Hoja de repaso: Fundamentals of Particle Interactions

📋 Course Outline

1. Flavour symmetry revisited
2. Quantum Chromodynamics local gauge principle
3. Colour confinement and asymptotic freedom
4. QCD in electron positron annihilation
5. Hadron hadron collisions and colour factors
6. Weak interaction charged current and V minus A
7. Chiral structure and W boson propagator
8. Lepton universality and neutrino scattering
9. Neutrino oscillations and mass eigenstates
10. Ionisation energy loss and minimum ionising particles
11. Electromagnetic showers and critical energy
12. Electromagnetic calorimeters and shower containment

📖 1. Flavour symmetry revisited

🔑 Key Concepts & Definitions

• Flavour symmetry : Flavour symmetry is an approximate invariance that treats different quark flavours as interchangeable in the strong-interaction description.
• Isospin SU(2) : Isospin SU(2) is the flavour symmetry subgroup that groups up and down quarks into a doublet with nearly equal strong interactions.
• SU(3) flavour symmetry : SU(3) flavour symmetry is the larger flavour symmetry that organizes the light quarks into multiplets and relates their strong-interaction properties.
• Flavour multiplets : Flavour multiplets are sets of hadron states grouped together because flavour symmetry predicts relations among their quantum numbers and wavefunctions.

📝 Essential Points

• Flavour symmetry is revisited by refining how quark-flavour states are combined into hadron wavefunctions using symmetry constraints.
• Isospin treats up and down quarks as a two-component system, leading to structured relations among hadrons built from these flavours.
• SU(3) flavour symmetry extends the idea to include the strange quark, producing a classification of light-flavour hadrons into multiplets.
• The symmetry is approximate because quark masses and other effects break the ideal interchangeability of flavours.
• The revisited treatment emphasizes how symmetry representations guide the construction of baryon states from quark content and flavour quantum numbers.

💡 Memory Hook

Isospin = up/down only (SU(2)); SU(3) = add strange (bigger flavour multiplets).

📖 2. Quantum Chromodynamics local gauge principle

🔑 Key Concepts & Definitions

• Quantum Chromodynamics : Quantum Chromodynamics is the quantum field theory describing the strong interaction via colored quarks and gluons.
• Local gauge invariance : Local gauge invariance is the requirement that the physics is unchanged under position-dependent gauge transformations.
• Color SU(3) gauge symmetry : Color SU(3) gauge symmetry is the non-Abelian symmetry group governing how quarks transform under the strong interaction.
• Gluon gauge boson : A gluon is the gauge boson associated with the SU(3) color symmetry and mediates the strong force.
• Non-Abelian gauge theory : A non-Abelian gauge theory is a gauge theory whose symmetry group has non-commuting generators, leading to self-interacting gauge fields.

📝 Essential Points

• QCD is built to be invariant under local SU(3) color transformations, which fixes the form of the strong-interaction couplings.
• Quarks carry color charge, and gluons couple to color currents rather than to electric charge.
• Because SU(3) is non-Abelian, the gluon field includes self-interaction terms, unlike Abelian theories such as QED.
• Local gauge invariance determines the structure of the QCD covariant derivative used in the quark kinetic term.
• The gauge principle implies that introducing gauge fields is necessary to maintain invariance under local color rotations.
• Gauge invariance constrains the allowed interaction vertices, producing quark–gluon and gluon–gluon interactions consistent with SU(3) symmetry.

💡 Memory Hook

Local symmetry → gauge fields: SU(3) color rotations force gluons, and non-commuting generators make gluons self-interact.

📖 3. Colour confinement and asymptotic freedom

🔑 Key Concepts & Definitions

• Colour confinement : Colour confinement is the QCD property that coloured quarks and gluons cannot appear as isolated free particles.
• Asymptotic freedom : Asymptotic freedom is the QCD behaviour where the strong interaction becomes weaker at very short distances or high energies.
• Quantum Chromodynamics : Quantum Chromodynamics is the fundamental theory describing strong interactions between quarks and gluons.
• Strong interaction running coupling : The strong interaction running coupling is the effective strength of QCD that changes with the energy scale of the process.
• Energy-scale dependence : Energy-scale dependence is the idea that the effective description of particle interactions depends on the energy regime being probed.

📝 Essential Points

• Colour confinement explains why observable hadrons are colour-neutral bound states rather than free coloured quarks or gluons.
• Asymptotic freedom explains why QCD interactions are effectively weaker at high energies, enabling perturbative calculations in that regime.
• The effective strength of the strong force varies with the energy scale, so the same QCD theory yields different effective behaviours at different energies.
• At low energies, confinement dominates and quarks are effectively locked into bound states, while at high energies asymptotic freedom dominates.
• QCD is the strong-interaction theory underlying both confinement at long distances and asymptotic freedom at short distances.
• The energy-scale viewpoint links atomic, nuclear, and collider regimes by showing that different effective physics applies at different energies.

💡 Memory Hook

Confinement = “can’t escape” at low energy; asymptotic freedom = “free to interact weakly” at high energy.

📖 4. QCD in electron positron annihilation

🔑 Key Concepts & Definitions

• Quantum Chromodynamics : Quantum Chromodynamics is the quantum field theory describing the strong interaction between quarks via colour charge.
• Colour charge : Colour charge is the QCD analogue of electric charge carried only by quarks, which is what makes them feel the strong force.
• Hadron confinement : Hadron confinement is the phenomenon that quarks are never observed as free particles but only inside bound states called hadrons.
• Electron positron annihilation : Electron positron annihilation is the process where an electron and a positron annihilate to produce other particles, including hadronic final states through QCD.

📝 Essential Points

• Only quarks carry colour charge, so only quarks experience the strong force in the Standard Model.
• Because of QCD dynamics, quarks appear experimentally only inside hadrons such as protons and neutrons.
• In electron–positron annihilation, hadronic final states arise when the produced quark–antiquark system hadronizes via QCD confinement.
• QCD is part of the Standard Model alongside QED and the weak force, but it specifically governs the strong interaction sector.
• Quarks differ from leptons because their strong-force interactions make their observable states bound, unlike electrons, muons, taus, and neutrinos.
• QCD is a quantum field theory, so the strong interaction is treated through field-mediated processes rather than action-at-a-distance potentials.

💡 Memory Hook

Colour charge → strong force → quarks confined into hadrons; in e+e−, hadrons signal QCD.

📖 5. Hadron hadron collisions and colour factors

🔑 Key Concepts & Definitions

• Hadron hadron collisions : Hadron hadron collisions are interactions between composite particles (hadrons) whose internal quarks and gluons participate in the hard scattering.
• Colour charge : Colour charge is the QCD property carried by quarks that determines how strongly they interact via gluon exchange.
• Gluon exchange : Gluon exchange is the QCD mechanism where the strong interaction between coloured partons is mediated by massless gluons.
• Colour factors : Colour factors are numerical weights from QCD’s colour algebra that multiply scattering amplitudes and determine relative strengths of processes.
• Parton model picture : The parton model picture treats a hadron as containing quarks and gluons that scatter as if they were quasi-free at high energies.

📝 Essential Points

• In QFT, forces are described by exchange of gauge bosons, so the strong interaction is mediated by gluons (spin-1, massless).
• Only quarks carry colour charge, so only quarks participate in the strong interaction while colourless particles do not couple to gluons.
• In hadron collisions, the observed event rate depends on which quarks and gluons inside the hadrons undergo the hard exchange.
• Colour factors arise because gluons couple to colour charge and the amplitude includes sums over colour states.
• The relative strength of the strong interaction is much larger than electromagnetism at a distance scale of about 1 fm, with indicative strength near 1 versus $10^{-3}$.
• Because exchanged gluons are not directly observed, only the combined effect of all allowed time-orderings contributes to the physical scattering amplitude.

💡 Memory Hook

QCD = “Quarks carry Colour”; gluons are the “Colour messengers,” and colour factors are the “algebra weights” multiplying the amplitude.

📖 6. Weak interaction charged current and V minus A

🔑 Key Concepts & Definitions

• Weak charged-current interaction : The weak charged-current interaction is the Standard Model force that couples quarks with a change of flavour via W-boson exchange.
• Flavour change : Flavour change is the transition where a particle’s quark or lepton type changes, which is enabled by the weak charged current.
• Coupling constant g : The coupling constant g sets the interaction strength at each gauge-boson–fermion vertex in quantum field theory amplitudes.
• Dimensionless coupling αW : The dimensionless weak coupling αW is a convenient form proportional to g2 that controls interaction probabilities at each vertex.

📝 Essential Points

• Charged-current weak coupling is strongest between up-type quarks (u,c,t) and down-type quarks (d,s,b) of the same generation.
• The weak charged-current interaction is especially important for decays because it introduces a change of flavour between initial and final fermions.
• Each interaction vertex contributes a factor g to the transition matrix element, so for two vertices M ∝ g2 and |M|2 scales with higher powers of g.
• Using a dimensionless coupling α ∝ g2 is convenient because the interaction probability includes one factor of α per vertex.
• At low energies the weak interaction is much weaker than QED because the W boson is very massive, even though αW is larger than QED’s α.

