Introduction to Feynman Diagrams and Dynamics of Interactions
... The basic vertex shows the coupling of a charged particle (an electron here) to a quantum of the electromagnetic field, the photon. Note that in my convention, time flows to the right. Energy and momentum are conserved at each vertex. Each vertex has a coupling strength characteristic of the interac ...
... The basic vertex shows the coupling of a charged particle (an electron here) to a quantum of the electromagnetic field, the photon. Note that in my convention, time flows to the right. Energy and momentum are conserved at each vertex. Each vertex has a coupling strength characteristic of the interac ...
Dilepton production
... • The x’s are the momentum fraction carried by the fusing partons. • 1-x is carried away by the other constituents. These fragment into a cloud of mostly low momentum pions. • Worried about the lack of anti-valence quarks at ...
... • The x’s are the momentum fraction carried by the fusing partons. • 1-x is carried away by the other constituents. These fragment into a cloud of mostly low momentum pions. • Worried about the lack of anti-valence quarks at ...
Oleg Teryaev
... Coupling <-> decay width ||=|<2j|BH>| T(+P=C) invariance
Crossing from t- to s-channel gluons
BH complementarity (Lab vs “comoving” frames)?
Relation of Gravity (Hawking radiation) and QCD (jet
fragmentation)
Return to classical picture – quantum production of
singlet quantum (quark-gluon) st ...
... Coupling <-> decay width |
Comparison of y-scaling for Electrons and Hadrons
... at intermediate energies and momentum transfers. Scaling, with several variables condensed into just one, has served to unify many efforts. Electron-nuclear physics goes by a very well-known reaction mechanism. Although the strong interaction complicates analysis of inclusive hadron scattering at si ...
... at intermediate energies and momentum transfers. Scaling, with several variables condensed into just one, has served to unify many efforts. Electron-nuclear physics goes by a very well-known reaction mechanism. Although the strong interaction complicates analysis of inclusive hadron scattering at si ...
PHYS4016 Nuclear Physics
... main models for heavier nuclei: the Liquid Drop Model, the Fermi Gas Model and the Shell Model, and be able to explain nuclear structure in their terms. The students should understand and be able to operate with the mathematical formalism of scattering, both using electrons and nucleons ...
... main models for heavier nuclei: the Liquid Drop Model, the Fermi Gas Model and the Shell Model, and be able to explain nuclear structure in their terms. The students should understand and be able to operate with the mathematical formalism of scattering, both using electrons and nucleons ...
PPTX
... • Long story short – somehow this trick is working • Modern event generators use NLL based calculations to describe jet fragmentation • Also need to supplement it with some model to convert quarks and gluons into hadrons • Local Parton Hadron Duality – one parton gives you roughly one hadron during ...
... • Long story short – somehow this trick is working • Modern event generators use NLL based calculations to describe jet fragmentation • Also need to supplement it with some model to convert quarks and gluons into hadrons • Local Parton Hadron Duality – one parton gives you roughly one hadron during ...
#NSLive Mysteries of matter: What the LHC will discover next
... All potential data of the five lattices have been scaled to a universal curve by subtracting Vo and measuring energies and distances in appropriate units of &E. The dashed curve correspond to V(R) = R — ~/12R. Physical units are calculated by exploiting the relation &cr =420 MeV. ...
... All potential data of the five lattices have been scaled to a universal curve by subtracting Vo and measuring energies and distances in appropriate units of &E. The dashed curve correspond to V(R) = R — ~/12R. Physical units are calculated by exploiting the relation &cr =420 MeV. ...
LECTURE 22 THE STRONG COUPLING CONSTANT, QUARK-GLUON PLASMA (QGP)
... of the fine structure constant α in QED To account for the quark confinement, we need to add a confining potential ...
... of the fine structure constant α in QED To account for the quark confinement, we need to add a confining potential ...
PHY 551 - Stony Brook University
... Model is a Quantum Field Theory: the union of Quantum ChromoDynamics (QCD) and the electro-weak theory. Standard ...
... Model is a Quantum Field Theory: the union of Quantum ChromoDynamics (QCD) and the electro-weak theory. Standard ...
kavic_Poster0216
... dimensions with a large number of colors. The primary focus of our research is to construct the spectrum of gauge-invariant glueball states. In the 2+1 case, we use a Hamiltonian approach proposed by Karabali, Kim, and Nair (1997) in which the theory is rewritten in terms of gauge-invariant “corner” ...
... dimensions with a large number of colors. The primary focus of our research is to construct the spectrum of gauge-invariant glueball states. In the 2+1 case, we use a Hamiltonian approach proposed by Karabali, Kim, and Nair (1997) in which the theory is rewritten in terms of gauge-invariant “corner” ...
LOYOLA COLLEGE (AUTONOMOUS), CHENNAI – 600 034
... 1. Find the determinant value of the Loerntz transformation matrix. 2. State the relation between relativistic energy and relativistic momentum. 3. Define 4-current and write down the continuity equation in terms of it. 4. State the covariant form of Lorentz force equation. 5. Define differential sc ...
