Heavy quark production in e + e - & pp collisions
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1 Heavy quark production in e + e - & pp collisions Seminar talk by Bernhard Maaß 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 1
2 Outline I. Introduction to heavy quark production II. Producing quarks in e + e - collisions III. Hadronic structure and e - p collisions IV. Advanced experiments: pp collisions 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 2
3 Introduction to heavy quark production 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 3
4 Heavy quarks charm: SLAC and Brookhaven e + e - annihiliation (1974) bottom: Fermilab p-nucleus (1977) top: Tevatron p + p - annihilation (1995) 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 4 Source: wikipedia: quark
5 collider... SLAC: acceleration of e + and e - up to 50 GeV Tevatron: acceleration of p + and p - up to 900 GeV (when discovering top-quarks) 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 5 Source: wikipedia: SLAC, Tevatron
6 ... and particle detectors CDF-Detector from Tevatron 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 6 Source: [povh]
7 Producing quarks in e + e - collisions 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 7
8 e + e - annihilation the basic process e + + e - q + q all weak/em-interacting particles can be produced 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 8 Source: [povh]
9 muon production as reference Muon production e + + e - µ + + µ - EM-process due to high Z o mass easy to calculate µ-mass: MeV τ-mass: 1.777GeV Z o -mass: 91.2 GeV reaction cross section: Bhabha-Diffraction 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 9 Source: [povh]
10 lepton universality lepton universality / leptons are point-masses (< m) 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 10 Source: [povh]
11 Resonances and quarks Resonances with light and heavy quarks are observed charm bottom top maximum e + e - collider cm-energy: ~ 172 GeV 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 11 Source: [povh]
12 between the resonance free quarks can be produced between the resonances. e + e - qq Hadrons Due to color confinement, the quark/antiquark-pair will immediatly hadronize ( fragmentation ) 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 12 Source: [bethke]
13 Fragmentation The (pertubative) process is on a scale of d << 1fm e + e - qq Hadrons The fragmentation process occurs on much larger scales - d >> 1fm Every quark/antiquark will hadronize and therefore: σ(e + e - qq ) =σ(e + e - Hadrons) when σ(qq Hadrons) = Dezember 2013 IKP TU Darmstadt Bernhard Maaß 13
14 Charm discovery Discovery of the charm-quark: The charm decays (mainly) into Pions and Kaons. These particles have to be detected and identified. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 14 Source: [charm], [charm2]
15 Production ratio Cross section ratio: The cross sections of the different quark flavours are summed up: 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 15 Source: [berger], [povh]
16 Stepwise quark production 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 16 Source: [berger]
17 Gluons and QCD corrections Quarks can emitt gluons due to strong interaction: e + + e - q + q + g A pertubative calculations yields: 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 17 Source: [berger]
18 Jets After fragmentation of the quarks, the hadrons can be detected as jets. The ratio 2-jet/3-jet events allows the determination of the strong coupling α s 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 18 Source: [povh]
19 Hadronic structure and e - p collisions 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 19
20 Parton modell Parton model: The proton consists of partons which are involved in the scattering process. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 20 Source: [povh]
21 Deep inelastic scattering inelastic scattering: e + p e + X at higher (virtual) photon energies, the proton sub-structure is revealed: it contains three quarks. < 1 GeV > 1 GeV 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 21 1 GeV ~ 1.24fm Source: [bethke]
22 Scaling and scaling violation scaling of structure function......and scaling violation 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 22 Source: [povh],[ berger]
23 sea quarks and gluons Sea quarks and gluons contribute to the proton structure function. They are revealed at higher scattering energies. << 1 GeV 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 23 Source: [bethke]
24 Structure function The parton distribution function can be calculated via DGLAPequations. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 24 Source: [strucfunrpp]
25 Advanced experiments: pp collisions 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 25
26 proton-proton collisions hard process: scattering of pointlike proton constituents. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 26 Source: [beck]
27 Hard and soft processes hard process: the proton structure does not change in the time of the scattering process. It can be calculated pertubative. soft process: in the soft reaction, the quarks fragmentize and form hadrons. This takes place in an infinite time frame. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 27 Source: [bethke]
28 Factorization Factorization describes the total scattering cross section, which links the parton densities and the cross section of the hard process. The independence of these elements are a great simplification of the model. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 28 Source: [kraemer]
29 Event detection Detectable are the particle jets which emerge from the hard scattering process. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 29 Source: wikipedia: top antitop quark event, www-cdf.fnal.gov
30 top-quark detection The decay channels can be reconstructed and their cross sections and branching ratios be determined. The top quark decays in bottom quarks before hadronization because of their big mass. A significant signal is a six-jet-event. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 30 Source: [abe],[beck]
31 top-quark detection The invariant mass of different decay modes can be combined to the top-quark resonance 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 31 Source: www-cdf.fnal.gov, [abe]
32 Summary Depending on the c.m. energy, all quarks can be produced in e + e - collisions. This is easy in theory because of the point-like leptons, but it is difficult to reach sufficient energies. pp-collisions have higher energies, but the proton sub-structure causes difficulties when extracting reaction cross sections. This can be avoided because the hard process in which the quarks are produced occurs to be on a much smaller length and time scale than the soft hadronization (fragmentation) process the soft and the hard process factorize. The other partons do not participate in the process as well. 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 32
33 Acknowledgment Thank you for your attention. Also, thanks a lot to Professor Friman for the mentoring and support! 12. Dezember 2013 IKP TU Darmstadt Bernhard Maaß 33
34 References Image sources: [abe]: F. Abe, M. G. Albrow et al. Evidence for top quark production in pp collisions at s=1.8 TeV Physical Review D, Volume 50, Nr. 5, [beck]: Beck, Douglas H. et al. Top quark physics at hadron colliders Springer-Verlag, Advances in the Physics of Particles and Nuclei, Volume 28, 2006 [berger]: Berger, C. Elementarteilchenphysik Springer-Verlag, 2. Auflage, 2006 [bethke]: Bethke, S. QCD, Jets, Strukturfunktionen Vorlesungspräsentation des Max-Planck-Instituts, 2003 [charm]: Q. S. Abrams, J.-E. Augustin et al. Discovery of a Narrow Resonance in e+e- Annihilation Physical Review Letters, Volume 33, Nr. 23, [charm2]: J. Kogut, L. Susskindt Electron-Positron Annihilation at and above the Threshold for Production of Charmed Hadrons Physical Review Letters, Volume 34, Nr. 12, [kraemer]: M. Krämer Heavy Quark Production at High Energy Colliders Presentation at Zeus Collaboration Meeting, University of Edinburgh, October 2001 [berger]: B. Povh Teilchen und Kerne Springer-Verlag, 8. Auflage, Dezember 2013 IKP TU Darmstadt Bernhard Maaß 34
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