The Chiral Constituent Quark Model (cCQM)
... ✰ To obtain LL and NL interaction potentials by using a constituent quark model whose parameters are already fixed from other sectors, so that it is fully predictive. ✰ To study what can we infer from this model about the H dibaryon. ...
... ✰ To obtain LL and NL interaction potentials by using a constituent quark model whose parameters are already fixed from other sectors, so that it is fully predictive. ✰ To study what can we infer from this model about the H dibaryon. ...
Aalborg Universitet The Landauer-Büttiker formula and resonant quantum transport
... eigenvectors are (exponentially) small at the contact sites, and not completely symmetric (since t1 6= t2 ). In fact, a few eigenvectors with more symmetry do generate some small peaks. The spatial localisation of the second and the sixth eigenvector is shown in Figs. 2b,c. The peak aspect changes d ...
... eigenvectors are (exponentially) small at the contact sites, and not completely symmetric (since t1 6= t2 ). In fact, a few eigenvectors with more symmetry do generate some small peaks. The spatial localisation of the second and the sixth eigenvector is shown in Figs. 2b,c. The peak aspect changes d ...
![JLab 12 GeV upgrade (3) [C3]](http://s1.studyres.com/store/data/022944901_1-077cfe868d2821e182d97c43c37805ed-300x300.png)
JLab 12 GeV upgrade (3) [C3]
... (GluEx and heavy baryon and meson spectroscopy) The transverse structure of the hadrons (rated) (Elastic and transition Form Factors) The longitudinal structure of the hadrons (rated) (Unpolarized and polarized parton distribution functions) The 3D structure of the hadrons (unrated) (Generalized Par ...
... (GluEx and heavy baryon and meson spectroscopy) The transverse structure of the hadrons (rated) (Elastic and transition Form Factors) The longitudinal structure of the hadrons (rated) (Unpolarized and polarized parton distribution functions) The 3D structure of the hadrons (unrated) (Generalized Par ...
Poster-Okubo - Department of Physics and Astronomy
... 1996 Gail G. Hanson (Indiana University) and Roy F. Schwitters (University of Texas - Austin ) "Gail Hanson and Roy Schwitters are honored for their separate contributions which together provided the first clear evidence that hadronic final states in e+e? annihilation, which are largely composed of ...
... 1996 Gail G. Hanson (Indiana University) and Roy F. Schwitters (University of Texas - Austin ) "Gail Hanson and Roy Schwitters are honored for their separate contributions which together provided the first clear evidence that hadronic final states in e+e? annihilation, which are largely composed of ...
Inclusive DIS in saturation models
... Universal gluodynamics & energy dependence of QS A.H. Mueller, hep-ph/0301109 ...
... Universal gluodynamics & energy dependence of QS A.H. Mueller, hep-ph/0301109 ...
Theory of Fundamental Interactions
... their interaction with the Higgs field. Lecture 14. Salam – Weinberg model. Fermion masses and their interaction with the Higgs field. Part 2 (10th semester). Introduction to Quantum Chromodynamics (QCD) ...
... their interaction with the Higgs field. Lecture 14. Salam – Weinberg model. Fermion masses and their interaction with the Higgs field. Part 2 (10th semester). Introduction to Quantum Chromodynamics (QCD) ...
You are going to read the chapter at home.
... Introduce a complete set of time-independent single-particle wave functions ...
... Introduce a complete set of time-independent single-particle wave functions ...
ppt
... Specifically, we have not observed a clear hybrid states with mass around 4260 MeV in the vector ...
... Specifically, we have not observed a clear hybrid states with mass around 4260 MeV in the vector ...
Slides - Agenda INFN
... Energy-loss at strong coupling? • it is unclear if the perturbative QCD approach can describe the suppression of high-pT particles in Au+Au collisions at RHIC, in particular for heavy-quark energy loss: high-pT electrons from c and b decays indicate similar suppression for light and heavy quarks, w ...
... Energy-loss at strong coupling? • it is unclear if the perturbative QCD approach can describe the suppression of high-pT particles in Au+Au collisions at RHIC, in particular for heavy-quark energy loss: high-pT electrons from c and b decays indicate similar suppression for light and heavy quarks, w ...
Document
... Wigner distribution of initial wavefunction gives seeds of fluctuations. These seeds grow when inserted into classical equations ...
... Wigner distribution of initial wavefunction gives seeds of fluctuations. These seeds grow when inserted into classical equations ...
ppt - Cyclotron Institute
... The classical field of the nucleus at high energies Saddle point of effective action-> Yang-Mills equations ...
... The classical field of the nucleus at high energies Saddle point of effective action-> Yang-Mills equations ...
Transparancies for Feynman Graphs
... KG as old as QM, originally dismissed. No spin 0 particles known. Pion was only discovered in 1948. Dirac equation of 1928 described known spin ½ electron. Also described an anti-particle – Dirac boldly postulated existence of positron Discovered by Anderson in 1933 using a cloud chamber (C.Wilson) ...
... KG as old as QM, originally dismissed. No spin 0 particles known. Pion was only discovered in 1948. Dirac equation of 1928 described known spin ½ electron. Also described an anti-particle – Dirac boldly postulated existence of positron Discovered by Anderson in 1933 using a cloud chamber (C.Wilson) ...