... 1. Find the determinant value of the Loerntz transformation matrix. 2. State the relation between relativistic energy and relativistic momentum. 3. Define 4-current and write down the continuity equation in terms of it. 4. State the covariant form of Lorentz force equation. 5. Define differential sc ...
Neutron Scattering Theory - Oklahoma State University
... • Time-independent Schrodinger wave equation: Hψ = Eψ Where, H is Hamiltonian operator. ...
... • Time-independent Schrodinger wave equation: Hψ = Eψ Where, H is Hamiltonian operator. ...
Quantum Mechanical Derivation of the Wallis Formula for $\ pi$
... A famous pre-Newtonian formula for π is obtained directly from the variational approach to the spectrum of the hydrogen atom in spaces of arbitrary dimensions greater than one, including the physical three dimensions. ...
... A famous pre-Newtonian formula for π is obtained directly from the variational approach to the spectrum of the hydrogen atom in spaces of arbitrary dimensions greater than one, including the physical three dimensions. ...
Kang_3
... How are quarks and gluons distributed spatially? How do partons carry the proton spin-1/2? (spin and orbital angular momentum) How are these quark and gluon distributions correlated with overall nucleon properties, such as spin direction? ...
... How are quarks and gluons distributed spatially? How do partons carry the proton spin-1/2? (spin and orbital angular momentum) How are these quark and gluon distributions correlated with overall nucleon properties, such as spin direction? ...
Tutorial 1 - NUS Physics Department
... 7. In reactions of the type A B A C1 C2 (in which particle A scatters off particle B, producing C1 , C2 ,) , there is another inertial frame [besides the lab (B at rest) and the CM (PTOT = 0 )] which is sometimes useful. It is called the Breit, or “brick wall,” frame, and it is the syst ...
... 7. In reactions of the type A B A C1 C2 (in which particle A scatters off particle B, producing C1 , C2 ,) , there is another inertial frame [besides the lab (B at rest) and the CM (PTOT = 0 )] which is sometimes useful. It is called the Breit, or “brick wall,” frame, and it is the syst ...
Asymptotic Freedom: From Paradox to Paradigm
... Screening by virtual particles wipes out interactions The demise of quantum field theory was widely proclaimed - and welcomed! ...
... Screening by virtual particles wipes out interactions The demise of quantum field theory was widely proclaimed - and welcomed! ...
see flyer - Centre for Research in String Theory
... "The strong nuclear force binding the nucleus is described very well by Quantum Chromo-Dynamics (QCD) which has been directly tested in high energy collisions of elementary particles. However, extracting quantitative predictions from QCD for low energy or macroscopic phenomena is one of the outstand ...
... "The strong nuclear force binding the nucleus is described very well by Quantum Chromo-Dynamics (QCD) which has been directly tested in high energy collisions of elementary particles. However, extracting quantitative predictions from QCD for low energy or macroscopic phenomena is one of the outstand ...
On-Shell Methods in Quantum Field Theory
... events have high multiplicity of hard clusters (jets) each jet has a high multiplicity of hadrons higher-order perturbative corrections are important ...
... events have high multiplicity of hard clusters (jets) each jet has a high multiplicity of hadrons higher-order perturbative corrections are important ...
Homework Set No. 4, Physics 880.02
... at the Born level shown in the figure below. The figure is for the amplitude, which needs to be squared and multiplied by appropriate factors to get the cross section. ...
... at the Born level shown in the figure below. The figure is for the amplitude, which needs to be squared and multiplied by appropriate factors to get the cross section. ...
Problem set 7
... Problem set 7 Due by beginning of class on Monday Mar 5, 2012 BCH formula for x and p , SHO 1. Consider the function f (t) = etA Be−tA where A, B are a pair of operators (e.g. position and momentum or creation and annihilation operators etc.). t is a parameter which could be a time interval or a spa ...
... Problem set 7 Due by beginning of class on Monday Mar 5, 2012 BCH formula for x and p , SHO 1. Consider the function f (t) = etA Be−tA where A, B are a pair of operators (e.g. position and momentum or creation and annihilation operators etc.). t is a parameter which could be a time interval or a spa ...
CHAPTER 5 : EXAMPLES IN QUANTUM γ e- → γ e- ∎ ELECTRODYNAMICS
... These were important experiments in the history of high-energy physics. From the particle data group, the figure shows the ratio R = σ ( e e → hadrons ) / σ ( e ebar → μ μbar) . The underlying process in hadron production is e- + e+ → q + qbar. Neglecting QCD interactions we would just have R = cons ...
... These were important experiments in the history of high-energy physics. From the particle data group, the figure shows the ratio R = σ ( e e → hadrons ) / σ ( e ebar → μ μbar) . The underlying process in hadron production is e- + e+ → q + qbar. Neglecting QCD interactions we would just have R = cons ...
12.5.2. QCD
... Evidence of the existence of gluons can be gleaned from the structure functions of deep inelastic scattering. ...
... Evidence of the existence of gluons can be gleaned from the structure functions of deep inelastic scattering. ...