Transport formalism
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Transport formalism. Linear matrix elements. Second order matrix elements. Truncated maps. Violation of the symplectic condition !. Lie algebraic treatment. Dragt-Finn factorization :. generators. [A. Dragt et al., Ann. Rev. Nucl. Part. Sci. 38 (1988) 455]. Linear matrix.

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Transport formalism

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Transport formalism

Transport formalism

Linear matrix elements

Second order matrix elements

Truncated maps

Violation of the symplectic condition !


Lie algebraic treatment

Lie algebraic treatment

Dragt-Finn factorization :

generators

[A. Dragt et al., Ann. Rev. Nucl. Part. Sci. 38 (1988) 455]

Linear matrix

produces Tijkand higher order terms (sextupole effects)

produces third order and higher order terms (octupoles effects)

Numerical methods for nonlinear optimization : PARTICLE TRACKING,

Dynamic aperture scans, particle spectra…


Tracking codes simulations to show the feasibility

Tracking codes:Simulations to show the feasibility

Entrance:

IP:

Importance of the benchmarking of codes

Guinea-Pig

Multiparticle tracking

Optics lattice

Beam-beam

interaction

transport

performance

MAD

Placet

SAD

Lie

[T. Asaka and J. Resta Lopez, CLIC-Note-637]


Nanometer size beams in clic

Nanometer-Size Beams in CLIC

Nominal: σx=40.12 nm; σy=0.55 nm

Simulations: σx≈47.3 nm; σy≈0.65 nm

Beam profile at the IP:

Some problems: Residual horizontal dispersion at the IP


Nanometer size beams in clic1

Nanometer-Size Beams in CLIC

Phase space at the IP:

Particles with lower energy than the nominal one (1500 GeV) contribute strongly

to the tails of the transversal phase space


Chromatic effects in phase space

Chromatic effects in phase space

Chromatic aberrations study by means of tracking from matched initial ellipses at 1σ for the transversal plane X

Red line: center ellipse movement in phase space

up to third order !


Chromatic effects in phase space1

Chromatic effects in phase space

Chromatic aberrations study by means of tracking from matched initial ellipses at 1σ (figure on the left)and 3σ (figure on the right) for the transversal plane Y

The particles at high position amplitude of several sigmas contribute to the

population of the long tails. For the case of the ellipses at 3σ in the vertical

phase space, it is possible to observe a strong deformation of the shape caused by the sextupoles located in the FFS.


Limits of the luminosity

Limits of the Luminosity

L/L0Placet

Without SR

With SR

  • Tolerable bandwidth up to 1 % energy spread

  • The synchrotron radiation is a very important limitation factor for the

  • luminosity


Collimation issues in clic

Collimation issues in CLIC


Beam beam effects

Beam-beam effects

Luminosity versus vertical offset

Analytic calculation considering a rigid gaussian beam:

Simulations with Guinea-Pig: it includes beam-beam effects

Disruption parameters:

Dy= 3.5 (CLIC)

Dy=19.4 (ILC)


Input linac bds beam beam output

ILC integrated simulations

Input LINAC BDS Beam-Beam Output

Updated simulations:

Placet

Guinea-Pig

FB

Simulink

G. White version (2005):

Input LINAC BDS Beam-Beam Output

Placet

Matmerlin

Guinea-Pig

FB

Simulink


Ground motion and fb system

Ground motion and FB system

Nominal: L=2x1034 cm-2s-1

85 % of the nominal

luminosity


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