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DESY Accelerator Physics Seminar February, 9 th 2010 1 Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar February, 9 th 2010

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Page 1: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 1

Operational Experience with the LHC and SPS Tune Resonance Phenomena

Tobias Baer

DESY Accelerator Physics Seminar

February, 9th 2010

Page 2: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 2

Content

1. CERN Accelerator Complex

2. Operational Experience with the LHC

3. Tune Resonance Phenomena in the SPS and Machine Protection via Fast Position Interlocking

Page 3: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 3

1. CERN Accelerator Complex

2. Operational Experience with the LHC

3. Tune Resonance Phenomena in the SPS and Machine Protection via Fast Position Interlocking

Page 4: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 4

CERN

Mt. Blanc

Lake Geneva

CMS

Geneva

LHCb

ATLAS

ALICE

Page 5: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 5

CERN Accelerator Complex

Page 6: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 6

• Ring circumference: 26.7 km

• Collision Energy: 2 ∙ 7 TeV

• 4+2 Experiments: ATLAS, CMS, ALICE, LHCb andTOTEM, LHCf

Large Hadron Collider

Page 7: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 7

1. CERN Accelerator Complex

2. Operational Experience with the LHC

3. Tune Resonance Phenomena in the SPS and Machine Protection via Fast Position Interlocking

Page 8: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 8

• LHC incident

• LHC run 2009

• Plans for 2010

2. Operational Experience with the LHC

Page 9: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 9

LHC startup 2008

LHC startup: September 10th 2008

• Both beams around the ring (within few hours)

Following days:

• All base instrumentation operational (BPMs, BLMs, Tune, BCTs)

• Beam 2 captured by RF

• Beam lifetime > 1h

Page 10: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 10

September 19th Incident

Quadrupole-dipole interconnection (27R3)

Page 11: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 11

September 19th Incident

Quadrupole-dipole interconnection (27R3)

Vacuum chamber

Dipole Bus bar

Page 12: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 12

Bus Bar

Page 13: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 13

Bus Bar

bus U-profile bus

wedge

Solder

bus U-profile bus

wedge

Solder No solder

Good joint

Bad joint

Page 14: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 14

Event Sequence on Sept. 19th

• Last commissioning step of main dipole circuit in sector 34: ramp to 9.3 kA (5.5 TeV)

• At 8.7 kA electrical fault in bus bar between dipole and quadrupole

Local resistance: ~220 nW (nominal 0.35 nW)

• 400MJ out of 600MJ stored in the circuit were dissipated in cold-mass and electrical arcs

• 6 tons of helium were released

Page 15: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 15

LHC repairs in detail

14 quadrupolemagnets replaced

39 dipole magnets replaced

204 electrical inter-connections repaired

Over 4km of vacuum beam tube cleaned

New longitudinal restraining system for 50 quadrupoles

Almost 900 new helium pressure release ports

6500 new detectors and 250km cables for new Quench Protection System

Page 16: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 16

LHC run 2009

Page 17: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 17

Startup Nov. 20th 2009

Beam position

Also Day 1: Capture of both beams with RF

Page 18: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 18

Startup Nov. 20th 2009

Page 19: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 19

First Collisions

Day 4: First collisions at 2∙450 GeV

ATLAS CMS

Page 20: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 20

Ramp

Day 4: 1st Ramp to 560 GeV

Day 11: 3rd Ramp to 1.18 TeV

Page 21: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 21

3rd Ramp

Page 22: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 22

Tune = Number of betatron oscillations per machine revolution

Tune

S=0 Closed Orbit

Page 23: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 23

Tune = Number of betatron oscillations per machine revolution

Tune

S=0 Closed Orbit

Page 24: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 24

Tune = Number of betatron oscillations per machine revolution

Tune

S=0

QH ≈ 7.6

Closed Orbit

BetatronOscillation

Page 25: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 25

Tune = Number of betatron oscillations per machine revolution

Tune Resonance: m∙QH±n∙QV=k m, n, k = integer

m+n = order of resonance

Tune

S=0

QH ≈ 7.6

Closed Orbit

BetatronOscillation

Page 26: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 26

Ramp to 1.18 TeV

Page 27: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 27

CMS Solenoid

Day 10: Switching on CMS Solenoid.

Orbit difference with/without Solenoid on

Momentum change: dp/p = -0.1 ‰

Page 28: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 28

Tidal Effect on Energy

LHC measures influence of tidal forces 10 days after first beam

Page 29: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 29

Milestones in 2009 run

Date Day Achieved

Nov 20 1 Both beams circulating. Key beam instrumentation working.

Nov 23 4 First collisions at 450 GeV. First ramp (reached 560 GeV).

Nov 30 11 Ramp to 1.18 TeV.

Nov 30 11 Experiment solenoids on.