The positons of the three quarks composing the proton are
... the proton’s spin substructure have been made recently, employing the technique of deep inelastic scattering with spin-polarized beams bombarding spin-polarized targets. By combining these measurements with constraints from other data, one can infer the fraction of the proton’s spin carried by the i ...
... the proton’s spin substructure have been made recently, employing the technique of deep inelastic scattering with spin-polarized beams bombarding spin-polarized targets. By combining these measurements with constraints from other data, one can infer the fraction of the proton’s spin carried by the i ...
Title: Some Combinatorial Problems Inherent in and Related
... creation and annihilation operators. It will be shown that this procedure naturally leads to far reaching generalizations of classical combinatorial Bell and Stirling numbers for which closed form analytic formulas in terms of hypergeometric functions are obtained. These representations, termed exte ...
... creation and annihilation operators. It will be shown that this procedure naturally leads to far reaching generalizations of classical combinatorial Bell and Stirling numbers for which closed form analytic formulas in terms of hypergeometric functions are obtained. These representations, termed exte ...
How does mathematics Affect science?
... charge, they usually all cancel each other out. This is where math is very important. If an atom has 5 protons, 6 neutrons and 5 electrons what would the overall charge be? Think of it this way: Neutrons have no charge so don’t affect the charge. The protons and electrons do however. Turn it int ...
... charge, they usually all cancel each other out. This is where math is very important. If an atom has 5 protons, 6 neutrons and 5 electrons what would the overall charge be? Think of it this way: Neutrons have no charge so don’t affect the charge. The protons and electrons do however. Turn it int ...
PowerPoint file - University of Regina
... Quark and Gluon Structure of Hadronic Matter from Hard Scattering Understand the role of quarks and gluons in nuclei: Nuclear Binding, Quarks and gluons in nuclear medium We know that structure functions change in the nucleus Can we see x>1 effects? Are the nuclear enhancements of valence quarks, s ...
... Quark and Gluon Structure of Hadronic Matter from Hard Scattering Understand the role of quarks and gluons in nuclei: Nuclear Binding, Quarks and gluons in nuclear medium We know that structure functions change in the nucleus Can we see x>1 effects? Are the nuclear enhancements of valence quarks, s ...
Over 99% of the known mass of the universe is composed of two
... quarks and gluons. The latter serves as mediators of the strong interaction that holds the quarks together, and it is this force which is ultimately responsible for nuclear binding. One of the driving goals of nuclear physics is to characterize the fundamental properties of the nucleon to allow comp ...
... quarks and gluons. The latter serves as mediators of the strong interaction that holds the quarks together, and it is this force which is ultimately responsible for nuclear binding. One of the driving goals of nuclear physics is to characterize the fundamental properties of the nucleon to allow comp ...
New perspective of QCD at high energy
... Two basic kinematical variables in deep inelastic scattering electron(k) + proton(p) electron(k’) + X Lorentz invariant quantities ...
... Two basic kinematical variables in deep inelastic scattering electron(k) + proton(p) electron(k’) + X Lorentz invariant quantities ...
QCD and Nuclei
... “The most important unsolved problem in theoretical nuclear physics related to solar neutrinos is the range of values allowed by fundamental physics for the hep production cross section” ...
... “The most important unsolved problem in theoretical nuclear physics related to solar neutrinos is the range of values allowed by fundamental physics for the hep production cross section” ...
Physics 8805: Nuclear Few- and Many-Body Physics
... (o) If the neutron lifetime is so short, why are there any stable nuclei? ...
... (o) If the neutron lifetime is so short, why are there any stable nuclei? ...
The Lippmann-Schwinger equation reads ψk(x) = φk(x) + ∫ dx G0(x
... the moment we have put only k, k 0 to label the relative motion, but later we will put back quantum numbers for the nuclei; • accordingly, x, x0 should be a set of coordinates for the nuclei and their relative motion. This leads to the scattering amplitude Z m f (θ) = − dx0 φk0 (x0 )V (x0 )ψk (x0 ). ...
... the moment we have put only k, k 0 to label the relative motion, but later we will put back quantum numbers for the nuclei; • accordingly, x, x0 should be a set of coordinates for the nuclei and their relative motion. This leads to the scattering amplitude Z m f (θ) = − dx0 φk0 (x0 )V (x0 )ψk (x0 ). ...
ppt
... Gluons are colored Random sources evolving on time scales much larger than natural time scales-very similar to spin glasses Bosons with large occupation # ~ Typical momentum of gluons is ...
... Gluons are colored Random sources evolving on time scales much larger than natural time scales-very similar to spin glasses Bosons with large occupation # ~ Typical momentum of gluons is ...
20071008133014301
... The Quantum Vacuum Every so often quantum effects create a quark anti-quark pair. The attractive force is so strong that binding energy >> mass energy The vacuum has lower energy if it fills itself with quark antiquark pairs! ...
... The Quantum Vacuum Every so often quantum effects create a quark anti-quark pair. The attractive force is so strong that binding energy >> mass energy The vacuum has lower energy if it fills itself with quark antiquark pairs! ...