study and optimization of dynamic aperture for the superkekb ler e.levichev and p.piminov, binp sb...

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Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

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Page 1: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Study and Optimization of Dynamic Aperture for the SuperKEKB LER

E.Levichev and P.Piminov,

BINP SB RAS, Novosibirsk, Russia

Page 2: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

LER Main Parameters

Parameter Value Unit

Circumference, L 3.0162 km

Energy 4.0 GeV

Horizontal emittance, εx 5.77 nm·rad

Compaction factor, α 2.76·10 -4

Betatron tunes, νx/νz 45.53/45.57

Natural chromaticity, ξx/ξz -107.4/-807.5

Comp. chromaticity, ξx/ξz -0.76/-3.66

Horizontal beta @ IP 3 cm

Vertical beta @ IP 270 um

Horizontal sigma 13 um

Vertical sigma 0.08 um

(the lattice from ItalyIP19B-work3c3.sad)

Page 3: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

IR Optical Functions

Page 4: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Main sources of the DA limitation

• QC1 fringe field

• Vertical sextupoles SL2

• QC2 fringe field

• Kinematics term

• Fringe fields of other quadrupoles

• Arc sextupoles

In order of weakening

Page 5: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

DA from the main nonlinearities

QC2

Kinematic

QC1SL2

Other lenses

Page 6: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

QC1 and QC2 DA optimizationQC1 and QC2 fringes can be compensated by octupole corrector distributed in the quad + separate octupoles in the IR vertical chromatic section

Magenta – QC1&QC2 fringes corrected, green – QC1&QC2 + other quads corrected, blue – QC1&QC2 + other quads + kinematics corrected, black – uncorrected DA

Page 7: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

SL2 sextupoles optimizationThick SL2 sextupoles are corrected by additional low strength sextupole correctors placed close to the main ones

Blue – corrected SL2 sexts, red – all other sextupoles added, black – uncorrected DA

Page 8: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Situation before global sextupole optimization

Tune momentum dependence. Black – initial one: horizontal tune for positive and negative momentum deviation goes to 0.5 at ±1.4%; vertical tune for -1% goes to 0.5. This value define the bandwidth. Red is after optimization.

On- and off- energy dynamic aperture. Synchrotron oscillations are on

Page 9: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Global sextupole optimization

Tune momentum dependence after global sextupole optimization (red). The bandwidth increases to –2.4%, +2.2%

On- and off- energy dynamic aperture is also increases after global sextupole optimization. Synchrotron oscillations are on

Page 10: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Horizontal DA vs momentum deviation

Black is initial, red is final

Page 11: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

DA tune scan

(Very preliminary, resolution is poor)Such scans are useful for the DA optimization together with luminosity optimization

Horizontal DA to the left and vertical DA to the right. Color indicates the DA size.High order resonances are not identified yet.

Page 12: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Recommendations for the Crab Sextupoles Insertion

- The best location for the crab sextupoles is seems just after the chromatic correction sections. - The chromatic correction sections could be designed more compact and the vertical beta (as it seems) may be decreased- It is better to arrange linear and the nonlinear dispersion function zero in the crab sextupole- Arcs is not a proper place for the crab sextupoles from our experience- Additional sextupole compensator to correction the length effects of the crab sextupoles can be applied- In principle, our experts can consider the linear optics for the crab sextupoles insertion

Page 13: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

CRAB = 0, IR Sext = 0

CRAB = 0

CRAB = 1

Y Sections

Distorted by CRAB

Spin Rotators

Distorted by arc sexts

Example from SuperB: Distortion of the particle motion due to nonlinear coupling

Picture show horizontal envelope of the last stable vertical trajectory vs azimuth of the storage ring.

CRAB+ CRAB-

Page 14: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

Compact Y Chromatic SectionBeta functions of the Vertical Chromatic Section of the Super-Tau-Charm Factory

0,0,2

@0

10

minmax

minmax

minmax

M

Bmax

Bmin

M(1→2) M(2→3)=-I1 2 3

minmax31 )22( L

Page 15: Study and Optimization of Dynamic Aperture for the SuperKEKB LER E.Levichev and P.Piminov, BINP SB RAS, Novosibirsk, Russia

After several optimization steps, it was managed to improve the dynamic aperture of the SuperKEKB LER for both on-and off-momentum particles. The quadrupole fringe field nonlinearities and kinematical effects were compensated by octupole correctors inserted in the FF quadrupoles (main sources of perturbation of this kind). The strong sextupoles of the IR vertical chromatic section, which deteriorate the dynamic aperture through the third order aberration terms, can be corrected by small additional sextupole correctors placed in the same section. Global optimization of all sextupole families by simplex method allows increasing the dynamic aperture for on- anf off-momentum cases.

The same algorithm can be applied to the HER of the SuperKEKB project.

As the strong crab sextupoles can reduce the dynamic aperture just like the SL2 sextupoles in the vertical chromatic section, their influence can be corrected by the same low strength sextupoles located in the vicinity of the main sextupoles.

Summary