- Hadrons like baryons and mesons were originally classified based on their properties, and were later found to be constructed from more fundamental particles called quarks.
- There were initially three quark flavors - up, down, and strange. Mesons are quark-antiquark pairs while baryons contain three quarks.
- Additional quark flavors of charm, bottom, and top were discovered through the discovery of new hadrons that could not be explained by the original three quark flavors alone.
This document provides an overview of elementary particles. It discusses their classification into baryons, leptons, and mesons. Baryons include protons, neutrons, and heavier hyperons. Leptons contain electrons, photons, neutrinos, and muons. Mesons have masses between baryons and leptons. Each particle is described along with its properties. The document also discusses particles and their antiparticles, and conservation laws related to parity, charge conjugation, time reversal, and the combined CPT symmetry.
Quarks are elementary particles that combine to form composite particles like protons and neutrons. There are six types of quarks that differ in their mass and electric charge. Quarks are never found in isolation due to the strong force and possess properties like spin, electric charge, and color charge. The up, down, charm, strange, top, and bottom quarks make up three generations and have corresponding antiquarks. Experiments in the 1960s-70s discovered quarks were the constituents of protons and neutrons. The quark model helped explain experimental results and is part of the Standard Model of particle physics.
The document discusses the four fundamental particles that make up all ordinary matter - up quarks, down quarks, strange quarks, and charm quarks. Murray Gell-Mann named quarks after a line in James Joyce's book "Finnegan's Wake" and received the 1969 Nobel Prize for his work classifying elementary particles. As particle accelerators achieve higher energies, they can probe matter at finer scales and produce more massive objects via E=mc^2, leading to the discoveries of heavier quarks like bottom and top quarks.
The Zeeman effect occurs when spectral lines split into multiple components in the presence of an external magnetic field. In 1896, Zeeman first observed this effect when placing a sodium light source between electromagnets. Normally, lines split into three components, but more complex splitting can occur. Later theories by Lorentz and others explained the polarization and patterns observed. Both classical and quantum mechanics can explain normal Zeeman splitting, while anomalous splitting requires quantum theory accounting for electron spin. Today, the Zeeman effect provides insights into atomic structure and is used in applications like solar magnetic field analysis.
This document is a project report submitted by Priyanka Verma and Smriti Singh for their Bachelor of Science degree in physics. It discusses elementary particles, including their characteristics, classification, conservation laws, and examples like electrons, positrons, protons, neutrons, pions, and kaons. The report includes certificates of completion from their college principal and physics professors.
Magnetic properties and SuperconductivityVIGHNESH K
油
Magnetic properties and superconductivity, meissner effect, superconductors, bcs theory, applications of superconductors, cooper pair, magnetic materials, hystersis, high temperature suerconductors, Types of suerconductors, high temperature superconductors, magnetism,right hand rule
This document discusses magnetic properties of solids. It defines key terms like magnetization, magnetic susceptibility, paramagnetism and diamagnetism. Paramagnetism occurs in materials with partially filled electron subshells, allowing isolated atomic magnetic dipole moments to align with an external magnetic field. Diamagnetism is a weaker effect where an applied field induces orbital electron currents that create a magnetic field opposing the external field. The document outlines the classical and quantum mechanical origins of these magnetic behaviors.
weiss molecular theory of ferromagnetismsantoshkhute
油
Weiss' Theory (Domain theory of ferromag : According to weiss, a feromagnetic substance. contains atoms with permanent magnetic. moments, as in a paramagnetic substance, but due to special form of interaction.
This document provides an overview of semiconductor theory and devices. It begins by introducing the three categories of solids based on electrical conductivity: conductors, semiconductors, and insulators. It then discusses band theory, which models the allowed energy states in solids as continuous bands separated by forbidden gaps. Semiconductors are defined as having energy gaps small enough for thermal excitation of electrons between bands. The document covers models like the Kronig-Penney model that explain energy gaps. It also discusses how temperature affects resistivity in semiconductors by increasing the number of electrons excited into the conduction band.
