadrupole = 0.75 mk=0.43 m-2 g = k*Bρ ≈ 250 T/m

aperture assumption: r0=30σ

pole tip field:

-> scale mini-β quad length to 7.5m

B0 = 0.75 T

σ x = εxβ x = 2nm * 600m=1.1mm

σ y = εyβ y = 0.002nm *18000m

=0.19mm

B0 ≈30mm *250T /m=7.5T

* beam separation / crossing angle / synchrotron radiation / beam-beam interaction in the vicinity of strong quadrupole gradients

Page 9: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design

24 Arcs : built out of 56 standard FoDo cells & 2 half bend cells at beginning and endlength of arc: ≈ 3.0kmeach arc is embedded in dispersion free regions ...

arcs are connected by straight. sections ... 12 long (mini β and RF) ... 12 ultra shorties tbc

to be optimised

Page 10: TLEP   ... Lattice Design & Beam Optics

TLEP Octant

Straight – Arc – Arc – Straightarcs are connected in pairs via a disp-free-empty cell-> only reason: in case of additional insertions we get the boundary conditions for free.

Page 11: TLEP   ... Lattice Design & Beam Optics

TLEP Arc-Straights

8 Straights : 9 empty (i.e. dispersion free) FoDo cells including matching sections arc-straight, l = 450m

arc cells empty cells arc cells empty cells

to be optimised: βy at matching section, needs an additional quadrupole lens already built in but not used yet. and / or optimisation of the lens positions

Page 12: TLEP   ... Lattice Design & Beam Optics

TLEP Mini-Betas

4 Mini-beta-Insertions : based on empty (i.e. dispersion free) FoDo cells

L*=4mβ*x =1m, β*y =1mm

standard doublet structure & matching sectionβm,ax =18 km

Page 13: TLEP   ... Lattice Design & Beam Optics

TLEP The Ringrf-sections

Lring = 79.9km4 min- betas, 24 disp free straights, 12 long straights 8 for rf equipment, 4 for mini-betas & rf

** ** * * * ** * * *

Page 14: TLEP   ... Lattice Design & Beam Optics

TLEP ... new parameter list

Page 15: TLEP   ... Lattice Design & Beam Optics

TLEP ... Lattice Design V9.ebeam dynamics of the ring

Main Parameters:

momentum compaction

energy loss per turn:€

α cp ≈DR

= 11*10−2 mL0 /(2π )

≈ 8.64 *10−6 MADX: αcp =8.94*10-6

η ≈1γ 2 −α cp ≈ −α cp

γ=1750000.511

= 342466

ΔU0(keV ) ≈ 89 * E 4 (GeV )ρ

ΔU0 ≈ 8.4 GeV

Ndipoles = 2932

θ = 2π2932

= 2.14 mrad

MADX: ΔU0=8.2 GeV

E =175GeV , Bρ = 583.33

ρ = LB

θ≈ 9.95km

Page 16: TLEP   ... Lattice Design & Beam Optics

TLEP ... V 9.e

Main Parameters:

Damping & Beam Emittance

Nota bene: Emittance is as before nicely small .. still smaller than the design value (2nm).however for a theoretical, ideal lattice without coupling, beam-beam, solenoid fields,tolerances error tolerances to be considered,

how realistic is 2nm and 1 permille for εy / εx

Page 17: TLEP   ... Lattice Design & Beam Optics

ΔPsy ≈ ΔU0

T0

* N p = 8.2*106eV *1.6 *10−19Cb266*10−6 s

*9 *1012

ΔPsy ≈ 44 MW

Synchrotron Radiation Power175 GeV, 80km

Np = 9*1012

ΔU0 = 8.2 GeVT0 = 266 μs

... and Saw-Tooth effect (still without mini-beta)rf distributed over 12 straights and 216 cavities (60MV each)

Page 18: TLEP   ... Lattice Design & Beam Optics

Next steps:

* Optics fine tuning: including radiation effects

* Do we really need Dx= 15 cm or should we relax ??

* Establish complete versions for different Mini Beta Optionslocal / global Q’ correction

* Optimise RF distributionhow many straights do we really need ???

* Lattice for lower energiesbeam separation ???

* 80 km / 100 km ??? tbd

* start with the Ph.D. topics:what about the momentum acceptance ???

*** define a mid term parameter table ( t >> 2 days )


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