basic concepts of charged particle detection: part 2
DESCRIPTION
Basic Concepts of Charged Particle Detection: Part 2. Overview. Lecture 1: Concepts of particle detection: what can we detect? Basic design of particle detectors Energy loss of charged particles in matter: Bethe Bloch formula Lecture 2: - PowerPoint PPT PresentationTRANSCRIPT
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Charged Particle Detection 2David Futyan 1
Basic Concepts of ChargedParticle Detection:
Part 2
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Charged Particle Detection 2David Futyan 2
Overview
Lecture 1:Concepts of particle detection: what can we detect?Basic design of particle detectorsEnergy loss of charged particles in matter: Bethe Bloch formula
Lecture 2: Energy loss through Bremsstrahlung radiation (electrons)Momentum measurement in a magnetic fieldMultiple Coulomb scattering - effect on momentum resolutionInteraction of photons
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Charged Particle Detection 2David Futyan 3
Energy Loss of Electrons and Positrons
Electrons lose energy through ionization as for heavy charged particles, but due to small mass additional significant loss through bremsstrahlung radiation.Total energy loss:
€
dEdX tot
= dEdX rad
+ dEdX ion
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Charged Particle Detection 2David Futyan 4
Energy Loss Through Ionization for Electrons
Ionization loss for high energy electrons (»1MeV) can be approximated by Bethe Bloch formula with =1, z=1:
Approximate and only valid for high energy. Full treatment requires modification of the Bethe Bloch formula due to:
Small electron mass: assumption that incident particle is undeflected during collision process is not validCollisions are between identical particles - Q.M. effects due to indistinguishability must be taken into account.e.g. see Leo p.37NB. Tmax=Te/2, where Te = KE of incident electron
€
−dEdX ion
= 4πNAre2mec
2 ZA
12
ln 2mec2γ 2Tmax
I2 −1 ⎡ ⎣ ⎢
⎤ ⎦ ⎥
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Charged Particle Detection 2David Futyan 5
Bremsstrahlung Radiation
Emission of e.m. radiation arising from scattering in the E field of a nucleus in the absorber medium.Classically, can be seen as radiation due to acceleration of e+ or e- due to electrical attraction to a nucleus.
Radiative energy loss dominates for electrons for E > few 10s of MeV.
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Charged Particle Detection 2David Futyan 6
Energy Loss Through Bremsstrahlung
= Fine structure constant:
Note that (recall )
Bremsstrahlung only significant for electrons/positrons
For E < ~1TeV, electrons/positrons are the only particles in which radiation contributes significantly to energy loss.
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−dEdX rad
= 4αNA re2 Z 2
AE ln 183
Z1/ 3
€
−dEdX rad
∝ 1m2
€
re = 14πε0
e2
mec2
€
me
mμ
⎛
⎝ ⎜ ⎜
⎞
⎠ ⎟ ⎟
2
≈ 40000€
=e2
hc4πε0
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Charged Particle Detection 2David Futyan 7
Radiation Length
Define Radiation Length, X0:
Radiation length is the the mean distance over which a high-energy electron loses all but 1/e of its energy by bremsstrahlung.
e.g. Pb: Z=82, A=207, =11.4 g/cm3:X0 ≈ 5.9 g/cm2
Mean penetration distance: x = X0/ = 5.9/11.4 = 5.2mm
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−dEdX rad
= EX0
€
1X0
= 4αNA re2 Z 2
Aln 183
Z1/ 3
€
E = E0e−x / X 0
where
Units of X0: g cm-2
Divide by density to get X0 in cm
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Charged Particle Detection 2David Futyan 8
Comparison with Energy Loss Through Ionization
Compare:
Rapid rise of radiation loss with electron energy
Almost all energy of electron can be radiated in one or two photons! In contrast ionization loss quasi-continuous along path of particle.
€
dEdX rad
∝ Z 2E
€
dEdX ion
∝ Z ln E
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Charged Particle Detection 2David Futyan 9
Critical EnergyCritical energy is energy for which:
E.g. EC for electrons in Cu(Z=29): ~20 MeV
Energy loss through bremsstrahlung dominates for E > few 10s of MeV.e.g. electrons in LHC events: tens of GeV bremsstrahlung completely dominates.
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dEdX rad
= dEdX ion
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ECsolid +liq ≈ 610MeV
Z +1.24
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ECgas ≈ 710MeV
Z +1.24
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Charged Particle Detection 2David Futyan 10
Example: Bremsstrahlung in CMSElectron must traverse ~1X0 of material in the inner tracker (13 layers of Si strip detectors) before it reaches the electromagnetic calorimeter.On average, about 40% of electron energy is radiated in the tracker
Spray of deposits in the ECAL - must be combined to give calorimeter energy measurement.
Momentum at vertex should be determined from track curvature before 1st bremsstrahlung emission.
