The lower blob corresponds to double quark distributions. They look like distribution functions with respect to x. Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": A parton distribution function within so called collinear factorization is defined as the probability density for finding a particle with a . Parton distributions functions (pdfs) encode the binding of the quark/ gluons within the proton.
They look like distribution functions with respect to x.
In light cone gauge parton distribution functions are matrix elements of number operators inside a hadron, so they appear to be manifestly . These distributions have hybrid properties: Parton distributions functions (pdfs) encode the binding of the quark/ gluons within the proton. Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": A parton distribution function within so called collinear factorization is defined as the probability density for finding a particle with a . The lower blob corresponds to double quark distributions. At the scale q of the hard interaction, factorization does not yield standard parton distribution functions (pdfs) for the initial state. They look like distribution functions with respect to x. A parton distribution function (pdf) within so called collinear factorization is defined as the probability density for .
A parton distribution function within so called collinear factorization is defined as the probability density for finding a particle with a . Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": The lower blob corresponds to double quark distributions. They look like distribution functions with respect to x. At the scale q of the hard interaction, factorization does not yield standard parton distribution functions (pdfs) for the initial state.
These distributions have hybrid properties:
Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": They look like distribution functions with respect to x. These distributions have hybrid properties: The lower blob corresponds to double quark distributions. At the scale q of the hard interaction, factorization does not yield standard parton distribution functions (pdfs) for the initial state. A parton distribution function within so called collinear factorization is defined as the probability density for finding a particle with a . Parton distributions functions (pdfs) encode the binding of the quark/ gluons within the proton. In light cone gauge parton distribution functions are matrix elements of number operators inside a hadron, so they appear to be manifestly . A parton distribution function (pdf) within so called collinear factorization is defined as the probability density for .
At the scale q of the hard interaction, factorization does not yield standard parton distribution functions (pdfs) for the initial state. In light cone gauge parton distribution functions are matrix elements of number operators inside a hadron, so they appear to be manifestly . Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": These distributions have hybrid properties: The lower blob corresponds to double quark distributions.
Parton distributions functions (pdfs) encode the binding of the quark/ gluons within the proton.
At the scale q of the hard interaction, factorization does not yield standard parton distribution functions (pdfs) for the initial state. A parton distribution function (pdf) within so called collinear factorization is defined as the probability density for . The lower blob corresponds to double quark distributions. These distributions have hybrid properties: They look like distribution functions with respect to x. A parton distribution function within so called collinear factorization is defined as the probability density for finding a particle with a . Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": In light cone gauge parton distribution functions are matrix elements of number operators inside a hadron, so they appear to be manifestly . Parton distributions functions (pdfs) encode the binding of the quark/ gluons within the proton.
Parton Distribution Functions : HERAFitter - HERAFitter : In light cone gauge parton distribution functions are matrix elements of number operators inside a hadron, so they appear to be manifestly .. They look like distribution functions with respect to x. Protons are a complicated quantum mechanical system made up of a large (indeterminant) number of "partons": In light cone gauge parton distribution functions are matrix elements of number operators inside a hadron, so they appear to be manifestly . A parton distribution function within so called collinear factorization is defined as the probability density for finding a particle with a . At the scale q of the hard interaction, factorization does not yield standard parton distribution functions (pdfs) for the initial state.