Injection path for MR & particle losses at MR_SCR

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Injection path for MR & particle losses at MR_SCR Alexander Molodozhenstev KEK MR commissioning group January 17, 2006

description

Injection path for MR & particle losses at MR_SCR. Alexander Molodozhenstev KEK MR commissioning group January 17, 2006. Schematic layout of Injection Path for MR. Beam from RCS. BP2. BP1. BP3. Kicker magnets. Magnet Septum. Circulating beam. QDX. QFR. QDT. QFP. - PowerPoint PPT Presentation

Transcript of Injection path for MR & particle losses at MR_SCR

Page 1: Injection path for MR & particle losses at MR_SCR

Injection path for MR &particle losses at MR_SCR

Alexander MolodozhenstevKEK

MR commissioning groupJanuary 17, 2006

Page 2: Injection path for MR & particle losses at MR_SCR

Schematic layout of Injection Path for MR

Circulating beam

Beam from RCS

QDXQFPQDTQFR

BP

1

BP

2

BP

3

Mag

net

Sep

tum

Kic

ker

ma

gn

ets

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Scheme of the INJECTION path (April, 2005) … SAD data

70 75 80 85 90 95-0.025

-0.020

-0.015

-0.010

-0.005

0.000

0.005

0.010

COD during INJECTION

Circulating Beam

QFR QDT QFP

BP#3 BP#2 BP#1

OPMS: 3-2-1

INJECTION:Bumps & OPMS

x [m

]

z [m]

Page 4: Injection path for MR & particle losses at MR_SCR

Time pattern (h=9) 1st batch

~ 1 msec~ 200 turns

2nd batch 3rd batch 4th batch

40 msec~ 7’435 turns

OPMS

BP

Opposite Field Magnet Septum – PULSE (sinusoidal)Bump Magnets – like DC

~850nsec

~ 120 msec

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Parameters of the INJECTION beam-line (SAD data)

Elements Strength (k0L)

[rad]

Effective Length

[m]

BP1 0.0024269618 0.20

BP2 -0.0063929115 0.50

BP3 0.0020820796 0.20

OPMS5 -0.01649460 0.35

OPMS4 0.03298920 0.70

OPMS3 -0.01649460 0.35

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Elements representation (for MAD & ORBIT)

Elements Eff.Length [m] Theta [rad] E1 [rad] E2 [rad]

BP1 0.20 0.00242269 0.0 0.0024

BP2 0.50 -0.0063929 -0.0023 -0.0041

BP3 0.20 0.00208207 0.0021 0.0

OPMS5 0.35 -0.0164946 -0.0023 -0.0142

OPMS4 0.70 0.03298920 0.0142 0.0187

OPMS3 0.35 -0.0164946 -0.0187 0.0023

QFP 1.76 … as quadrupole

QFR 0.86 … as quadrupole

QDT 1.86 … as COMBINED function BM plus Edge Focusing:

xCOD ~ 0.02m, e1=-0.002, e2=+0.002

* Edge focusing effect will lead to the vertical beta-beating

Page 7: Injection path for MR & particle losses at MR_SCR

INJECTION_Path_MR Lattice parameters

Qx = 22.4279 (22.4281)Qy = 20.8227 (20.8199)x,max = 40.715m (40.812m)y,max = 33.922m (33.257m)Dx,max = 3.072m (3.057m)

With OMS

ORIGINAL

Without OMS

Qx = 22.4281Qy = 20.8195x,max = 40.818my,max = 33.197mDx,max = 3.057m

D:\Alex\Work\2005\MR\MAD\mad050509I_for_ORBIT_YES_Inj_Bump\Teapot_ORBIT_Tracker\22428_20819\Yes_CCSX\Test#3_COD\Check_Dec05\DR_Short\INJD_short.mad

Vertical -beating ~ 2…3 % (without quadrupole components of OMS)

Page 8: Injection path for MR & particle losses at MR_SCR

Simulation approach #1

#1 … Lattice with BP & OMS (rectangular pulse) & CFQDT:: 200 turns#2 … Lattice with BP & --- & CFQDT :: 7’235 turns

Page 9: Injection path for MR & particle losses at MR_SCR

Simulation approach #2

• RCS 0.6MW beam (v050906/Transverse:: 95254mp)• RCS_MR Beamline Collimator :: 54 mm.mrad (90935mp)• Matched beam at MR_SCR position for Qx=22.428, Qy=20.82 including injection

dogleg• Sextupole magnets for chromaticity correction are ON

• Uniform Longitudinal distribution: = ± 60 degree (Bf = 0.3), p/p = ± 0.002• MR scraper acceptance = 70 mm.mrad• RF:: h=9; VRF= 140 / 91 kV• Beampipe:: Rectangular shape / size(X,Y) = ± 70 mm• NFFT: 100×100 / Nbin: 512 / z < 1.5m

• INJECTION DOGLEG:: Bump Magnets (1,2,3) + Opposite Field Magnet Septums (1,2,3) + Combined Function QDT

• Different conditions for Bump Magnets and Opposite Field Magnet Septums…(#1: DC for ALL; #2: DC for Bumps and PUSLE for Opposite MS; #3: only DC Bumps)

• Overall number of turns = 2’000.

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NO Injection Dogleg

MRSCR=70 mm.mrad

99% emittance LOST particles

V

H

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Case 1: DC for ALL elements of INJECTION dogleg

V

H

99% emittance LOST particles

2000 turns BP & OMS & CFQDT …

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Case 2: DC for Bump-magnets and PULSE for OMS of INJECTION dogleg

V

H

99% emittance LOST particles

200 turns BP & OMS & CFQDTplus 1800 turns BP & CFQDT …

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Footprint for case #2

4Qx

= 9

0

4Qy = 83

4Qx=

89

2Q x–2Q y

=3

3Qx=

67

Qx+2Q

y=64

-Qx+2Q y

=19

Only Space-Charge resonancesand Normal Sextupole resonancesare indicated

Qx

Qy

Red – Space Charge resonancesBlue – Normal Sextupole resonances

after 2000turns

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Case 1_2: DC for ALL elements of INJECTION dogleg

NO CC_Sextupoles, dp=0

99% emittance LOST particles

2000 turns BP & OMS & CFQDT …

NO_CCSX:: dp/p = 0 NO influence of Normal Sextupole Resonances

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99% Emittance behavior during the injection process (MR_SCR70)

V

H

Page 16: Injection path for MR & particle losses at MR_SCR

Particle losses at MR_SCR70 during injection process

1.63%

0.92%

0.35%

0.10 %

120msec40msec 80msec

1st batch

2nd batch

3rd batch

4th batch

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Budget of MR particle lossesSingle bunch power of the case of 0.6MW beam from RCS (h=9, 8 bunches) is 3.56kW.

Power of the lost beam at the injection energy for each batch …

1 batch 2 batch 3 batch 4 batch

~ 116 W ~ 66 W ~ 25 W ~ 7.2 W

Total power of the lost beam at the injection energy for 8 bunches ~ 214 W (120msec injection time) … < 450W !!!

Injection time:: 120 msec

RCS_Beam (TR::v050906, LD::Uniform)MR_SCR_Acceptance = 70 π mm.mrad (CLM54 in RCS_MR_BeamLine)

Page 18: Injection path for MR & particle losses at MR_SCR

… continue

(1) Introduction of realistic field-error of the MR magnets

(2) Introduction of misalignment of MR magnets (excitation of skew-resonances)