XVIII SEMINARIO NAZIONALE di FISICA NUCLEARE E SUBNUCLEARE. Fisica dello Spin. Mauro Anselmino Torino University and INFN . Why spin ….?.
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XVIII SEMINARIO NAZIONALE di FISICA NUCLEARE E SUBNUCLEARE
Fisica dello Spin
Mauro Anselmino Torino University and INFN
Why spin ….?
Spin is one of the most fundamental concepts in physics, deeply rooted in Poincaré invariance and hence in the structure of space-time itself. All elementary particles we know today carry spin, among them the particles that are subject to the strong interactions, the spin-1/2 quarks and the spin-1 gluons. Spin, therefore, plays a central role also in our theory of the strong interactions, Quantum Chromodynamics (QCD), and to understand spin phenomena in QCD will help to understand QCD itself.
Research Plan for Spin Physics at RHIC, 2005
Polarized Deep Inelastic Scattering: exploring the proton longitudinal spin structure
Surprises:Transverse Single Spin Asymmetries(unintegrated polarized parton distributions)
The last missing piece of the proton structure:transversity
Polarized Deep Inelastic Scattering
What do we know, and how, about the proton structure?
Main source of information is DIS
parity conserving case (one photon exchange)
measuring dσ one extracts information on the structure functionsF1, F2, g1andg2
F1,2related toq(x,Q2), g(x,Q2 ) quark, gluon distributions
g1 related to∆q(x,Q2), ∆g(x,Q2)quark, gluonhelicity distributions
QCD parton model
de Florian, Navarro, Sassot
Dirk Ryckbosh, DIS 2005
Research Plan for Spin Physics at RHIC
February 11, 2005
Figure 11: Left: results for Δg(x,Q2 = 5GeV2) from recent NLO analyses [1, 2, 36] of polarized
DIS. The various bands indicate ranges in Δg that were deemed consistent with the scaling
violations in polarized DIS in these analyses. The rather large differences among these bands
partly result from differing theoretical assumptions in the extraction, for example, regarding the
shape of Δg(x) at the initial scale. Note that we show xΔg as a function of log(x), in order
to display the contributions from various x-regions to the integral of Δg. Right: the “net gluon
polarization” Δg(x,Q2)/g(x,Q2) at Q2 = 5 GeV2, using Δg of  and its associated band,
and the unpolarized gluon distribution of .
de Florian, Navarro, Sassot
Direct measure of Δg needed
large pT di-hadron production in SIDIS
pQCD elementary interactions
polarized case: measure
pQCD elementary asymmetries
RHIC proposal 2005
prompt photon production at RHIC
Flavour separation -W production at RHIC
parity violating longitudinal single spin asymmetry
Flavour decomposition in SIDIS,
large x behaviour
Charged–Current Deep-Inelastic Scattering (neutrino factory)
S. Forte, M. Mangano, G. Ridolfi
LO QCD parton model results
Some combinations of the polarized structure functions are of particular interest. For example: