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LHC: High Luminosity, UFOs and other surprises
Even before the drawing-board stage, the farsighted John Adams noted in 1977 that the tunnel for a future large electron–positron (LEP) collider
should also be big enough to accommodate another ring of magnets.
Rüdiger Schmidt, CERN
23 July 2012
Hadron Collider Summer School
Introduction to the LHC accelerator
Accelerator physics and LHC performance limitations
Machine protection, collimation and UFOs
Beam operation in 2012
Acknowledgements for slides from T.Baer, M.Lamont,
R.Steinhagen, D.Wollmann and J.Wenninger
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LHC: A long story starting in the distant past
First ideas to first protons: from 1984 to 2008 Tears of joy…. first beam in 2008 Tears of sadness…first (and hopefully last) accident in
2008
What doesn’t kill you makes you stronger The story of the champagne bottles
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Introduction to LHC Accelerator Physics Crash Course
• Why protons? Why superconducting magnets? Why “two” accelerators in one tunnel?
LHC layout and beam transport High Luminosity and the consequences High Energy and the consequences Wrapping up: LHC Parameters The CERN accelerator complex: injection and transfer LHC superconducting magnets Machine protection and collimation LHC operation Summary and conclusions
Outline
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Energy and Luminosity
Particle physics requires an accelerator colliding beams with
a centre-of-mass energy substantially exceeding 1 TeV
In order to observe rare events, the luminosity should be in
the order of 1034 [cm-2s-1] (challenge for the LHC accelerator)
Event rate:
Assuming a total cross section of about 100 mbarn for pp
collisions, the event rate for this luminosity is in the order of
109 events/second (challenge for the LHC experiments)
Nuclear and particle physics require heavy ion collisions in
the LHC (quark-gluon plasma .... )
][][ 212 cmscmLtN
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LHC pp and ions
7 TeV/c
26.8 km Circumference
CERN Main Site
SwitzerlandLake Geneva
France
LHC Accelerator (100 m down)
SPS Accelerator
CERN-Prevessin
CMS, TOTEM
ALICE
LHCb
ATLAS
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The LHC: just another collider ?
Start Type Max proton energy [GeV]
Length [m]
B Field [Tesla]
Lumi [cm-2s-1]
Stored beam
energy [MJoule]
TEVATRONFermilab Illinois USA
1983
p-pbar 980 6300 4.5 4.3 1032 1.6 for protons
HERA DESY Hamburg
1992
p – e+p – e-
920 6300 5.5 5.1 1031 2.7 for protons
RHICBrookhavenLong Island
2000
Ion-Ionp-p
250 3834 4.3 1.5 1032 0.9 per proton beam
LHCCERN
2008
Ion-Ionp-p
7000 Now 4000
26800 8.3 1034
Now 6 1033
362 per Namebeam
Factor 7 4 2 50 100
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Accelerator Physics
Crash Course
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The hierarchy in physics
DIE ZEIT 19/07/2012, citing Mike Lamont (Head of CERN accelerator operation):
Und unter den Physikern gebe es eine Hierarchie: »Ganz oben stehen die Theoretiker, dann kommen die Experimentalphysiker und dann wir, die Maschinenleute.«
Among physicists there is a hierarchy: » On top are the theorists, then the experimental physicist, then us, the machine people.«
Accelerator physicist
Experimental physicist
Theorist
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To accelerate a particle to high energy …
Particle energy about 10 kJoule
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To get to 7 TeV: Synchrotron – circular accelerator and many passages in RF cavities
LHC circular machine with energy gain per turn ~0.5 MeVacceleration from 450 GeV to 7 TeV will take about 20 minutes
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Lorentz Force
The force on a charged particle is proportional to the charge, the electric field, and the vector product of velocity and magnetic field:
For an electron or proton the charge is:
Acceleration (increase of energy) only by electrical fields – not by magnetic fields:
][. C106021eq 19
0
)( BvEF
q
EvBvvEv
Fv
qqdtdEdtdE
))((
2
1
s
sE sdF
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Particle deflection: superconducting magnets
The force on a charged particle is proportional to the charge, the electric field, and the vector product of velocity and magnetic field given by Lorentz Force:
)( BvEF
qRe
pB
0
z
x
s
v
B
F• Maximum momentum 7000 GeV/c
• Radius 2805 m fixed by LEP tunnel
• Magnetic field B = 8.33 Tesla
• Iron magnets limited to 2 Tesla, therefore superconducting magnets are required
• Deflecting magnetic fields for two beams in opposite directions
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Deflection by 1232
superconducing dipole
magnets
Superconducting magnets in LHC tunnel
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Particle acceleration: accelerating protons to 7 TeV
Acceleration of the protons in an electrical field with 7 TV
But: no constant electrical
field above some Million Volt (break down)
no time dependent electrical field above some 10 Million Volt (about 30 MV/m)
1 MeV requires U = 1 MV
2s
1s
U sdE
UqqEs
s
s
s
2
1
2
1sdEsdF
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LHC RF frequency 400 MHz
Revolution frequency 11246 Hz
Particle acceleration with RF cavity
)(tE
Time varying field
Maximum field about 20 MV/m
Beams are accelerated in bunches (no continuous beam)
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RF systems: 400 MHz
400 MHz system:
16 sc cavities (copper sputtered with niobium) for 16 MV/beam were built and assembled in four modules
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400 MHz RF buckets and bunches
E
time
RF Voltage
time
LHC bunch spacing = 25 ns = 10 buckets 7.5 m
2.5 ns
The particles are trapped in the RF voltage:this gives the bunch structure
RMS bunch length 11.2 cm 7.6 cmRMS energy spread 0.031% 0.011%
450 GeV 7 TeV
The particles oscillate back and forth in time/energy
RF bucket
2.5 ns
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Limitation of the energy
LEP was operating with electrons and positrons with an
energy of 103 GeV / particle
As a factory for Higgs (?), operation at 120 GeV would be
required (....assuming that ATLAS and CMS results are
confirmed)
This was just a little above the LEP limit
There is a large interest in exceeding the LEP energy by one
order of magnitude (LHC => 7 TeV)
The LHC provides proton – proton collisions
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Radius
Lorenz Force = accelerating force
Particle trajectory Radiation field
charged particle
Figure from K.Wille
Power emitted for one particle: Ps=e0
2 c
6 0 m0 c2 4
E4
2
with E = energy, m0 = rest mass, e0 = charge, and = radius
Energy loss for charged particles by synchrotron radiation
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Energy loss for charged particles electrons / protons in LEP tunnel
Elep 100GeV Elhc 7000GeV
Energy loss for one particle per turn:
Ulep 3.844 109 eV Ulhc 8.121 103 eV
Total power of synchrotronradiation:
Number of electrons in LEP: Nlep 1012 Number of protons in LHC Nlhc 1014
Ptotal_lep Nlep Plep Ptotal_lhc Nlhc Plhc
Ptotal_lep 1.278 107 W Ptotal_lhc 2.699 103 W
The power of the synchrotronradiation emitted at the LHC is very small, but the radiation goes into the supraconducting magnets at 1.9 K ... 20 K
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LHC layout and beam transport
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LHC Layout
eight arcs (sectors)
eight long straight section (about 700 m long) IR4: RF + Beam
instrumentation
IR5:CMS
IR1: ATLAS
IR8: LHC-BIR2: ALICE
InjectionInjectionBeams from SPS
?? ??
??
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Beam transport
Need for getting protons on a circle: dipole magnets
Need for focusing the beams:
Particles with different injection parameters (angle, position) separate with time• Assuming an angle difference of 10-6 rad, two particles would
separate by 1 m after 106 m. At the LHC, with a length of 26860 m, this would be the case after 50 turns (5 ms !)