This document discusses statistical mechanics and the distribution of energy among particles in a system. It provides 3 main types of statistical distributions based on the properties of identical particles: Maxwell-Boltzmann, Bose-Einstein, and Fermi-Dirac statistics. Maxwell-Boltzmann statistics applies to distinguishable particles, while Bose-Einstein and Fermi-Dirac apply to indistinguishable particles (bosons and fermions respectively), with the key difference being that fermions obey the Pauli exclusion principle. The document also discusses applications of these distributions, including the Maxwell-Boltzmann distribution law for molecular energies in an ideal gas.
This chapter discusses the optical properties of phonons in materials. It covers:
1) Optical and acoustic phonons - some interact directly with light, others cause light scattering.
2) Optical excitation of phonons - how phonons contribute to optical properties through the dielectric function.
3) Phonon polaritons - mixed phonon-photon excitations in crystals near resonance frequencies.
4) Light scattering - concepts of Brillouin, Raman, and Rayleigh scattering involving phonons.
5) Coherent Raman spectroscopy - an experimental technique that enhances weak Raman scattering signals.
1. The document discusses different types of magnetism, including ferromagnetism.
2. Ferromagnetism is described as the strongest type of magnetism, which is why it is used in many technological devices. Everyday examples include refrigerator magnets.
3. Ferromagnetic materials become magnetic due to the alignment of electron spins within the material. At temperatures above the Curie point, the electron spins become disordered and the material loses its magnetism.
This document discusses the magnetic properties of diamagnetic and paramagnetic materials. Diamagnetic materials are repelled by magnetic fields as they create an induced magnetic field in the opposite direction. They have no permanent dipoles. Paramagnetic materials are weakly attracted to magnetic fields as they have some unpaired electrons that create a net magnetic moment parallel to an applied field. The key difference is that paramagnetic materials are attracted to fields while diamagnetic materials are repelled.
The document discusses atomic magnetic moments, which can be classified into two types: orbital magnetic moments, due to an electron's orbital angular momentum as it orbits the atom's nucleus, and spin magnetic moments, due to the electron's intrinsic spin. An orbiting electron creates an equivalent orbital magnetic dipole moment, while the electron's spin results in a spin magnetic moment that precesses around the atom.
This document discusses energy bands in solids and classifications of materials based on their band structure. It explains that in solids, electron energy levels form bands of allowed energies separated by forbidden bands. Materials are classified as conductors, insulators or semiconductors depending on their band gap. Conductors have overlapping bands resulting in no band gap, insulators have a large band gap, and semiconductors have a narrow band gap that allows excitation of electrons with small amounts of energy. Intrinsic and extrinsic semiconductors are also described based on their pure or doped material composition and charge carrier types.
The Zeeman effect is the splitting of a spectral line into multiple spectral lines when in the presence of a magnetic field. It was first observed in 1896 by Dutch physicist Pieter Zeeman when he placed a sodium flame between magnetic poles and observed the broadening of spectral lines. Zeeman's discovery earned him the 1902 Nobel Prize in Physics. The pattern and amount of splitting provides information about the strength and presence of the magnetic field.
Difference b/w electron, neutron and X-ray diffraction and advantagesBHOLU RAM SWAMI
油
This document summarizes and compares three diffraction techniques: X-ray diffraction, electron diffraction, and neutron diffraction. X-ray diffraction uses X-rays with wavelengths around 1 Angstrom that interact with electron density. Electron diffraction uses electron beams with similar wavelengths that interact through electromagnetic forces. Neutron diffraction uses neutrons with wavelengths around 2 Angstrom that are scattered by atomic nuclei through nuclear forces. Each technique has advantages - X-ray diffraction is most common and convenient, electron diffraction can handle nano-sized crystals, and neutron diffraction is useful for light elements and determining magnetic structures. The document outlines the basic principles, interactions, advantages, and differences between these three diffraction methods.
This PPT gives introduction
to Dielectrics, Piezoelectrics & Ferroelectrics Materials, Methods and Applications. A quick glance at the dielectric phenomena, symmetry, classification, modelling, figures of merit and applications.
Comprehensive overview of the physics and applications of
ferroelectric
The document discusses band theory of solids and semiconductor devices. It explains that in solids, discrete electron energy levels split into bands. The valence band is fully filled while the conduction band is empty or partially filled, with a band gap separating the two. Semiconductors have a smaller band gap than insulators. Intrinsic semiconductors have equal numbers of electrons and holes, while extrinsic ones are doped with impurities. PN junctions are formed by combining P-type and N-type materials and act as diodes, allowing current in one direction. Diodes have applications as rectifiers, transistors, and other devices that convert between electrical and optical signals.
The standard model of particle physics attempts to describe the fundamental interactions of nature. It classifies all known elementary particles and their interactions via gauge bosons that mediate four fundamental forces. While successful, it is limited and does not account for gravity, dark matter, neutrino masses, inflation, or the asymmetry of matter and antimatter in the universe. Many theories beyond the standard model have been proposed to address its limitations, such as supersymmetry, grand unification, string theory, and others.
The document discusses ferromagnetism and magnetic domains. It defines ferromagnetic materials as those that exhibit spontaneous magnetization from aligned atomic magnetic moments, even without an external magnetic field. It describes how ferromagnetic materials contain many small regions called magnetic domains, where atomic dipoles are aligned within each domain. In an unmagnetized material, the domains are randomly oriented, resulting in no net magnetization. An external magnetic field causes domains aligned with the field to grow at the expense of others, through the movement of domain walls, increasing the material's overall magnetization.
1. Weiss developed a molecular field theory to explain paramagnetism, proposing that atomic magnetic moments align due to an internal molecular field proportional to the magnetization.
2. The molecular field arises from exchange interactions between neighboring atomic moments due to the Pauli exclusion principle and Coulomb interaction.
3. The Curie-Weiss law describes the paramagnetic susceptibility above the Curie temperature, relating it inversely to temperature minus the Curie-Weiss temperature.
origin of quantum physics -
Inadequacy of classical mechanics and birth of QUANTUM PHYSICS
ref: Quantum mechanics: concepts and applications, N. Zettili
This document summarizes the principles and applications of Mossbauer spectroscopy, also known as nuclear gamma resonance spectroscopy. It discusses how Mossbauer spectroscopy probes nuclei using gamma rays and measures gamma absorption spectra. It explains how nuclei in solid crystals can undergo nuclear resonance because they are bound and not free to recoil. The document also outlines several key parameters that must be satisfied for Mossbauer spectroscopy to be effective, including the energy of nuclear transitions and lifetimes of excited states. Finally, it provides examples of how Mossbauer spectroscopy has been used to identify iron oxide nanoparticles in magnetotactic bacteria.
Ferromagnetic materials have three main characteristics:
1) They become spontaneously magnetized in the absence of an external magnetic field due to parallel alignment of magnetic moments.
2) They have a magnetic ordering temperature called the Curie temperature, above which they become paramagnetic.
3) They are used in many devices like transformers, electromagnets, and computer hard drives due to their magnetic properties.
NANO106 is UCSD Department of NanoEngineering's core course on crystallography of materials taught by Prof Shyue Ping Ong. For more information, visit the course wiki at http://nano106.wikispaces.com.
1) When hydrogen gas is excited by electricity, the electrons absorb energy and move to higher energy orbits. As the electrons fall back down, they emit photons of light at specific wavelengths.
2) The wavelengths of emitted photons form distinct line spectra that are unique to hydrogen. Bohr calculated the wavelengths for the hydrogen spectral lines.
3) There are several hydrogen spectral series defined by the electron falling from different excited states to the n=1, 2, 3, 4, or 5 states. The Lyman, Balmer, Paschen, Brackett, and Pfund series occur in the ultraviolet, visible, and infrared regions of the spectrum.
The document discusses the classification and properties of fundamental particles. It explains that particles can be classified into three main categories: hadrons, which are made up of quarks; leptons, which are elementary particles not made of smaller particles; and quarks, which combine to form hadrons. The document also discusses the properties of quarks, including their relative charge, baryon number, and strangeness. It provides examples of how conservation laws, such as charge conservation, must be satisfied in particle interactions and decays.
This document provides a summary of big-bang cosmology and the evidence supporting it. It discusses how observations of the cosmic microwave background radiation, light element abundances from big-bang nucleosynthesis, galaxy rotation curves, and type 1a supernovae provide evidence that the universe began in a hot, dense state and is undergoing expansion. It also summarizes the evidence for dark matter from various astronomical observations and outlines how weakly interacting massive particles are a leading candidate. The document concludes by discussing baryogenesis and possible mechanisms for the observed matter-antimatter asymmetry of the universe.
weiss molecular theory of ferromagnetismsantoshkhute
油
Weiss' Theory (Domain theory of ferromag : According to weiss, a feromagnetic substance. contains atoms with permanent magnetic. moments, as in a paramagnetic substance, but due to special form of interaction.
This document provides an overview of semiconductor theory and devices. It begins by introducing the three categories of solids based on electrical conductivity: conductors, semiconductors, and insulators. It then discusses band theory, which models the allowed energy states in solids as continuous bands separated by forbidden gaps. Semiconductors are defined as having energy gaps small enough for thermal excitation of electrons between bands. The document covers models like the Kronig-Penney model that explain energy gaps. It also discusses how temperature affects resistivity in semiconductors by increasing the number of electrons excited into the conduction band.
This document discusses statistical mechanics and the distribution of energy among particles in a system. It provides 3 main types of statistical distributions based on the properties of identical particles: Maxwell-Boltzmann, Bose-Einstein, and Fermi-Dirac statistics. Maxwell-Boltzmann statistics applies to distinguishable particles, while Bose-Einstein and Fermi-Dirac apply to indistinguishable particles (bosons and fermions respectively), with the key difference being that fermions obey the Pauli exclusion principle. The document also discusses applications of these distributions, including the Maxwell-Boltzmann distribution law for molecular energies in an ideal gas.
This chapter discusses the optical properties of phonons in materials. It covers:
1) Optical and acoustic phonons - some interact directly with light, others cause light scattering.
2) Optical excitation of phonons - how phonons contribute to optical properties through the dielectric function.
3) Phonon polaritons - mixed phonon-photon excitations in crystals near resonance frequencies.
4) Light scattering - concepts of Brillouin, Raman, and Rayleigh scattering involving phonons.
5) Coherent Raman spectroscopy - an experimental technique that enhances weak Raman scattering signals.
1. The document discusses different types of magnetism, including ferromagnetism.
2. Ferromagnetism is described as the strongest type of magnetism, which is why it is used in many technological devices. Everyday examples include refrigerator magnets.
3. Ferromagnetic materials become magnetic due to the alignment of electron spins within the material. At temperatures above the Curie point, the electron spins become disordered and the material loses its magnetism.
This document discusses the magnetic properties of diamagnetic and paramagnetic materials. Diamagnetic materials are repelled by magnetic fields as they create an induced magnetic field in the opposite direction. They have no permanent dipoles. Paramagnetic materials are weakly attracted to magnetic fields as they have some unpaired electrons that create a net magnetic moment parallel to an applied field. The key difference is that paramagnetic materials are attracted to fields while diamagnetic materials are repelled.
The document discusses atomic magnetic moments, which can be classified into two types: orbital magnetic moments, due to an electron's orbital angular momentum as it orbits the atom's nucleus, and spin magnetic moments, due to the electron's intrinsic spin. An orbiting electron creates an equivalent orbital magnetic dipole moment, while the electron's spin results in a spin magnetic moment that precesses around the atom.
This document discusses energy bands in solids and classifications of materials based on their band structure. It explains that in solids, electron energy levels form bands of allowed energies separated by forbidden bands. Materials are classified as conductors, insulators or semiconductors depending on their band gap. Conductors have overlapping bands resulting in no band gap, insulators have a large band gap, and semiconductors have a narrow band gap that allows excitation of electrons with small amounts of energy. Intrinsic and extrinsic semiconductors are also described based on their pure or doped material composition and charge carrier types.