💡 Memory Hook

W boson is heavy → weak decays are suppressed at low energy; charged current enables flavour change.

📖 7. Chiral structure and W boson propagator

🔑 Key Concepts & Definitions

• Chiral structure : Chiral structure describes how weak interactions couple differently to left- and right-handed fermion components.
• Charged-current weak interaction : Charged-current weak interaction is the weak process mediated by a W boson that changes particle flavour at the interaction vertex.
• W boson propagator : The W boson propagator is the factor in amplitudes that describes how an exchanged W boson propagates between two weak vertices.
• Muon decay : Muon decay is a weak decay where a muon transforms into an electron, a muon neutrino, and an electron antineutrino.

📝 Essential Points

• The charged-current weak interaction produces a flavour change at the W-vertex, so weak decays can occur even when electromagnetic or strong decays are forbidden.
• The electron is stable because it is the lightest charged lepton, so there is no weak decay conserving energy and momentum.
• In muon decay, the diagram arrow in negative time corresponds to an antiparticle, specifically an electron antineutrino.
• Unstable particles typically travel a distance of order $\gamma v\tau$ before decaying, with $\gamma=1/\sqrt{1-v^2/c^2}$ accounting for time dilation.
• If a particle can decay via the strong interaction, that decay almost always dominates over electromagnetic or weak decay modes; electromagnetic dominates over weak when strong is absent.

💡 Memory Hook

W-mediated charged current: flavour changes at the vertex; muon decay shows antiparticle arrows for antineutrinos.

📖 8. Lepton universality and neutrino scattering

🔑 Key Concepts & Definitions

• Lepton universality : Lepton universality is the hypothesis that the weak interaction couples equally to different charged leptons, up to small mass effects.
• Neutrino scattering : Neutrino scattering is the interaction of neutrinos with matter in which the neutrino transfers energy and momentum to target particles.
• Minimum ionising particle : A minimum ionising particle is a charged particle whose ionisation energy loss $dE/dx$ is near the minimum of its characteristic curve.
• Bethe–Bloch equation : The Bethe–Bloch equation gives the mean ionisation energy loss $dE/dx$ of a charged particle moving through matter as a function of its speed and material properties.

📝 Essential Points

• Ionisation energy loss is largest at low velocity because the Bethe–Bloch form contains a $1/v^2$ dependence.
• For relativistic particles with $v\approx c$, $dE/dx$ depends only logarithmically on $(\beta\gamma)^2$ where $\beta=v/c$ and $\gamma=1/\sqrt{1-\beta^2}$.
• The effective ionisation potential $I_e$ is very approximately $I_e\sim 10Ze\,\text{eV}$ for a material with atomic number $Z$.
• For a fixed medium, the ionisation loss rate depends mainly on density $\rho$ rather than detailed composition, because atom number density scales like $n=\rho/(A\,\mu)$.
• Minimum ionising particles occur near the minimum of the $dE/dx$ curve at about $\beta\gamma\approx 3$ (as indicated in the figure discussion).
• For muons below about $100\,\text{GeV}$, ionisation is the dominant energy-loss mechanism, so they can traverse dense detectors leaving an ionisation trail.

💡 Memory Hook

$dE/dx$: low $v$ → big loss ($1/v^2$); high $v$ → slow rise (log in $(\beta\gamma)^2$).

📖 9. Neutrino oscillations and mass eigenstates

🔑 Key Concepts & Definitions

• Neutrino oscillations : Neutrino oscillations are the phenomenon where a neutrino changes flavour as it propagates due to mixing between mass and flavour states.
• Mass eigenstates : Mass eigenstates are the neutrino states with definite masses that propagate with different phases, enabling oscillations.
• Flavour eigenstates : Flavour eigenstates are the neutrino states produced and detected via weak interactions, which are superpositions of mass eigenstates.
• Mixing between states : Mixing between flavour and mass eigenstates means flavour states are linear combinations of mass eigenstates with specific amplitudes.