Dec 04 15 Aperture measurements finished. LHCb and ALICE dipoles on.

Dec 05 16 Machine protection (Injection, Beam dump, Collimators) ready for safe operation with pilots.

Dec 08 19 Ramp colliding bunches to 1.18 TeV

Dec 14 25 Collisions with STABLE BEAMS, 16 on 16 bunches at 450 GeV,Intensity > 1010 protons per bunch

Dec 16 27 Ramp 4 on 4 bunches to 1.18 TeV. Squeeze to β*=7 m.

Page 30: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 30

Plans for 2010

Page 31: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 31

Plans for 2010

Date Activity

Feb 16 Injection Test

Feb 22 Start recommissioning with Beam

End Feb Ramp to 3.5 TeV.

Beg. Mar Commission Squeeze

Mid Mar Stable, Save Beams at 3.5 TeV

Stepwise Increase Intensity, each step followed by extended running period (estimate: up to ≈7∙1013 protons during 2010)

Ramp to Higher Energies in 2013 (warm up of machine needed)

Page 32: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 32

1. CERN Accelerator Complex

2. Operational Experience with the LHC

3. Tune Resonance Phenomena in the SPS and Machine Protection via Fast Position Interlocking

Page 33: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 33

• Incident 27.06.2008

• Integer Tune resonances

• Orbit Resonance

• Dispersion Resonance

• Supersymmetric Resonances

• Machine Protection

3. Tune Resonance Phenomena in the SPS and Machine Protection via Fast Position Interlocking

Page 34: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 34

• Commissioned in 1976

• Ring circumference: 6.9 km

• Top Energy: 450 GeV

• Intensity: up to5∙1013 protons

• Beam Energy: up to 2.5 MJ

• Tevatron: 2 MJ, LHC (nominal) 362MJ

Super Proton Synchroton

Octupole

Sextupole

Correctors and BI

Quadrupole

4 Dipoles

Page 35: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 35

• Commissioned in 1976

• Ring circumference: 6.9 km

• Top Energy: 450 GeV

• Intensity: up to5∙1013 protons

• Beam Energy: up to 2.5 MJ

• Tevatron: 2 MJ, LHC (nominal) 362MJ

Super Proton Synchroton

Octupole

Sextupole

Correctors and BI

Quadrupole

4 Dipoles

Page 36: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 36

SPS Incident 27.06.2008

Page 37: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 37

SPS Incident June 27th 2008

Beam impact of high intensity beam

(about 3∙1013 protons @ 400 GeV)

Page 38: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 38

SPS Incident June 27th 2008

Beam impact of high intensity beam

(about 3∙1013 protons @ 400 GeV)

Page 39: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 39

Event Sequence on June 27th

• After injection of 2 high intensity batches a failure in the main timing system occurred

• The beam was accelerated to 400GeV but not extracted

• The magnets were ramped down again

• The tune shifted towards an integer tune resonance and the beam punctured the vacuum chamber in the vertical plane (dipole current corresponding to 399.05 GeV)

Page 40: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 40

SPS Incident June 27th 2008

Page 41: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 41

Integer Tune Resonance

Page 42: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 42

Integer Tune Resonance

• Influence of dipolar error on Closed Orbit:

(e.g. quadrupole misalignments)

s

sdQssssFQ

ssx ))()(cos()()(

)sin(2

)()(

Page 43: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 43

Integer Tune Resonance

• Influence of dipolar error on Closed Orbit:

(e.g. quadrupole misalignments)

s

sdQssssFQ

ssx ))()(cos()()(

)sin(2

)()(

Beta functionBetatron phase

Resonance conditionError function Tune

Page 44: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 44

Integer Tune Resonance

• Influence of dipolar error on Closed Orbit:

(e.g. quadrupole misalignments)

• QH, QV = integer => diverging closed orbit

s

sdQssssFQ

ssx ))()(cos()()(

)sin(2

)()(

Beta functionBetatron phase

Resonance conditionError function Tune

Page 45: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 45

Turn-by-Turn Position

Linear Decrease of Horizontal Tune

Page 46: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 46

Orbit Resonances

0

2

4

6

8

10

23.5 24.0 24.5 25.0 25.5 26.0 26.5

Ho

rizo

nta

l RM

S cl

ose

d o

rbit

[m

m]

Horizontal Tune

Horizontal RMS closed orbit

Measurement

Simulation

NominalQH=26.13

Page 47: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 47

Turn-by-Turn Position

Linear Decrease of Horizontal Tune

Page 48: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 48

• Dispersion:

(generated by dipole magnets, transforms like orbit)

Dispersion Resonance

p

psDsx

)()(

Page 49: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 49

• Dispersion:

(generated by dipole magnets, transforms like orbit)

