Measurement of the 3He spin-structure functions and of neutron (3He) spin-dependent sum rules at 0.035 ≤ Q2 ≤ 0.24 GeV2 (original) (raw)

Spin-isospin correlations in nuclear force and QCD sum rules

Nuclear Physics A, 1994

The Ok,unolo-Noletl bclnffel ,momal 5, t e the f,nlme iheot~ to t xplatu the cliff( route of masses of nmtot nuclei [1] t)lo~ldes lhe ~ell kno~n ch,dleuge lo traditional nu(le,n phx',J(~,, )wldmg the bmld up of l'-,o',,plll brt,lkmg folco,, tier( we qho",~ I/ov'~ ¢ellalll featm e~, ot su(h loiter, ( an I)e obialned 110111 Q('I) sum t Ii1(", ,real 3 ~e', Thv, ploblem is (m15 a ',ingle example of lhe b~ oad t la,,s of l)t oblem', allsmg m ms esl ~gallon of lh( nu~ leon pl,wed rote the mallet lot xxhwh the appma(h is needed 0375-9474/94/$07 00 © 1994 -Elsevmr Science B V All nghts reserved SSDI 0375-9474(94)00399-8

Effect of symmetry breaking of polarized light sea quarks on the nucleon and nuclear structure functions, and sum rules

Phys. Rev. C 108, 035203, 2023

In this study, we performed calculations and analyses of the structure functions of polarized nucleons and light nuclei, specifically 3 He and 3 H, using second-order Feynman diagrams. Our investigation focused on two main aspects: First, we examined the symmetry properties of polarized light sea quarks. Second, we conducted a detailed investigation into the impacts of symmetry breaking on the structure functions of both nucleons and nuclei. To achieve this, we utilized the existing polarized parton distribution functions (polarized PDFs) available in the literature. These PDFs were used to calculate and compare the polarized structure functions g 1 and g 2 of the nuclei. Additionally, we examined and analyzed the Bjorken and Efremov-Leader-Teryaev sum rules by utilizing the moments of the polarized structure functions. The Lorentz color force components, namely F y,n E and F y,n B , were determined using the twist-2, twist-3, and twist-4 matrix elements. When symmetry breaking is applied, it is observed that they have similar magnitudes but opposite signs. Our theoretical predictions for the polarized structure functions of nucleons and light nuclei, taking into account the symmetry breaking of light sea quarks, exhibit better agreement with experimental data.

Measurements of the Q2-dependence of the proton and neutron spin structure functions g1p and g1n

2000

HAL is a multidisciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L'archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d'enseignement et de recherche français ou étrangers, des laboratoires publics ou privés. Measurements of the Q 2 dependence of the proton and neutron spin structure functions g p _1 and g n _1

The nucleon axial isoscalar coupling in quantum chromodynamics sum rules

Physics Letters B, 1994

The correction arising from the three-gluon condensate to the QCD sum rules of the nucleon coupling constant to the axial isoscalar current, g~t, is calculated. It is found that the contribution of the three-gluon condensate can make the sum rules more stable. The resultant theoretical value, g] = 0.58 + 0.20, agrees with the phenomenological estimate. The first moments of the spin structure functions for proton, neutron and deuteron are found to be consistent with the improved Ellis-Jaffe sum rules.

The effect of light sea quark symmetry breaking on polarized nucleus and sum rules

PoS(ICHEP2022)1170 , 2022

The polarized structure functions of 3𝐻𝑒 and 3𝐻 nuclei are calculated in NLO approximation, considering and disregarding the light sea quark symmetry breaking. We employ the polarized structure function of the nucleons within the nucleus extracted from our two recent analysis on polarized DIS data and on polarized DIS+SIDIS data. Since the data of the second analysis cover a bigger range of Bjorken variable, both SU(2) and SU(3) symmetry breaking is considered within the analysis. Then we calculate and compare the polarized structures of nuclei extracted from both scenarios. Also the Bjorken and ELT sum rules are calculated using the moments of structure functions. The results are compared with experimental data and the differences are investigated.

Erratum to: “Nucleon polarizabilities from low-energy Compton scattering” [Phys. Lett. B 567 (2003) 200]

Physics Letters B, 2005

An effective field theory is used to give a model-independent description of Compton scattering at energies comparable to the pion mass. The amplitudes for scattering on the proton and the deuteron, calculated to fourth order in small momenta in chiral perturbation theory, contain four undetermined parameters that are in one-to-one correspondence with the nucleon polarizabilities. These polarizabilities are extracted from fits to data on elastic photon scattering on hydrogen and deuterium. For the proton we find: α p = (12.1 ± 1.1 (stat.)) +0.5 −0.5 (theory) and β p = (3.4 ± 1.1 (stat.)) +0.1 −0.1 (theory), both in units of 10 −4 fm 3. For the isoscalar polarizabilities we obtain: α N = (13.0 ± 1.9 (stat.)) +3.9 −1.5 (theory) (in the same units) while β N is consistent with zero within sizable error bars. Electromagnetic polarizabilities are a fundamental property of any composite object. For example, atomic polarizabilities contain information about the charge and current distributions that result from the interactions of the protons, neutrons, and electrons inside the atom. Protons and neutrons are, in turn, complex objects composed of quarks and gluons, with interactions governed by QCD. It has long been hoped that neutron and proton polarizabilities will give important information about the strong-interaction dynamics of QCD. For example, in a simple quark-model picture these polarizabilities contain averaged information about the charge and current distribution produced by the quarks inside the

Novel Corrections to the Momentum Sum Rule for Nuclear Structure Functions

2021

We address novel features of deep inelastic lepton scattering on nuclei at small Bjorken variable xB j. In this regime the lepton-nuclear cross section involves the interference between the standard lepton-quark scattering amplitude for the deep inelastic scattering (DIS) process on a single nucleon and a two-step process where diffractive scattering on a first nucleon combines with the amplitude for DIS on a second nucleon. The phases associated with the t-channel exchanges to the diffractive amplitude can produce either a destructive or constructive quantum-mechanical interference of the one-step and two-step amplitudes. This provides a mechanism regulating the respective amounts of shadowing suppression and anti-shadowing enhancement at low xB j. Furthermore, the standard leading-twist operator product and handbag diagram analyses of the forward virtual Compton amplitude on the nucleus are inapplicable, barring a conventional probabilistic interpretation. A main observable conseq...