SlideShare una empresa de Scribd logo
1 de 4
Descargar para leer sin conexión
Quarks


                                                    • 100’s 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, Ne’eman et al.
 • Particles having the same spin-parity (Jπ)
   tend to have similar masses                      • Plot the known particles on Strangeness vs
                                                      Isospin plots
                                                                                            Same charge




                                                3                                                   4

Rohlf 17.7                                          Krane 18.11
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
                                                            +        +       −                        −
                                                 η      π        K       π       π   0
                                                                                         K   0
                                                                                                  K       K   0
                                                                                                                      η′
 • Initially, 3 quark “flavours”

       Flavour Name          Charge (e)              • (The  , ,π 0 η η ′ are in fact admixtures
                                                       of qq pairs)
           u         Up            +2/3
                                                     • “Pseudoscalar Mesons”
           d       Down            −1/3

           s       Strange         − 1/3

                                             7                                                                    8
Mesons                                           Mesons

• These 9 mesons form an Octet (8) and a            • Lowest energy state has the quark and anti-
  Singlet (1 – the η′).                                                   with l = 0
                                                      quark spins
                                                                   ↑↓
• Interchange quarks e.g.

         d↔s & d ↔s                                 π (q ) = −π (q )                  fermions


                                                    ∴ π (q q ) = π (q ) ⋅ π (q ) ⋅ (−1) l = −1
         η ′ ⇒ (uu , dd , ss )

                 η′ → η′                            • The lowest energy state of a meson has
                                                                     π       −
                 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 π = 1−

                                               9                                                 10




                  Baryons                                            Baryons

• A quark triplet                                   • Lowest energy state has the quark spins
                                                      with
                                                                                                 ↑↓↑
                                                             l =0
• Baryons have B = +1.           qqq
                                                        π (q ) = −π (q )             fermions

• Antiparticles have B = −1            qqq              ∴ π (q qq ) = π (q ) = +1
          p = uud , n = udd                                π ( q q q ) = π ( q ) = −1
          Λ0 = uds, Λ0 = u d s

Proton       u          u         d     uud         • The lowest energy state of a baryon has
                                                                      π      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                       Jπ =     2
  T3       +1/2       +1/2       −1/2   +1/2
                                               11                                                12
Colour                                              Charm
• 19** Discovery of the       Ω−
                                                     • 1974 Stanford and Brookhaven:
• Strangeness:      S = −3 ⇒ sss                       Discovery of the J /  ψ    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 they’re                    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       Υ
• 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

Más contenido relacionado

La actualidad más candente

Introduction to particle physics
Introduction to particle physicsIntroduction to particle physics
Introduction to particle physicsHelen Corbett
 
ppt on Elementary Particles By Jyotibhooshan chaturvedi
ppt on Elementary Particles By Jyotibhooshan chaturvedippt on Elementary Particles By Jyotibhooshan chaturvedi
ppt on Elementary Particles By Jyotibhooshan chaturvediJyotibhooshan Chaturvedi
 
Elementary particles
Elementary particlesElementary particles
Elementary particlesSNS
 
Elementary particles and their properties
Elementary particles and their propertiesElementary particles and their properties
Elementary particles and their propertiesZeeshan Khalid
 
To the point particle physics
To the point particle physicsTo the point particle physics
To the point particle physicsShahzada Khan
 
Elementary particles
Elementary particlesElementary particles
Elementary particlesSNS
 
Nuclear Basics Summer 2010
Nuclear Basics Summer 2010Nuclear Basics Summer 2010
Nuclear Basics Summer 2010Roppon Picha
 
6563.nuclear models
6563.nuclear models6563.nuclear models
6563.nuclear modelsakshay garg
 
Standard model of particle physics
Standard model of particle physicsStandard model of particle physics
Standard model of particle physicsupvita pandey
 
Nuclear Shell models
Nuclear Shell modelsNuclear Shell models
Nuclear Shell modelsNumanUsama
 
Elementry particles project by Jyotibhooshan chaturvedi
Elementry particles project by Jyotibhooshan chaturvediElementry particles project by Jyotibhooshan chaturvedi
Elementry particles project by Jyotibhooshan chaturvediJyotibhooshan Chaturvedi
 
Basics Nuclear Physics concepts
Basics Nuclear Physics conceptsBasics Nuclear Physics concepts
Basics Nuclear Physics conceptsMuhammad IrfaN
 
Problems on fermi part 2
Problems on fermi part 2Problems on fermi part 2
Problems on fermi part 2kiranmadhale1
 
Particle Physics Today ,Tomorrow and Beyond
Particle Physics Today ,Tomorrow and BeyondParticle Physics Today ,Tomorrow and Beyond
Particle Physics Today ,Tomorrow and BeyondThiliniMaheshika2
 
nuclear binding energy
 nuclear binding energy nuclear binding energy
nuclear binding energyZeeshan Khalid
 
5 nuclear stability and radioactive decay
5 nuclear stability and radioactive decay5 nuclear stability and radioactive decay
5 nuclear stability and radioactive decayMissingWaldo
 

La actualidad más candente (20)

Strangeness in particle physics
Strangeness in particle physicsStrangeness in particle physics
Strangeness in particle physics
 
