6533b861fe1ef96bd12c5824

RESEARCH PRODUCT

Measurement of the Charged-Pion Polarizability

C. AdolphR. AkhunzyanovM. C. AlexeevC. D. AlexeevA. AmorosoV. V. AndrieuxV. AnosovA. AustregesiloB. BadelekF. BalestraJ. BarthG. BaumR. BeckY. BedferA. BerlinJ. BernhardK. BickerJ. BielingR. BirsaJ. BisplinghoffM. BodlakM. BoerP. BordaloF. BradamanteC. BraunA. BressanM. BuecheleE. BurtinL. CapozzaM. ChiossoS. U. ChungA. CicuttinM. ColantoniM. L. CrespoQ. CurieS. Dalla TorreS. S. DasguptaS. DasguptaO. Yu DenisovA. M. DinkelbachS. V. DonskovN. DoshitaV. DuicW. DuennweberM. DziewieckiA. EfremovC. EliaP. D. EversheimW. EyrichM. FaesslerA. FerreroA. FilinM. FingerM. FingerH. FischerC. FrancoN. Du Fresne HohenescheJ. M. FriedrichV. FrolovF. GautheronO. P. GavrichtchoukS. GerassimovR. GeyerI. GnesiB. GobboS. GoertzM. GorzellikS. GrahmuellerA. GrassoB. GrubeT. GrussenmeyerA. GuskovT. GuthoerlF. HaasD. HarrachD. HahneR. HashimotoF. H. HeinsiusF. HerrmannF. HinterbergerCh HoeppnerN. HorikawaN. D HoseS. HuberS. IshimotoA. IvanovYu IvanshinT. IwataR. JahnV. JaryP. JasinskiP. JoergR. JoostenE. KabussB. KetzerG. V. KhaustovYu A. KhokhlovYu KisselevF. KleinK. KlimasewskiJ. H. KoivuniemiV. N. KolosovK. KondoK. KoenigsmannI. KonorovV. F. KonstantinovA. M. KotzinianO. KouznetsovM. KraemerZ. V. KroumchteinN. KuchinskiR. KuhnF. KunneK. KurekR. P. KurjataA. A. LednevA. LehmannM. LevillainS. LevoratoJ. LichtenstadtA. MaggioraA. MagnonN. MakkeG. K. MallotC. MarchandA. MartinJ. MarzecJ. MatousekH. MatsudaT. MatsudaG. MeschcheryakovW. MeyerT. MichigamiYu V. MikhailovY. MiyachiM. A. MoinesterA. NagaytsevT. NagelF. NerlingS. NeubertD. NeyretV. I. NikolaenkoJ. NovyW. -D NowakA. S. NunesA. G. OlshevskyI. OrlovM. OstrickR. PankninD. PanzieriB. ParsamyanS. PaulD. PeshekhonovS. PlatchkovJ. PochodzallaV. A. PolyakovJ. PretzM. QuaresmaC. QuintansS. RamosC. RegaliC. ReicherzE. RoccoN. S. RossiyskayaD. I. RyabchikovA. RychterV. D. SamoylenkoA. SandaczS. SarkarI. A. SavinG. ShrizzaiP. SchiavonC. SchillT. SchlueterK. SchmidtH. SchmiedenK. SchoenningS. SchopfererM. SchottO. Yu ShevchenkoL. SilvaL. SinhaS. SirtlM. SluneckaS. SosioF. SozziAleš SrnkaL. SteigerM. StolarskiM. SulcR. SulejH. SuzukiA. SzabelskiT. SzameitatP. SznajderS. TakekawaJ. Ter WolbeekS. TessaroF. TessarottoF. ThihaudS. UhlI. UmanM. ViriusL. WangT. WeisrockM. WilfertR. WindmoldersH. WollnyK. ZarembaM. ZavertyaevE. ZemlyanichkinaM. ZiembickiA. ZinkCollaboration Compass

subject

Particle physicsChiral perturbation theoryPhotonComputerSystemsOrganization_COMPUTERSYSTEMIMPLEMENTATIONStrong interactionComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONGeneral Physics and AstronomyFOS: Physical sciencesComputerApplications_COMPUTERSINOTHERSYSTEMSGeneralLiterature_MISCELLANEOUSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)PionPolarizabilityNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentPhysicsChPTMuonCompton scatteringpolarisabilitypolarisability; ChPTComputingMethodologies_PATTERNRECOGNITIONHigh Energy Physics::ExperimentMagnetic dipoleParticle Physics - Experiment

description

The COMPASS collaboration at CERN has investigated pion Compton scattering, $\pi^-\gamma\rightarrow \pi^-\gamma$, at centre-of-mass energy below 3.5 pion masses. The process is embedded in the reaction $\pi^-\mathrm{Ni}\rightarrow\pi^-\gamma\;\mathrm{Ni}$, which is initiated by 190\,GeV pions impinging on a nickel target. The exchange of quasi-real photons is selected by isolating the sharp Coulomb peak observed at smallest momentum transfers, $Q^2<0.0015$\,(GeV/$c$)$^2$. From a sample of 63\,000 events the pion electric polarisability is determined to be $\alpha_\pi\ =\ (\,2.0\ \pm\ 0.6_{\mbox{\scriptsize stat}}\ \pm\ 0.7_{\mbox{\scriptsize syst}}\,) \times 10^{-4}\,\mbox{fm}^3$ under the assumption $\alpha_\pi=-\beta_\pi$, which relates the electric and magnetic dipole polarisabilities. It is the most precise measurement of this fundamental low-energy parameter of strong interaction, that has been addressed since long by various methods with conflicting outcomes. While this result is in tension with previous dedicated measurements, it is found in agreement with the expectation from chiral perturbation theory. An additional measurement replacing pions by muons, for which the cross-section behavior is unambigiously known, was performed for an independent estimate of the systematic uncertainty.

10.1103/physrevlett.114.062002http://cds.cern.ch/record/1702252