Particles would „drop“ due to gravitation The beam size must be well controlled
• At the collision point the beam size must be tiny
Particles with (slightly) different energies should stay together
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Magnets and beam stability
Dipole magnets• To make a circle around LHC
Quadrupol magnets• To keep beam particles together• Particle trajectory stable for particles with nominal momentum
Sextupole magnets• To correct the trajectories for off momentum particles • Particle trajectories stable for small amplitudes (about 10 mm)
Multipole-corrector magnets• Sextupole - and decapole corrector magnets at end of dipoles
Particle trajectories can become instable after many turns (even after, say, 106 turns)
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Focusing using lenses as for light beams
f1
x x
Quadrupolemagnet – B-field zero in centre, linear increase (as an optical lense)
Dipolemagnet – B-field in aperture constant
z z
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Assuming proton runs along s (=y), perpendicular to x and z
z
x
zconstz
xconstx
x
z
)(
)(
B
B
x
z
s
z
s
x Side viewfocusing
Looking along protontrajectory
Top viewdefocusing
From Maxwell equations:
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Focusing of a system of two lenses for both planes
d = 50 m
horizontal plane
vertical plane
f1 100m
f2 100 m
d 50m
F1
f1
1
f2
d
f1 f2
1
F 200 m
To focuse the beams in both planes, a succession of focusing and defocusing quadrupole magnets is required: FODO structure
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R.Schmidt
A (F0D0) cell in the LHC arcs
SSS
quadrupoleMQF
sextupole corrector(MCS)
decapoleoctupolecorrector(MCDO)
lattice sextupole
(MS)
lattice sextupole
(MS)
lattice sextupole
(MS)
orbit corrector
special corrector (MQS)
special corrector
(MO)
special corrector
(MO)
quadrupoleMQD
quadrupoleMQF
main dipole
MB
orbit corrector
orbit corrector
main dipole
MB
main dipole
MB
main dipole
MB
main dipole
MB
main dipole
MB
LHC Cell - Length about 110 m (schematic layout)
Vertical / Horizontal plane(QF / QD)
Quadrupole magnets controlling the beam size „to keep protons together“ (similar to optical lenses)
10000 magnets powered in 1700 electrical circuits
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Particle stability and superconducting magnets - Quadrupolar- and multipolar fields
LHC
Teilchenschwingungim Quadrupolfeld(kleine Amplitude)
Harmonische Schwingung(Koordinatentransformation)
Kreisbewegung im Phasenraum
z
y
y
y'
LHC
Teilchenschwingungbei nichlinearen Feldernund grosser Amplitude
Amplitude wächst bis zumTeilchenverlust
Keine Kreisbewegung im Phasenraum
z
y
y
y'
Particle oscillations in quadrupole field (small amplitude)
Harmonic oscillation after coordinate transformation
Circular movement in phase space
Particle oscillation assuming non-linear fields, large amplitude
Amplitude grows until particle is lost (touches aperture)
No circular movement in phasespace
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Relevant parameters to remember
Betatron tune: number of oscillations of a proton within one turn
Closed orbit: deviation of the centre of the bunch from the ideal path (approximately a circle)
Resonances: if the value of the betatron tune is equal to, say, n+0.5 or n+0.3333, the beam is lost
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Betatron tune measurement
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LHC superconducting magnets
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1232 Dipole magnetsLength about 15 m
Magnetic Field 8.3 T
Two beam tubes with an opening of 56 mm
plus many other magnets, to ensure beam stability (1700 main magnets and about 8000 corrector magnets)
Dipole magnets for the LHC
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Coils for Dipolmagnets
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The superconducting state only occurs in a limited domain of temperature, magnetic field and transport current density
Superconducting magnets produce high field with high current density
Lowering the temperature enables better usage of the superconductor, by broadening its working range
T [K]
B [T]
J [kA/mm2]
Operating temperature of superconductors (NbTi)
J [kA/mm2]
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Beam tubes
Supraconducting coil
Nonmagetic collars
Ferromagnetic iron
Steelcylinder for Helium
Insulationvacuum
Supports
Vacuumtank
Dipole magnet cross section16 mBar cooling tube
Quadrupolemagnet
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Operational margin of a superconducting magnet
Temperature [K]
App
lied
field
[T]
Superconductingstate
Normal state
Bc
Tc
9 K
Applied Magnetic Field [T]
Bc critical field
1.9 K
quench with fast loss of ~5 · 109 protons
quench with fast loss of ~5 · 106 protons
8.3 T
0.54 T
QUENCH
Tc critical temperature
Temperature [K]
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Movies dipole magnets
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High Luminosity: many protons in the collider
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High luminosity by colliding trains of bunches
Number of „New Particles“
per unit of time:
The objective for the LHC as proton – proton collider is a luminosity of about 1034 [cm-2s-1]
• LEP (e+e-) : 3-4 1031 [cm-2s-1]• Tevatron (p-pbar) : some 1032 [cm-2s-1]• B-Factories : > 1034 [cm-2s-1]
212 cmscmLT
N
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Luminosity parameters
L =
N … number of protons per bunch … revolution frequency … number of bunches per beam … beam dimensions at interaction point
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Beam beam interaction determines parameters
Beam size 16 m, for = 0.5 m ( is a function of the lattice)
Beam size given by injectors and by space in vacuum chamber
Number of protons per bunch limited to about 1-31011 due to the beam-beam interaction and beam instabilities
Beam size 16 m, for = 0.5 m ( is a function of the lattice)
f = 11246 Hz
with 2808 bunches (every 25 ns one bunch) L = 1034 [cm-2s-1]
L = for one bunch
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…smallest beam size at experiments
QuadrupoleQuadrupole Collision point in experiment
Large beam size in adjacent quadrupole magnets Separation between beams needed, about 10 Limitation with aperture in quadrupoles Limitation of β function at IP to 1 m (2011) and 0.6 m (2012)
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The 2 LHC beams are brought together to collide in a ‘common’ region Over ~260 m the beams circulate in one vacuum chamber with ‘parasitic’
encounters (when the spacing between bunches is small enough) Total crossing angle of about 300 mrad
Experimental long straight sections
200 m
inner quadrupoletriplet
separationdipole (warm)
recombinationdipole
quadrupoleQ4
quadrupoleQ5
ATLAS or CMS
inner quadrupoletriplet
separationdipole
recombinationdipole
quadrupoleQ4
quadrupoleQ5
collision point
beam I
Example for an LHC insertion with ATLAS or CMS
24 m
beamdistance194 mm
beam II
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194 mm ATLAS IP
~ 260 m
Common vacuum chamber
Horizontal plane: the beams are combined and then separated
Vertical plane: the beams are deflected to produce a crossing angle at the IP to avoid undesired encounters in the region of the common vacuum chamber
a (mrad)
ATLAS -145 / ver.