Introduction to particle physics
Introduction to particle physicsIntroduction to particle physics
Introduction to particle physics
 
ppt on Elementary Particles By Jyotibhooshan chaturvedi
ppt on Elementary Particles By Jyotibhooshan chaturvedippt on Elementary Particles By Jyotibhooshan chaturvedi
ppt on Elementary Particles By Jyotibhooshan chaturvedi
 
Elementary particles
Elementary particlesElementary particles
Elementary particles
 
Elementary particles and their properties
Elementary particles and their propertiesElementary particles and their properties
Elementary particles and their properties
 
To the point particle physics
To the point particle physicsTo the point particle physics
To the point particle physics
 
Elementary particles
Elementary particlesElementary particles
Elementary particles
 
Lect26 handout
Lect26 handoutLect26 handout
Lect26 handout
 
Nuclear Basics Summer 2010
Nuclear Basics Summer 2010Nuclear Basics Summer 2010
Nuclear Basics Summer 2010
 
6563.nuclear models
6563.nuclear models6563.nuclear models
6563.nuclear models
 
Standard model of particle physics
Standard model of particle physicsStandard model of particle physics
Standard model of particle physics
 
Nuclear Shell models
Nuclear Shell modelsNuclear Shell models
Nuclear Shell models
 
Elementry particles project by Jyotibhooshan chaturvedi
Elementry particles project by Jyotibhooshan chaturvediElementry particles project by Jyotibhooshan chaturvedi
Elementry particles project by Jyotibhooshan chaturvedi
 
Basics Nuclear Physics concepts
Basics Nuclear Physics conceptsBasics Nuclear Physics concepts
Basics Nuclear Physics concepts
 
Nuclear chemistry
Nuclear chemistry Nuclear chemistry
Nuclear chemistry
 
Problems on fermi part 2
Problems on fermi part 2Problems on fermi part 2
Problems on fermi part 2
 
Particle Physics Today ,Tomorrow and Beyond
Particle Physics Today ,Tomorrow and BeyondParticle Physics Today ,Tomorrow and Beyond
Particle Physics Today ,Tomorrow and Beyond
 
MirrorMatter
MirrorMatterMirrorMatter
MirrorMatter
 
nuclear binding energy
 nuclear binding energy nuclear binding energy
nuclear binding energy
 
5 nuclear stability and radioactive decay
5 nuclear stability and radioactive decay5 nuclear stability and radioactive decay
5 nuclear stability and radioactive decay
 

Similar a Quarks

An Overview of Cosmology
An Overview of CosmologyAn Overview of Cosmology
An Overview of CosmologyPratik Tarafdar
 
Facultyetsuedublantonlecture3radiationppt3714
Facultyetsuedublantonlecture3radiationppt3714Facultyetsuedublantonlecture3radiationppt3714
Facultyetsuedublantonlecture3radiationppt3714Michel Tamira
 
Measurements of the Underlying Event
Measurements of the Underlying EventMeasurements of the Underlying Event
Measurements of the Underlying EventGabrielHare
 
Oxidised cosmic acceleration
Oxidised cosmic accelerationOxidised cosmic acceleration
Oxidised cosmic accelerationdhwesley
 

Similar a Quarks (6)

An Overview of Cosmology
An Overview of CosmologyAn Overview of Cosmology
An Overview of Cosmology
 
Facultyetsuedublantonlecture3radiationppt3714
Facultyetsuedublantonlecture3radiationppt3714Facultyetsuedublantonlecture3radiationppt3714
Facultyetsuedublantonlecture3radiationppt3714
 
Measurements of the Underlying Event
Measurements of the Underlying EventMeasurements of the Underlying Event
Measurements of the Underlying Event
 
Oxidised cosmic acceleration
Oxidised cosmic accelerationOxidised cosmic acceleration
Oxidised cosmic acceleration
 
Surveys
SurveysSurveys
Surveys
 
QMM
QMMQMM
QMM
 

Quarks

  • 1. Quarks • 100’s 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, Ne’eman et al. • Particles having the same spin-parity (Jπ) 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 + + − − η π K π π 0 K 0 K K 0 η′ • Initially, 3 quark “flavours” Flavour Name Charge (e) • (The , ,π 0 η η ′ 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 η′). with l = 0 quark spins ↑↓ • Interchange quarks e.g. d↔s & d ↔s π (q ) = −π (q ) fermions ∴ π (q q ) = π (q ) ⋅ π (q ) ⋅ (−1) l = −1 η ′ ⇒ (uu , dd , ss ) η′ → η′ • The lowest energy state of a meson has π − 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 π = 1− 9 10 Baryons Baryons • A quark triplet • Lowest energy state has the quark spins with ↑↓↑ l =0 • Baryons have B = +1. qqq π (q ) = −π (q ) fermions • Antiparticles have B = −1 qqq ∴ π (q qq ) = π (q ) = +1 p = uud , n = udd π ( q q q ) = π ( q ) = −1 Λ0 = uds, Λ0 = u d s Proton u u d uud • The lowest energy state of a baryon has π 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 Jπ = 2 T3 +1/2 +1/2 −1/2 +1/2 11 12
  • 4. Colour Charm • 19** Discovery of the Ω− • 1974 Stanford and Brookhaven: • Strangeness: S = −3 ⇒ sss Discovery of the J / ψ 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 they’re 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 Υ • 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