📝 Essential Points

• Oscillations arise because different mass eigenstates acquire different relative quantum phases during propagation.
• A neutrino produced in a flavour eigenstate is a superposition of mass eigenstates, so detection as another flavour has nonzero probability.
• The oscillation probability depends on the mass-squared differences between mass eigenstates and on the propagation distance and energy.
• If all relevant mass eigenstates had the same mass (no mass-squared difference), the relative phase would not change and oscillations would disappear.
• In the relativistic regime, the phase evolution can be expressed using $\Delta m^2$ rather than absolute masses, making $\Delta m^2$ the key parameter.

💡 Memory Hook

Oscillations = phase drift: different masses → different phases → flavour change.

📖 10. Ionisation energy loss and minimum ionising particles

🔑 Key Concepts & Definitions

• Ionisation energy loss : Ionisation energy loss is the continuous loss of energy by charged particles as they ionise atoms while traversing matter.
• Minimum ionising particle : A minimum ionising particle is a charged particle whose ionisation energy loss per unit length reaches a minimum in the relevant energy range.
• Hadronic interaction length : Hadronic interaction length is the mean distance between strong-interaction collisions of relativistic hadrons in a given medium.
• Radiation length : Radiation length is the characteristic distance over which high-energy electrons lose energy significantly via bremsstrahlung, setting the scale for electromagnetic shower development.
• Electromagnetic fraction : Electromagnetic fraction is the part of a hadronic shower energy that appears in an electromagnetic sub-shower, mainly from \pi^0\to\gamma\gamma decays.

📝 Essential Points

• Charged hadrons lose energy continuously through ionisation while also undergoing strong interactions with nuclei in the medium.
• Hadronic showers develop through a cascade of secondary particles produced in primary hadronic interactions.
• The nuclear interaction length $\lambda_I$ is defined as the mean distance between hadronic interactions of relativistic hadrons.
• The nuclear interaction length is significantly larger than the radiation length, e.g. for iron $\lambda_I\approx 17\,\text{cm}$ versus radiation length $\approx 1.8\,\text{cm}$.
• Hadronic showers are more variable than electromagnetic showers because many different final states can occur in high-energy hadronic interactions.
• Neutral pions produced in hadronic showers decay essentially immediately via $\pi^0\to\gamma\gamma$, creating an electromagnetic component whose energy fraction fluctuates event-by-event.

💡 Memory Hook

Ionisation is the steady “drip” for charged tracks; hadronic interactions are the rarer “hits” set by $\lambda_I$ (bigger than radiation length).

📖 11. Electromagnetic showers and critical energy

🔑 Key Concepts & Definitions

• Missing momentum : Missing momentum is the negative vector sum of measured particle momenta in an event, used to infer undetected particles.
• Tau-lepton : The tau-lepton is a heavy lepton that decays rapidly, so it is identified through its decay products and associated missing momentum.
• Hadronisation : Hadronisation is the QCD process that converts the energy in the strong field between quarks into new quark–antiquark pairs, forming hadrons.
• Jet : A jet is the collimated spray of particles produced when a high-energy quark or gluon fragments into hadrons.
• b-quark tagging : b-quark tagging is the experimental identification of b-quark jets by reconstructing a displaced secondary vertex from b-hadron decay.

📝 Essential Points

• Missing momentum is defined as $\vec p_{\rm mis}=-\sum_i \vec p_i$, and it should be near zero if all collision products are detected in the centre-of-mass frame.
• Significant missing momentum indicates the presence of an undetected neutrino in the event.
• Tau-leptons have a lifetime of $2.9\times10^{-13}$ s and are identified from their decay products plus missing momentum from neutrinos.
• Main tau decay modes include $\tau^-\to e^-\nu_e\nu_\tau$ (17.8%), $\tau^-\to\mu^-\nu_\mu\nu_\tau$ (17.4%), $\tau^-\to\pi^-(n\pi^0)\nu_\tau$ (48%), and $\tau^-\to\pi^-\pi^+\pi^-(n\pi^0)\nu_\tau$ (15%).
• Hadronic tau decays typically yield one or three charged pions and zero, one, or two $\pi^0$, with $\pi^0\to\gamma\gamma$ producing photons.
• In high-energy jets, particle separation is often smaller than calorimeter segmentation, so jet energy and momentum are obtained from total calorimeter deposits.

💡 Memory Hook

Missing momentum points to neutrinos: if the vector sum of what you see isn’t zero, something invisible carried momentum away.