Error function

Dispersion Resonance

Beta functionBetatron phase

Resonance condition

p

psDsx

)()(

s

sdQssssFQ

ssx ))()(cos()()(

)sin(2

)()(

Tune

Page 50: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 50

• Dispersion:

(generated by dipole magnets, transforms like orbit)

Error function

Dispersion Resonance

Beta functionBetatron phase

Resonance condition

p

psDsx

)()(

s

sdQssssFQ

ssx ))()(cos()()(

)sin(2

)()(

D

)(

1

s

Bending radiusTune

Page 51: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 51

• Dispersion:

(generated by dipole magnets, transforms like orbit)

• QH, QV = integer => diverging dispersion

Error function

Dispersion Resonance

Beta functionBetatron phase

Resonance condition

p

psDsx

)()(

s

sdQssssFQ

ssx ))()(cos()()(

)sin(2

)()(

D

)(

1

s

Bending radiusTune

Page 52: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 52

Dispersion Resonance

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DESY Accelerator Physics SeminarFebruary, 9th 2010 53

Dispersion Resonance

0

5

10

15

20

25

23.5 24.0 24.5 25.0 25.5 26.0 26.5

Ho

rizo

nta

l RM

S D

isp

ers

ion

[m

]

Horizontal Tune

Horizontal RMS Dispersion

MeasurementMeasurement (Shifted Tune)Simulation

NominalQH=26.13

Page 54: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 54

SPS: Supersymmetry of 6

Supersymmetric Resonances

Page 55: Operational Experience with the LHC and SPS Tune Resonance ... · Operational Experience with the LHC and SPS Tune Resonance Phenomena Tobias Baer DESY Accelerator Physics Seminar

DESY Accelerator Physics SeminarFebruary, 9th 2010 55

SPS: Supersymmetry of 6

Supersymmetric Resonances

1

2 3

4

56

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DESY Accelerator Physics SeminarFebruary, 9th 2010 56

Supersymmetric Resonances

1

2 3

4

56

SPS: Supersymmetry of 6

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DESY Accelerator Physics SeminarFebruary, 9th 2010 57

Supersymmetric Resonances

1

2 3

4

56

SPS: Supersymmetry of 6

• When Tune is multiple of 6:

Extreme Dispersion Resonance

• Dipole fields are super-symmetric

Integer Orbit Resonance

• Dipole errors are randomly distributed (no strong supersymmetry)

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DESY Accelerator Physics SeminarFebruary, 9th 2010 58

Machine Protection

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DESY Accelerator Physics SeminarFebruary, 9th 2010 59

Power Converter Interlock

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DESY Accelerator Physics SeminarFebruary, 9th 2010 60

Fast Position Interlock

• Original Design:

• 6 stripline coupler BPMs

• new Hardware using logarithmic amplifiers (large dynamic range)

• Turn-by-Turn Acquisition and Interlock Processing via FPGA

• Post Mortem Acquisition (1024 turns)

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DESY Accelerator Physics SeminarFebruary, 9th 2010 61

Acquisition Commissioning

y = 0.60x - 0.79

y = 0.59x - 0.39

-8

-6

-4

-2

0

2

4

6

8

-8 -6 -4 -2 0 2 4 6 8

vert

ical

po

siti

on

me

asu

red

by

new

HW

[m

m]

vertical position measured by MOPOS [mm]

New Hardware vs. Traditional Hardware(vertical orbit bump)

BPCE.618 V-position @ injection

BPCE.618 V-position @ 49 GeV

07 - 09.11.2009, CNGS beam@ injection: 14GeV, 2∙1013 p

@ 49GeV: 4∙1013 p

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DESY Accelerator Physics SeminarFebruary, 9th 2010 62

Acquisition Commissioning

Consistency Check:Vertical 3π orbit bump at BPCE 618

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DESY Accelerator Physics SeminarFebruary, 9th 2010 63

Acquisition Commissioning

y = 0.97x - 0.14y = 1.06x - 0.08

y = 1.76x - 0.07

-6

-4

-2

0

2

4

6

8

-4 -3 -2 -1 0 1 2 3 4

vert

ical

po

siti

on

me

asu

red

/tri

mm

ed

[m

m]

fitted bump amplitude @ BPCE.618.V [mm]

New Hardware vs. Traditional Hardware(3π vertical orbit bump)

Nominal Trim

BPCE.618.V new hardware

BPCE.618.V MOPOS

12.11.2009, CNGS beam14GeV, 2∙1013 p

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DESY Accelerator Physics SeminarFebruary, 9th 2010 64

• Compare current position with moving average of last 100 turns

• Interlock if difference larger 3mm

• Outlier detection

Interlock Algorithm

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DESY Accelerator Physics SeminarFebruary, 9th 2010 65