ALICE 90 / ver.
CMS 120 / hor
LHCb -220 /hor
~ 7 mm
Not to scale !
a
Separation and crossing: example of ATLAS
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LHC Main Parameters
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LHC Parameter
Nominal 2011 2012
Proton energy [TeV] 7.0 3.5 4.0
Current in main dipoles [kA] 11.85 6.0 6.8
Stored energy, dipole circuit (154 dipoles)
[GJ] 1.07 ~0.28 ~0.35
Protons per bunch - 1.15 x 1011 ~1.5 x 1011 ~1.5 x 1011
Number of bunches - 2808 1380 1380
Bunch spacing [ns] 25 50 50
Normalized emittance [mm] 3.75 2.0 - 3.0 2.0 - 3.0
β* in IP1 and IP5 [m] 0.55 1.5 / 1.0 0.6
Stored energy / beam [MJ] 362 ~116 ~130
Peak luminosity for ATLAS and CMS
[cm-2s-1] 1.0 x 1034 0.36 x 1034 ~0.6 x 1034
Integrated luminosity for ATLAS and CMS
[fb-1] - 5.6 15
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LHC Parameter (energy)
Nominal 2011 2012 (intended)
Proton energy [TeV] 7.0 3.5 4.0
Current in main dipoles [kA] 11.85 6.0 6.8
Stored energy, dipole circuit (154 dipoles)
[GJ] 1.07 ~0.28 ~0.35
Protons per bunch - 1.15 x 1011 ~1.5 x 1011 ~1.5 x 1011
Number of bunches - 2808 1380 1380
Bunch spacing [ns] 25 50 50
Normalized emittance [mm] 3.75 2.0 - 3.0 2.0 - 3.0
β* in IP1 and IP5 [m] 0.55 1.5 / 1.0 0.6
Stored energy / beam [MJ] 362 ~116 ~130
Peak luminosity for ATLAS and CMS
[cm-2s-1] 1.0 x 1034 0.36 x 1034 ~0.6 x 1034
Integrated luminosity for ATLAS and CMS
[fb-1] - 5.6 15
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LHC Parameter (luminosity)
Nominal 2011 2012
Proton energy [TeV] 7.0 3.5 4.0
Current in main dipoles [kA] 11.85 6.0 6.8
Stored energy, dipole circuit (154 dipoles)
[GJ] 1.07 ~0.28 ~0.35
Protons per bunch - 1.15 x 1011 ~1.5 x 1011 ~1.5 x 1011
Number of bunches - 2808 1380 1380
Bunch spacing [ns] 25 50 50
Normalized emittance [mm] 3.75 2.0 - 3.0 2.0 - 3.0
β* in IP1 and IP5 [m] 0.55 1.5 / 1.0 0.6
Stored energy / beam [MJ] 362 ~116 ~130
Peak luminosity for ATLAS and CMS
[cm-2s-1] 1.0 x 1034 0.36 x 1034 ~0.6 x 1034
Integrated luminosity for ATLAS and CMS
[fb-1] - 5.6 15
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Very high beam luminosity: consequences
High energy stored in the beams Dumping the beam in a safe way Avoiding beam losses, in particular in the superconducting
magnets• Beam induced magnet quenching (when 10-8-10-7 of beam hits magnet at 7
TeV)• Beam cleaning (Betatron and momentum cleaning)
Radiation, in particular in experimental areas from beam collisions (beam lifetime is dominated by this effect)• Single event upset in the tunnel electronics
Beam instabilities due to impedance and beam–beam effects Photo electrons, generated by beam losses - accelerated by the
following bunches – lead to instabilities
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LHC Layout
eight arcs (sectors)
eight long straight section (about 700 m long) IR4: RF + Beam
instrumentation
IR5:CMS
IR1: ATLAS
IR8: LHC-BIR2: ALICE
InjectionInjection
IR6: Beam dumping system
IR3: Moment Beam Cleaning (warm)
IR7: Betatron Beam Cleaning (warm)
Beam dump blocks
Detection of beam losses with >3600
monitors around LHC
Signal to kicker magnet
Beams from SPS
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Machine Protection and
Collimation
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HASCO 2012 Rüdiger Schmidt
Energy stored magnets and beam
0.01
0.10
1.00
10.00
100.00
1000.00
10000.00
1 10 100 1000 10000Momentum [GeV/c]
En
erg
y s
tore
d in
th
e b
eam
[M
J]
LHC 7 TeV
LHC at injection
ISR
SNSLEP2
HERA
TEVATRON
SPSppbar
SPS transfer to LHC
Factor~200
RHIC proton
LHC energy in magnets
LHC 3.5 TeV
SPS material test