📖 12. Electromagnetic calorimeters and shower containment

🔑 Key Concepts & Definitions

• Electromagnetic calorimeter : An electromagnetic calorimeter is a detector that measures the energy of electromagnetic showers by absorbing them in dense material.
• Shower containment : Shower containment is the design goal of choosing absorber thickness so most of an electromagnetic shower’s energy is deposited inside the calorimeter.
• Radiation length X0 : Radiation length is the material scale that characterizes how quickly high-energy electrons and photons lose energy via electromagnetic processes.
• Critical energy Ec : Critical energy is the energy where ionization losses and radiative losses for an electron become comparable in a given material.
• Gaussian beam profile : A Gaussian beam profile describes the transverse particle density of accelerator beams as a 2D Gaussian in x and y.

📝 Essential Points

• The number of interactions for a process is $N=\sigma\int L(t)dt$, so event counting requires the integrated luminosity.
• Instantaneous luminosity for head-on Gaussian beams is $L=\frac{f\,n_1n_2}{4\pi\sigma_x\sigma_y}$, with $f$ the bunch-collision frequency.
• Because beam transverse properties are not known precisely, cross sections are often extracted using a reference process: $\sigma=\sigma_{ref}\,\frac{N}{N_{ref}}$ (plus efficiency/background corrections).
• For electromagnetic shower containment, absorber thickness is estimated using radiation length $X_0$ and critical energy $E_c$ (given for tungsten as $X_0=0.35\,\text{cm}$ and $E_c=7.97\,\text{MeV}$).
• A 500 GeV electron electromagnetic shower in tungsten is “fully contained” by choosing a thickness large compared with the characteristic shower development scale set by $X_0$ and $E_c$.
• In the LHC, bunch spacing is 25 ns giving $f=40\,\text{MHz}$, which enters the luminosity calculation.

💡 Memory Hook

Containment is set by two material scales: $X_0$ (how fast the shower develops) and $E_c$ (where it slows via ionization).

📅 Key Dates

📊 Synthesis Tables

Standard Model interaction vertices

⚠️ Common Pitfalls & Confusions

1. Mixing up which force changes flavour: only the weak charged-current interaction changes flavour at the vertex, while electromagnetic and strong interactions do not.
2. Thinking gluons couple to electric charge: in QCD gluons couple to colour currents, and only quarks carry colour charge.
3. Confusing confinement with asymptotic freedom: confinement dominates at low energies/long distances, while asymptotic freedom makes QCD effectively weaker at high energies/short distances.
4. Using absolute neutrino masses instead of mass-squared differences: oscillations depend on relative phases and in the relativistic regime are expressed using Δm².
5. Assuming missing momentum is always zero: it should be near zero only if all collision products are detected in the centre-of-mass frame; neutrinos make it nonzero.
6. Forgetting that weak decays are suppressed at low energies because the W boson is very massive, even though the intrinsic weak coupling αW is larger than QED’s α.
7. Interpreting “minimum ionising” as “minimum energy”: it refers to the minimum of dE/dx versus βγ (around βγ ≈ 3), not to the particle’s total energy.

✅ Exam Checklist

1. State what flavour symmetry means and distinguish isospin SU(2) from SU(3) flavour symmetry in terms of which quark flavours are grouped.
2. Explain why flavour symmetry is approximate, and describe how symmetry representations guide construction of baryon states from quark content and flavour quantum numbers.
3. Define the QCD local gauge principle and colour SU(3) gauge symmetry, and state what a gluon is in this framework.
4. Describe how non-Abelian SU(3) leads to gluon self-interactions, and connect gauge invariance to the structure of the QCD covariant derivative and allowed vertices.
5. Define colour confinement and asymptotic freedom, and state which energy/length regimes each dominates.
6. In e+e− annihilation, explain how hadronic final states arise via quark–antiquark hadronisation through QCD confinement.
7. For hadron–hadron collisions, state the parton model picture and explain what colour factors are and why they weight amplitudes.
8. Explain why only coloured partons participate in the strong interaction and how unobserved gluon exchange leads to sums over allowed time-orderings.
9. Define the weak charged-current interaction and describe which quark pairs it couples (up-type to down-type) and how this enables flavour change.
10. Relate the coupling constant g to the scaling of amplitudes and probabilities at vertices, and explain why using a dimensionless α ∝ g² is convenient.
11. Describe the chiral structure of the charged-current weak interaction and explain what the W-boson propagator represents in amplitudes.
12. Use muon decay to explain the “negative time direction” arrow as an antiparticle (electron antineutrino) and connect this to the flavour structure of the decay.
13. State lepton universality and explain how neutrino scattering transfers energy–momentum to targets.
14. Use the Bethe–Bloch discussion to explain why dE/dx is largest at low velocity (1/v²) and why it rises slowly at relativistic speeds (log in (βγ)²).