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Charged Particle Detection 2David Futyan 11
Full Energy Loss Spectrum for Muons-dE/dX for positive muons over 9 orders of magnitude in momentum:
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Charged Particle Detection 2David Futyan 12
Momentum Measurement in a Magnetic Field
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pT = qBr
€
mv 2
r= Bqv
€
pT (GeV /c) = 0.3Br
€
L2r
= sin θ2
≈ θ2
€
θ ≈0.3BL
pT
€
s = r − rcos θ2 ⎛ ⎝ ⎜
⎞ ⎠ ⎟≈ r 1− 1− 1
2θ 2
4
⎛ ⎝ ⎜
⎞ ⎠ ⎟
⎛
⎝ ⎜
⎞
⎠ ⎟= rθ 2
8
€
s ≈ 0.3BL2
8pT
e.g. s = 3.75 cmfor pT=1 GeV/c,L=1m and B=1T
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Charged Particle Detection 2David Futyan 13
Momentum Measurement ErrorDetermination of sagitta from 3 measurements:
Momentum resolution:
Momentum resolution degrades linearly with increasing momentum, and improves quadratically with the radial size of tracking cavity.For N equidistant measurements, one obtains (R.L. Gluckstern, NIM 24 (1963) 381):
e.g. (pT)/pT = 0.5% for pT=1 GeV/c, L=1m, B=1T, x = 200 m and N=10
x
1
2
3
€
s = x2 − x1 + x3
2s
€
s = 32
σ x
€
pT
pT
= σ s
s= 3/2σ x
s
€
pT
pT meas
= 32
σ x8 pT
0.3BL2
€
pT
pT meas
= σ x pT
0.3BL2
720N + 4
€
pT
pT meas
∝ σ x pT
BL2
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Charged Particle Detection 2David Futyan 14
Multiple Coulomb Scattering
In addition to inelastic collisions with atomic electrons (i.e. ionization - Bethe Bloch), charged particles passing through matter also suffer repeated elastic Coulomb scattering from nuclei.Elastic Coulomb scattering produces a change in the particle direction without any significant energy loss.Change in direction caused by multiple Coulomb scattering degrades the momentum measurement.
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Charged Particle Detection 2David Futyan 15
Single Scattering
Individual collisions governed by Rutherford scattering formula:
Does not take into account spin effects or screeningAlthough single large angle scattering can occur for very small impact parameter, probability that a single interaction will scatter through a significant angle is very small due to 1/sin4(θ/2) dependence.For large impact parameter (much more probable), scattering angle is further reduced w.r.t. Rutherford formula due to partial screening of nuclear charge by atomic electrons.
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dσdΩ
= z2Z 2re2 mec
βp ⎛ ⎝ ⎜
⎞ ⎠ ⎟2
14sin4 (θ /2)
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Charged Particle Detection 2David Futyan 16
Multiple Coulomb ScatteringAs a particle passes through a thickness of material, combination of a very large number of small deflections results in a significant net deviation - multiple coulomb scatteringSmall contributions combine randomly to give a Gaussian probability distribution:
Plane of incidentparticle
( to B field)
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P(α )dα = 1π
e−α 2
dα
€
=θplane
θ planeRMSwhere
(Gaussian)
plane
€
=θplaneRMS
€
θ
€
θplaneRMS = 1
2θ space
RMS
θplane is projection of true space scattering angle onto plane of incident particle.
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Effect of Multiple Scattering on Resolution
Approximate relation (PDG):
Apparent sagitta due to multiple scattering (from PDG):
Contribution to momentum resolution from multiple scattering:
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θ0 = θ planeRMS ≈ 13.6MeV
pβcz L
X0
€
θ0 ∝1p
LX0
i.e.
Charge of incident particle Radiation length of absorbing material
€
splane = Lθ0
4 3
€
p
p MS
=splane
s≈ 0.05
B LX0
Independent of p!
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s ≈ 0.3BL2
8pTusing i.e.
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p
p MS
∝ 1B LX0
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Effect of Multiple Scattering on Resolution
(p)/p
σ(p)/p
σ(p)/p
p
MS
meas.total error
Estimated Momentum Resolutionvs pT in CMS
Example:pT = 1 GeV/c, L = 1m, B = 1 T, N = 10, x = 200m:
For detector filled with Ar, X0 = 110m:
€
p
p meas
≈ 0.5%
€
p
p MS
≈ 0.5%
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Charged Particle Detection 2David Futyan 19
Momentum Measurement Summary
Tracking detector design:High B field. e.g. CMS: 4 TeslaLarge size e.g. CMS tracker radius = 1.2mLow Z, low mass material. Gaseous detectors frequently chosen e.g. ATLAS Ar (91% of gas mixture) X0=110m
€
p
p MS
∝ 1B LX0
€
pT
pT meas
∝ σ x pT
BL2
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Interaction of PhotonsNo E field => inelastic collisions with atomic electrons and bremsstrahlung which dominate for charged particles do not occur for photons3 main interations:
1) Photoelectric effect (dominant for E<100keV): Photon is absorbed by an atomic electron with the subsequent
ejection of the electron from the atom.2) Compton scattering (important for E~1MeV): Scattering of photons on free electrons
(atomic electrons effectively free forE >> atomic binding energy)
3) Pair production (dominant for E>5MeV) Photon is converted into an electron-positron pair
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Charged Particle Detection 2David Futyan 21
Interaction of Photons
Result of these 3 interactions:1) Photons (x-rays, -rays) much more penetrating in matter than charged particles Cross-section for the 3 interactions much less than inelastic
collision cross-section for charged particles2) A beam of photons is not degraded in energy as it passes through a thickness of matter, only in intensity The 3 processes remove the photon from the beam entirely
(absorbed or scattered out). Photons which pass straight through have suffered no interaction
so retain their original energy, but no. of photons is reduced.Attenuation is exponential w.r.t. material thickness:
€
I(x) = I0 exp(−μx)
Absorption coefficient
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Charged Particle Detection 2David Futyan 22
e+e- Pair Procution
For energies > a few MeV, pair production is the dominant mechanism:
In order to conserve energy and momentum, pair production can only occur in the presence of a 3rd body, e.g. an atomic nucleus.
e.g. CMS ECAL: PbW04 crystals - dense material with heavy nuclei
In order to create the pair, photon must have energy E>2mec2 i.e. E>1.022MeV.
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Charged Particle Detection 2David Futyan 23
Electron-Photon Showers
Combined effect of pair production for photons and bremsstrahlung for electrons is the formation of electron-photon showers.
Shower continues until energy of e+e- pairs drops below critical energySee lectures on Calorimetry (Chris Seez)