6533b86ffe1ef96bd12ce75f

RESEARCH PRODUCT

The spin-dependent structure function g1(x) of the deuteron from polarized deep-inelastic muon scattering

S. BültmannS. BültmannT. KageyaM. BoutemeurM. BoutemeurD. FaschingD. FaschingT. PussieuxA. BressanA. BressanJ. E.j. OberskiE. M. KabußE. BurtinT. MatsudaT. MatsudaD.v. PeshekhonovK. M. TeichertI. SaboJay RobertsI.a. SavinV. G. KrivokhijineJ. NassalskiJ. ZhaoN. De BottonVictor KukhtinA. BravarB. W. MayesE. ArikR. SeitzR. SeitzG. GratiaW. TlaczalaJ. CranshawH. J. KesslerRoland WindmoldersM. LoweM. LoweA. ArvidsonJ. MartinoA. GallasA. NagaitsevG. K. MallotM. LamannaY. YlöstaloDavid MillerAina YañezG. BardinDrew ParksL. NaumannG. UnelT. O. NiinikoskiJ. LichtenstadtJ. LichtenstadtJ. KyynäräinenJ. KyynäräinenJ. KyynäräinenF. TessarottoW. KrögerW. KrögerH. PostmaJ. KirylukJ. SaboridoM. LitmaathM. LitmaathL. S. PinskyP. SchiavonN. HorikawaB. DerroD. Von HarrachM. K. BallintijnD. KrämerAbhay DeshpandeF. SeverF. SeverR. PuntaferroK. P. SchülerE. RondioJ. H. MoromisatoSatish DhawanG. BaumF. FeinsteinT. IwataYannis K. SemertzidisYannis K. SemertzidisJ. PyrlikMayda VelascoMayda VelascoL. BetevS. EichblattS. EichblattA. WitzmannA. WitzmannPatrick HautlePatrick HautleP. BjörkholmP. BjörkholmT. HasegawaT. HasegawaS. Dalla TorreJ. C. FaivreL. KlostermannL. KlostermannJ. M. Le GoffF. MarieJ. S. MccarthyC. CavataRegine WillumeitMatias RodriguezMatias RodriguezC. DulyaC. DulyaG. Van MiddelkoopA. OgawaP. BerglundB. FroisS. PlatchkovRoy WeinsteinN. De GrootN. De GrootJ. VogtE. Von GoelerP. ShanahanP. ShanahanA. KishiA. RosadoG. RädelG. IgoS. RockS. RockT. GaussiranL. V. KalinovskayaClemens A. HeuschClemens A. HeuschF. SimeoniG.i. SmirnovRicardo PiegaiaRicardo PiegaiaT. ÇUhadarA. De LesquenJ. PretzJ. A. GarzonJ. A. GarzonFranco BradamanteFranco BradamanteD. Y. BardinM. GiorgiJ. PolecB. BadelekC. FernandezC. FernandezR. BirsaN. HayashiA. SandaczF. Perrot-kunneC.s. OzbenS. TrentalangeD. G. CrabbYu. KisselevW. WislickiA. SteinmetzT. LindqvistD. L. AdamsT. AkdoganD. PoseA. RijllartBernardo AdevaA. DyringHeinrich B. StuhrmannA. StaudeT. J. KetelV. W. HughesUlrich LandgrafA. KarevF. LeharA. MagnonA. TripetA. TripetA. TripetB. E. BonnerM. Grosse-perdekampM. Grosse-perdekampRudiger VossMichal SzleperS. IshimotoR. Van DantzigI. G. BirdE. P. SichtermannK. ZarembaM. PloU. StieglerFaustino GómezKunikazu MoriK. MedvedAnna ZanettiK. KurekC. A. WhittenAnne-laure Martin

subject

PhysicsDISNuclear and High Energy PhysicsStrange quarkMuonSMCScatteringg1 structure functionSMC; DIS; g1 structure functionPerturbative QCDDeep inelastic scatteringNuclear physicsHigh Energy Physics::ExperimentSum rule in quantum mechanicsNucleonParticle Physics - ExperimentSpin-½

description

We present a new measurement of the spin-dependent structure function $g_{1}^{\rm d}$ of the deuteron from deep inelastic scattering of 190 GeV polarized muons on polarized deuterons. The results are combined with our previous measurements of $g_{1}^{\rm d}$. A perturbative QCD evolution in next-to-leading order is used to compute $g_{1}^{\rm d}(x)$ at a constant $Q^{2}$. At $Q^{2} = 10$ GeV$^{2}$, we obtain a first moment $\Gamma_{1}^{\rm d} = \int_{0}^{1} g_{1}^{\rm d}{\rm d}x = 0.041 \pm 0.008$, a flavour-singlet axial charge of the nucleon $a_{0} = 0.30 \pm 0.08$, and an axial charge of the strange quark $a_{s} = -0.09 \pm 0.03$. Using our earlier determination of $\Gamma_{1}^{\rm p}$, we obtain $\Gamma_1^{\rm p} - \Gamma_1^{\rm n} = 0.183 \pm 0.035$ at $Q^2 = 10\,\mbox{GeV}^2$. This result is in agreement with the Bjorken sum rule which predicts $\Gamma_1^{\rm p} - \Gamma_1^{\rm n} = 0.186 \pm 0.002$ at the same $Q^2$.

https://doi.org/10.1016/s0370-2693(97)00159-7