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What does this mean?
360 MJoule: the energy stored in one LHC beam corresponds
approximately to…
• 90 kg of TNT
• 8 litres of gasoline
• 15 kg of chocolate
It’s how ease the energy is released that matters most !!
The energy of an 200 m long fast train at 155 km/hour corresponds to the energy of 360 MJoule stored in one LHC beam
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55
Controlled SPS experiment 81012 protons clear damage beam size σx/y = 1.1mm/0.6mm
above damage limit for copper
stainless steel no damage 21012 protons
below damage limit for copper
6 cm
25 cm
• Damage limit ~200 kJoule
• 0.1 % of the full LHC 7 TeV beams
• factor of ~10 below the energy in a bunch train injected into LHC
V.Kain et al
A B D C
SPS experiment: Beam damage with 450 GeV proton beam
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56
Beam losses
In accelerators, particles are lost due to a variety of reasons • End of a physics fill• Beam-gas interaction • Losses from collisions • Losses due to the beam halo touching the aperture• Losses due to instabilities
Continuous beam losses are inherent to the operation of accelerators• Taken into account during the design of the accelerator
Accidental beam losses are due to a multitude of failures mechanisms
The number of possible failures leading to accidental beam loss is (nearly) infinite
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Layout of beam dump system in IR6
Beam 2
Beam dump block
Kicker magnets to paint (dilute)
the beam
about 700 m
about 500 m
15 fast ‘kicker’ magnets deflect the beam to the
outside
When it is time to get rid of the beams (also in case of emergency!), the beams are ‘kicked’ out of the ring by a system of kicker magnetsd send into a dump block !
Septum magnets deflect the
extracted beam vertically
quadrupoles
The 3 ms gap in the beam gives the kicker time to
reach full field.
Ultra-high reliability system !!
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Dump line in IR6
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Dump line
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Dump installation
CERN visit McEwen 60
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Beam dump with 1380 bunches
Beam spot at the end of the beam dumping line, just in front of the beam dump block
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62
Beam losses, machine protection and collimation
Continuous beam losses
Collimation prevents too high beam losses around the accelerator (beam cleaning)
A collimation system is a (very complex) system installed in the LHC to
capture mostly halo particles Such system is also called (beam) Cleaning System
Accidental beam losses
“Machine Protection” protects equipment from damage, activation and downtime
Machine protection includes a large variety of systems
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RF contacts for guiding image
currents
Beam spot
2 mm
View of a two sided
collimator
about 100 collimators are
installed in LHC
Ralph Assmann, CERN
length about 120 cm
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Betatron beam cleaning
Cold aperture
Cleaning insertion Arc(s) IP
Circulating beam
Illustration drawing
Arc(s)
Primarycollimator
Secondarycollimators
Tertiary beam halo + hadronic showers
Shower absorbers
Tertiarycollimators
SCTriplet
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• Ionization chambers to detect beam losses:• Reaction time ~ ½ turn (40 s)• Very large dynamic range (> 106)
• There are ~3600 chambers distributed over the ring to detect abnormal beam losses and if necessary trigger a beam abort !