The Zeeman effect is the splitting of a spectral line into multiple spectral lines when in the presence of a magnetic field. It was first observed in 1896 by Dutch physicist Pieter Zeeman when he placed a sodium flame between magnetic poles and observed the broadening of spectral lines. Zeeman's discovery earned him the 1902 Nobel Prize in Physics. The pattern and amount of splitting provides information about the strength and presence of the magnetic field.
Difference b/w electron, neutron and X-ray diffraction and advantagesBHOLU RAM SWAMI
油
This document summarizes and compares three diffraction techniques: X-ray diffraction, electron diffraction, and neutron diffraction. X-ray diffraction uses X-rays with wavelengths around 1 Angstrom that interact with electron density. Electron diffraction uses electron beams with similar wavelengths that interact through electromagnetic forces. Neutron diffraction uses neutrons with wavelengths around 2 Angstrom that are scattered by atomic nuclei through nuclear forces. Each technique has advantages - X-ray diffraction is most common and convenient, electron diffraction can handle nano-sized crystals, and neutron diffraction is useful for light elements and determining magnetic structures. The document outlines the basic principles, interactions, advantages, and differences between these three diffraction methods.
This PPT gives introduction
to Dielectrics, Piezoelectrics & Ferroelectrics Materials, Methods and Applications. A quick glance at the dielectric phenomena, symmetry, classification, modelling, figures of merit and applications.
Comprehensive overview of the physics and applications of
ferroelectric
The document discusses band theory of solids and semiconductor devices. It explains that in solids, discrete electron energy levels split into bands. The valence band is fully filled while the conduction band is empty or partially filled, with a band gap separating the two. Semiconductors have a smaller band gap than insulators. Intrinsic semiconductors have equal numbers of electrons and holes, while extrinsic ones are doped with impurities. PN junctions are formed by combining P-type and N-type materials and act as diodes, allowing current in one direction. Diodes have applications as rectifiers, transistors, and other devices that convert between electrical and optical signals.
The standard model of particle physics attempts to describe the fundamental interactions of nature. It classifies all known elementary particles and their interactions via gauge bosons that mediate four fundamental forces. While successful, it is limited and does not account for gravity, dark matter, neutrino masses, inflation, or the asymmetry of matter and antimatter in the universe. Many theories beyond the standard model have been proposed to address its limitations, such as supersymmetry, grand unification, string theory, and others.
The document discusses ferromagnetism and magnetic domains. It defines ferromagnetic materials as those that exhibit spontaneous magnetization from aligned atomic magnetic moments, even without an external magnetic field. It describes how ferromagnetic materials contain many small regions called magnetic domains, where atomic dipoles are aligned within each domain. In an unmagnetized material, the domains are randomly oriented, resulting in no net magnetization. An external magnetic field causes domains aligned with the field to grow at the expense of others, through the movement of domain walls, increasing the material's overall magnetization.
1. Weiss developed a molecular field theory to explain paramagnetism, proposing that atomic magnetic moments align due to an internal molecular field proportional to the magnetization.
2. The molecular field arises from exchange interactions between neighboring atomic moments due to the Pauli exclusion principle and Coulomb interaction.
3. The Curie-Weiss law describes the paramagnetic susceptibility above the Curie temperature, relating it inversely to temperature minus the Curie-Weiss temperature.
origin of quantum physics -
Inadequacy of classical mechanics and birth of QUANTUM PHYSICS
ref: Quantum mechanics: concepts and applications, N. Zettili
This document summarizes the principles and applications of Mossbauer spectroscopy, also known as nuclear gamma resonance spectroscopy. It discusses how Mossbauer spectroscopy probes nuclei using gamma rays and measures gamma absorption spectra. It explains how nuclei in solid crystals can undergo nuclear resonance because they are bound and not free to recoil. The document also outlines several key parameters that must be satisfied for Mossbauer spectroscopy to be effective, including the energy of nuclear transitions and lifetimes of excited states. Finally, it provides examples of how Mossbauer spectroscopy has been used to identify iron oxide nanoparticles in magnetotactic bacteria.