Interlock Algorithm

• Compare current position with moving average of last 100 turns

• Interlock if difference larger 3mm

• Outlier detection

Problem: Injection Oscillations

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DESY Accelerator Physics SeminarFebruary, 9th 2010 66

Interlock Algorithm

• Compare current position with moving average of last 100 turns

• Interlock if difference larger 3mm

• Outlier detection

Problem: Injection Oscillations

• Probable solution:

(Time dependent) Low pass filter

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DESY Accelerator Physics SeminarFebruary, 9th 2010 67

Fast Position Interlock

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DESY Accelerator Physics SeminarFebruary, 9th 2010 68

Fast Position Interlock

Offline test: 428/428 tune resonances triggered, 0/554 normal orbits triggered

in-situ tests continue next week

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DESY Accelerator Physics SeminarFebruary, 9th 2010 69

Summary

• (Integer) Tune Resonance are a challenging Machine Protection Issue

• (cp. complete beam loss in 3 turns)

• Protection with Turn-by-Turn Position Interlock

• When you are fast enough you can cross every resonance

• Be aware of Supersymmetric Tune Resonances

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DESY Accelerator Physics SeminarFebruary, 9th 2010 70

Thank you

for your Attention

Tobias Baer

CERN BE/OP

[email protected]

[email protected]

Office: +41 22 76 75379

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DESY Accelerator Physics SeminarFebruary, 9th 2010 71

Backup slides

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DESY Accelerator Physics SeminarFebruary, 9th 2010 72

LHC Main Dipole Circuit

Global protection of the bus-bar and bus-bar joints (splices) between magnets.

Protection threshold 1 V (160 V inductive voltage during ramp).

Bus-bar must cope with 100 second discharge time of circuit.

Local (quench) protection of each magnet

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Beam Screen Contamination

Beam Screen (BS) : The red color is characteristic of a clean copper

surface

BS with some contamination by super-isolation (MLI multi layer

insulation)

BS with soot contamination. The grey color varies depending on the thickness of the soot, from grey to

dark.

Beam screen with clean Copper surface

contaminated by super-isolation

contaminated with soot

60% of the chambers 20% of the chambers

Beam Screen (BS) : The red color is characteristic of a clean copper

surface

BS with some contamination by super-isolation (MLI multi layer

insulation)

BS with soot contamination. The grey color varies depending on the thickness of the soot, from grey to

dark.

Beam Screen (BS) : The red color is characteristic of a clean copper

surface

BS with some contamination by super-isolation (MLI multi layer

insulation)

BS with soot contamination. The grey color varies depending on the thickness of the soot, from grey to

dark.

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Cleaning of Beam Screen

Up to 50 passages in each direction with wet foam (alcohol)

Up to 15 passages with dry foam

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DESY Accelerator Physics SeminarFebruary, 9th 2010 75

Triplet Movement

12µm triplet misalignment => beam oscillation amplitude 0.3mm (in arc)

7.454

7.456

7.458

7.460

7.462

7.464

7.466

7.468

7.470

20:30 21:00 21:30 22:00 22:30 23:00 23:30 0:00

po

siti

on

[m

m]

time (UTC)

Haiti Earthquake (12.01.2010) measured by LHC hydrostatic leveling system

GISB.UX851R.HLS_LO:HEIGHT_MM

21:53 Earthquake

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Triplet Movement

-0.800

-0.600

-0.400

-0.200

0.000

0.200

0.400

0.600

0.800

1.000

vert

ical

po

siti

on

[m

m]

s [m]

12µm Misalignment of MQXB.A2R5

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Hump and UPS

Hump: Fast frequency shifting oscillation Time resolved Hump structure

with mean drifting slowly between0.25 and 0.32

courtesy of Ralph Steinhagen

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Dispersion Resonance

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Dispersion Resonance

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Dispersion Resonance

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Dispersion Resonance

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FMCM

Recombination Dipole RD1 OFF, FMCM active

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FMCM

Recombination Dipole RD1 OFF, FMCM masked (inactive)

83

orbit starts to change 270 turns = 23.9 ms before beam dump

00:21:29.4200orbit start to change 00:21:29.3961

FMCM masked trigger 00:21:29.378

beam losses start at00:21:29.4020

courtesy of Rudiger Schmidt

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Beam Losses

Recombination Dipole RD1 OFF, FMCM masked (inactive)

courtesy of Rudiger Schmidt

beam losses start at00:21:29.402

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Power Converter

Recombination Dipole RD1 OFF, FMCM masked (inactive)

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Power Converter

Recombination Dipole RD1 OFF, FMCM masked (inactive)

BLM trigger: 00:21:29.420

dI = 0.69 A (1.6%)Inom = 43.17 AIdump = 42.42 A

orbit starts to change 00:21:29.396

FMCM trigger

dI=0.025%

courtesy of Rudiger Schmidt

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