Beam Loss Monitors
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Rüdiger Schmidt
Continuous beam losses during collisions
66
CMS Experiment
ATLAS Experiment
LHC Experiment
ALICE Experiment
MomentumCleaning
RF and BI
Beamdump
Betatron Cleaning
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Measurement: 500kJ losses at primary collimators (loss rate: 9.1e11 p/s) – IR7
Daniel Wollmann
TCP: ~505 kJ
Q8L7: ~335 J
Q11L7: ~35 J
Q19L7: ~4.7 J
Q8L7:h ~ 6.7e-4
Lower limit:RqLdil ~ 1.22e9 p/s (with
cresp= 2 )
Lost energy over 1 s
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Strategy for protection and related systems
Avoid that a specific failure can happen
Detect failure at hardware level and stop beam operation Detect initial consequences of failure with beam
instrumentation ….before it is too late…
Stop beam operation• stop injection• extract beam into beam dump block• stop beam by beam absorber / collimator
Elements in the protection systems• hardware monitoring and beam monitoring• beam dump (fast kicker magnet and absorber block)• collimators and beam absorbers• beam interlock systems linking different systems
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Machine Protection at
Injection
…throwing 3 MJ at LHC
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HASCO 2012 Rüdiger Schmidt
SPS, transfer line and LHC
1 km
Beam is accelerated in SPS to 450 GeV (stored energy of 3 MJ)
Beam is transferred from SPS to LHC
Beam is accelerated in LHC to 3.5 TeV (stored energy of 100 MJ)
Scraping of beam in SPS before transfer to LHC
Transfer line 3km
LHC
SPS6911 m
450 GeV / 400 GeV3 MJ
Acceleration cycle of ~10 s
CNGS Target
IR8
Switching magnetFast extraction
kicker
Injection kicker
Transfer line
Injection kicker
IR2 Fast extraction kicker
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HASCO 2012 Rüdiger Schmidt
Protection at injection
LHC circulating beam
Circulating beam in LHC
LHC vacuum chamber
Transfer line vacuum chamber
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HASCO 2012 Rüdiger Schmidt
LHC circulating beam
Beam injected from SPS and transfer line
Protection at injection
Beam from SPS
Injection Kicker
LHC injected beam
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HASCO 2012 Rüdiger Schmidt
LHC circulating beam
Kicker failure (no kick)
Protection at injection
Beam from SPS
Injection Kicker
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HASCO 2012 Rüdiger Schmidt
LHC circulating beam
Beam absorbers take beam in case of kicker misfiringTransfer line collimators ensure that incoming beam trajectory is ok
Protection at injection
Beam from SPS
Injection Kicker Set of transfer line
collimators (TCDI) ~5σ
Injection absorber(TDI) ~7σ
phase advance 900
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HASCO 2012 Rüdiger Schmidt
LHC circulating beam
Beam absorbers take beam in case of kicker misfiring on circulating beam
Protection at injection
Injection Kicker
Injection absorber(TDI) ~7σ
Circulating beam – kicked out
phase advance 900
LHC circulating beam
Set of transfer line collimators (TCDI)
~5σ
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Understanding LHC operation• Filling• Ramp• Squeeze• Adjust• Stable beams• Pilot beam• Batches• Closed orbit • Beta function• Betatron tunes• Emittance• Impedance
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From first year to first fb-1
2008First beam in
LHC
2010First fb-1
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From 2010….
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…..to 2012
1 fb-1 6 fb-1
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Excellent fill 2195 in 2011
A nice long fill of about 18 hours……
Injection and
ramp
Stable beams
Beam dump
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Beam Intensities and Luminosity, 11-18/6/2012
Stable performance
Mix
ed b
ag
Stable performance
2×1014
6×1033
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LHC 8:30 meeting
Overview of fillsFill Duration Ibeam Lpeak
[e30 cm-2s-1]Lint [pb-1]
Dump
2723 2:26 2.03E+14 6406 46.06 Trip of ROD.A81B1, SEU?
2724 1:13 2.03E+14 6329 25.905 Electrical perturbation
2725 7:04 2.05E+14 6520 115.5 Trip of S81
2726 8:58 2.05E+14 6499 142.5Elecitrical perturbation, FMCM
2728 11:41 2.06E+14 6525 171.5 Operator dump
2729 3:28 2.06E+14 6502 67.7 BLM self trigger
2732 1:52 2.06E+14 6592.5 40 QPS trigger RQX.R1, SEU?