Ferromagnetic materials have three main characteristics:
1) They become spontaneously magnetized in the absence of an external magnetic field due to parallel alignment of magnetic moments.
2) They have a magnetic ordering temperature called the Curie temperature, above which they become paramagnetic.
3) They are used in many devices like transformers, electromagnets, and computer hard drives due to their magnetic properties.
NANO106 is UCSD Department of NanoEngineering's core course on crystallography of materials taught by Prof Shyue Ping Ong. For more information, visit the course wiki at http://nano106.wikispaces.com.
1) When hydrogen gas is excited by electricity, the electrons absorb energy and move to higher energy orbits. As the electrons fall back down, they emit photons of light at specific wavelengths.
2) The wavelengths of emitted photons form distinct line spectra that are unique to hydrogen. Bohr calculated the wavelengths for the hydrogen spectral lines.
3) There are several hydrogen spectral series defined by the electron falling from different excited states to the n=1, 2, 3, 4, or 5 states. The Lyman, Balmer, Paschen, Brackett, and Pfund series occur in the ultraviolet, visible, and infrared regions of the spectrum.
The document discusses the classification and properties of fundamental particles. It explains that particles can be classified into three main categories: hadrons, which are made up of quarks; leptons, which are elementary particles not made of smaller particles; and quarks, which combine to form hadrons. The document also discusses the properties of quarks, including their relative charge, baryon number, and strangeness. It provides examples of how conservation laws, such as charge conservation, must be satisfied in particle interactions and decays.
This document provides a summary of big-bang cosmology and the evidence supporting it. It discusses how observations of the cosmic microwave background radiation, light element abundances from big-bang nucleosynthesis, galaxy rotation curves, and type 1a supernovae provide evidence that the universe began in a hot, dense state and is undergoing expansion. It also summarizes the evidence for dark matter from various astronomical observations and outlines how weakly interacting massive particles are a leading candidate. The document concludes by discussing baryogenesis and possible mechanisms for the observed matter-antimatter asymmetry of the universe.
The document discusses analyzing the underlying event in proton-proton collisions using tracks reconstructed in the ATLAS inner detector. It describes selecting tracks based on requirements on hits, transverse momentum, distance of closest approach to the beam spot or primary vertex, and fit quality. Tracks are categorized as primary vertex tracks, used to reconstruct vertices, and beam-spot tracks, used to study trigger and vertex reconstruction efficiencies independently of vertexing. The analysis aims to isolate the low-energy QCD contribution to events using measurements in the transverse region.
Talk given at Cambridge DAMTP on Friday, 20 June 2008. Describes recent work on understanding what is necessary to embed accelerating cosmology in higher-dimensional theory.
The document discusses cosmological surveys and their history. It provides an overview of several major galaxy surveys from the 1970s-present, including their sky coverage and number of galaxies observed. It also describes techniques for measuring galaxy clustering statistics like the two-point correlation function 両(r) and power spectrum P(k) from survey data, and methods for estimating errors. Finally, it summarizes the current BOSS survey, which is aiming to constrain dark energy by measuring the baryon acoustic oscillation scale to 1% in distance and 2% in Hubble parameter in two redshift bins.
The document summarizes the quantum mechanical model of the atom. It describes how electrons are located in specific energy levels called orbitals, which are regions where electrons are most likely to be found. The location of electrons is determined by four quantum numbers - principal, azimuthal, magnetic, and spin. Electrons fill these orbitals based on specific rules, such as the Aufbau principle and Hund's rule, resulting in unique electron configurations for each element.
1. Quarks
100s of hadrons (baryons and mesons) are
known
Classified in terms of their properties
(mass, spin, parity, baryon number,
Particle Physics strangeness, isospin .)
Development of a schematic classification
scheme allowed one to predict the
Quarks properties of particles
(a Periodic Table for particles)
Eventually showed that all hadrons can be
constructed from fundamental, point-like
particles called quarks (and anti-quarks)
1 2
Hadrons The Eightfold Way
1961: Gell-Mann, Neeman et al.
Particles having the same spin-parity (J)
tend to have similar masses Plot the known particles on Strangeness vs
Isospin plots
Same charge
3 4
Rohlf 17.7 Krane 18.11
2. The Eightfold Way The Eightfold Way
Successful in predicting particles
A building block ?
Are quarks real or just nice maths ?
5 6
Krane 18.12 & 13
Quarks Mesons
All quarks are spin-1/2 fermions A quark-antiquark pair qq
Fractional charge + 2 e or
3 1e
3 Mesons have B = 0. {+ 1 1 = 0}
3 3
Baryon number = +1
3
9 bound states (mesons) from the 3 basic
quarks:
Intrinsic parity is +1
uu ud us du dd ds su sd ss
+ +
侶 K 0
K 0
K K 0
侶
Initially, 3 quark flavours
Flavour Name Charge (e) (The , , 0 侶 侶 are in fact admixtures
of qq pairs)
u Up +2/3
Pseudoscalar Mesons
d Down 1/3
s Strange 1/3
7 8
3. Mesons Mesons
These 9 mesons form an Octet (8) and a Lowest energy state has the quark and anti-
Singlet (1 the 侶). with l = 0
quark spins
Interchange quarks e.g.
ds & d s (q ) = (q ) fermions
(q q ) = (q ) (q ) (1) l = 1
侶 (uu , dd , ss )
侶 侶 The lowest energy state of a meson has
Same particle J =0
K0 = d s K 0 = ds Excited energy state has the quark and
with l = 0
anti-quark spins
Different particles
J = 1
9 10
Baryons Baryons
A quark triplet Lowest energy state has the quark spins
with
l =0
Baryons have B = +1. qqq
(q ) = (q ) fermions
Antiparticles have B = 1 qqq (q qq ) = (q ) = +1
p = uud , n = udd ( q q q ) = ( q ) = 1
0 = uds, 0 = u d s
Proton u u d uud The lowest energy state of a baryon has
1+
Q +2/3 +2/3 1/3 +1 J = 2
Spin +1/2 +1/2 +1/2 +1/2
Excited energy state has the quark spins
with
B 1/3 1/3 1/3 +1
l =0
3+
T +1/2 +1/2 +1/2 +1/2 J = 2
T3 +1/2 +1/2 1/2 +1/2
11 12
4. Colour Charm
19** Discovery of the
1974 Stanford and Brookhaven:
Strangeness: S = 3 sss Discovery of the J / meson
Spin = 3/2 so Cannot be constructed from the u, d, and s
quarks and anti-quarks.
3 s quarks, in the same quantum state
violates Exclusion Principle.
Must be a fourth quark --- Charm (c).
Introduce another property Colour or
Colour Charge
q=+2e
3
NOTHING to do with visual colour
So, we have 3 quarks with the same Yet another introduced property, u, d and s
flavour i.e. s but different colours. quarks have charm = 0. The c quark has
Red, Green & Blue so when theyre charm = +1
combined, the resulting baryon is White
i.e. Colour Neutral.
Mesons are also Colour Neutral e.g. Red
& Anti-Red
13 14
Bottom (Beauty) Quarks
1977 Fermilab: Discovery of the 離
Cannot be constructed from the u, d, s and Flavour Name Charge (e)
c quarks and anti-quarks.
Must be a fifth quark --- Bottom (b) or u Up +2/3
Beauty.
d Down 1/3
q=1e
3
s Strange 1/3
Top (Truth) c Charm +2/3
Reason to suspect there are 3 families of b Bottom 1/3
quark pairs, just like the 3 generations of
leptons t Top +2/3
1997 Fermilab: Evidence for the top quark
q=+2e
3
15 16