2733 12:34 2.06E+14 6674 183 Triplet RQX.L2 tripped.
2734 15:33 2.01E+14 6257.5 203.5 Operator dump
2736 17:29 2.02E+14 6465.5 233 Operator dump
2737 3:36 1.99E+14 6021 66.1 RF Trip 2B2
Total 51.1% 1301
51 % of time in stable beams; total of 1.3 fb-1 in one week !
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Good fill 2195 in 2011 – start of the fill
Start injection
End injection
Start energy ramp
End energy ramp
3.5 TeV
~1 hour
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Reference fill 2195 in 2011 – at 3.5 TeV
Start ramp to collisiong
Squeezing
Energy ramp to 3.5 TeV
Bringing beams into collision
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Luminosity increase
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Luminosity increase
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Luminosity increase
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Luminosity increase
To increase the luminosity, the beta function was reduced between 2011 and 2012 from 1.0 m to 0.6 m
This reduces the beam size in the experiments, and increases the beam size in the adjacent quadrupole magnets (inner triplets)
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…beam size at experiments in 2011
Collision point in experiment
Crossing angle to avoid parasitic beam-beam interaction Minimum separation in the order of 10 ( rms beam size)
Quadrupole Quadrupole
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…becoming smaller during more squeezing
Collision point in experiment
β function at IP down to 0.6 m in 2012 Larger beam size in quadrupole magnets Higher energy: emittance decreases for protons Separation needs to increase to keep 10 Problems with aperture in quadrupoles Collimators need to be set tighter
Quadrupole Quadrupole
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Record fill 2692 in 2012, max. integrated luminosity
Start energy ramp
End energy ramp4 TeV
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Fill 2701, typical fill in 2012
R.Schmidt 92
end squeeze and start
adjust end adjust
start squeeze
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Fill 2602, also a typical fill in 2012…….
R.Schmidt 93
21:41:24 start
squeeze
21:57:33 start
adjust 22:07:15end adjust
21:37:59 end ramp
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Rüdiger Schmidt
BLM system: beam losses before collisions
CMS Experiment
ATLAS Experiment
LHC Experiment
ALICE Experiment
MomentumCleaning
RF and BI
Beamdump
Betatron Cleaning
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Rüdiger Schmidt
Continuous beam losses during collisions
95
CMS Experiment
ATLAS Experiment
LHC Experiment
ALICE Experiment
MomentumCleaning
RF and BI
Beamdump
Betatron Cleaning
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Rüdiger Schmidt
2. An object falls into the beam
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Rüdiger Schmidt
Continuous beam losses during collisions
97
CMS Experiment
ATLAS Experiment
LHC Experiment
ALICE Experiment
MomentumCleaning
RF and BI
Beamdump
Betatron Cleaning
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Rüdiger Schmidt
Accidental beam losses during collisions
98
CMS Experiment
ATLAS Experiment
LHC Experiment
ALICE Experiment
MomentumCleaning
RF and BI
Beamdump
Betatron Cleaning
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Rüdiger Schmidt
Zoom one monitor: beam loss as a function of time
1 ms
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Rüdiger Schmidt
UFOs at LHC
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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Rüdiger Schmidt
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2012 Achieved vs. Target LuminosityEstimates from Moriand (Mike Lamont & Steve Myers)
Assumptions– 4 TeV, 50 ns, 1380 bunches, 1.6e11, 2.5 um, pile-up ~ 35
– 150 days of proton physics (assuming similar efficiencies to 2011)
Initial slow recovery a technical stop, but eventually caught up
Presently operating with ~1 fb-1/week
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What we learned…..
Head-on beam-beam effect is not a limitation Long range beam-beam effect has to be taken seriously
• Need separation of 10 -12 σ (otherwise bad lifetime and beam loss) Small as possible emittances are good Established β* reach (aperture, collimation, optics) Luminosity levelling via offset tested – works fine in LHCb! High-intensity operation close to beam instability limits Instabilities were observed and are not fully understood
• for small IP beam offsets while going into collisions, ….• impedances (kicker, collimator heating), collective effects, ...
Availability• Single Event Upsets, vacuum pressure increase, UFOs,
cryogenics, magnet protection system, ..…) – • vigorous follow-up and consolidation
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LHC Operation after the shutdown 2013/14
Energy 6.5 TeV during 2015 Bunch spacing 25 ns (in case of problem fall back to 50 ns) Beta-function at experiments ~0.5 m Pile-up of events in the experiments– assume acceptable
• Depends on bunch spacing and squeeze beyond 0.5 m• Beta* luminosity-levelling to mitigate the initial large pile-up
Performance could be impacted by• UFOs at higher energy and with 25 ns buch spacing• Radiation to electronics – SEU’s• Electron cloud & high energy & at 25 ns• Long-range beam-beam & smaller crossing angle & at 25 ns• Single- and bunch-by-bunch beam instabilities (impedances...)
It should be possible to achieve nominal luminosity of 1034 [cm-2s-1] or more
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Summary
• In 2012 the peak luminosity exceeded 6x1033 cm-2s-1 in ATLAS and CMS with beams of 50 ns spacing• The stored energy of the beams exceeded by a factor ~50 that of
existing or previous machines
• No beam induced magnet quench was observed with stored beams
• Operation in 2012 is at 4.0 TeV
• Integrated luminosity for 2012 is in excess of 7 fm-1, hope to reach 15-20 fm-1 until the end of the run in February 2013
• The consolidation of the splices between magnet will be done in 2013/14 to restart in 2015 at about 6.5 TeV
• UFOs could become a limitation for the availability of LHC at 6.5 TeV
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Thanks for your attention
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Reserve slides
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LHC nominal energy is 7 TeV
Why 3.5 TeV in 2011 and 4 TeV in 2012 ?
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Accident in 2008
Commissioning of main dipole circuit in last LHC sector: ramp to 9.3 kA (5.5 TeV)
At 8.7 kA an electrical fault developed in a dipole bus bar interconnection between a quadrupole and dipole
Later correlated to a local resistance of ~220 nOhm – nominal value 0.35 nOhm
An electrical arc developed which punctured the helium enclosure and the beam vacuum tube
Secondary arcs developed along the sector Around 400 MJ from a total of 600 MJ were dissipated in
the cold-mass and in electrical arcs Large amounts of helium were released into the insulating
vacuum, in total 6 tons were released
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Rupture of high current cable between two magnets
12 kA cable
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Pressure inside the cryostats
PTQVQV QV QVQV SVSV
Cold-massVacuum vesselLine ECold support postWarm JackCompensator/BellowsVacuum barrier
Q D D QD D D QD D D QD D D QD
• Self actuating relief valves could not handle the pressure
• designed for 2 kg He/s, incident ~ 20 kg/s• Large forces exerted on the vacuum barriers (every 2
cells, 230 m)• designed for a pressure of 1.5 bar, incident ~ 10 bar• Several quadrupoles displaced by up to ~50 cm• Connections to the cryogenic line damaged in some
places
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Incident location
Dipole bus bar
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Quadrupole-dipole interconnection (27R3)
Quadrupole support
• 39 dipoles out of 154• 14 quadrupole short straight
sections (SSS) out of 52
…had to be moved to the surface for control, repair or replacement
Collateral damage : displacements
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Incident in 2008, caused by a bad splice
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4 TeV - limitation of energy
• To reach nominal energy of 7 TeV requires a consolidation campaign of the connections (will take more than one year, requires full warm up of LHC)
• In order to avoid any risk, it was decided to limit the current in the main magnets and therefore the energy to 3.5 TeV for 2010 and 2011, and to 4.0 TeV for 2011
• It turned out that there is still excellent physics at this energy, and it is planned to increase the energy to 6.5 TeV after the consolidation
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Risk during a quench of a main dipole
1 qu
ench
/mon
th
If during 2012 the number of high current quenches stays below 5-6 then we have the same probability of burn-out as during 3.5 TeV run in 2011 with 40 quenches
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Schematic of the main dipole circuit
Global protection of the busbar and joints between magnetsprotection threshold 1 V (160 V inductive voltage during ramp)
Local (quench) protection of each
magnet
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Long Shutdown LS1
2013 – 2014: LS1 consolidate LHC for 6.5 / 7TeV: Measure all splices and repair the defective Consolidate interconnects with new design (clamp, shunt) Finish installation of pressure release valves (DN200) Magnet consolidation Electronics relocation, redesign, etc. to further reduce
SINGLE EVENT EFFECTS on electronics Install collimators with integrated button BPMs (tertiary
collimators and a few secondary collimators)
Extensive parallel consolidation and upgrades of experiments
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DN200 – He blow-hole
LHC MB Circuit Splice Consolidation PlansClamping and Shielding