thesis

Precision measurement of the mass difference between light nuclei and anti-nuclei with the ALICE experiment at the LHC

Abstract

Con questo lavoro è stata effettuata una misura della differenza Δμ=Δ(m/z)\Delta \mu = \Delta (m / |z|) fra il rapporto massa su carica del deutone (d) e dell'anti-deutone (d{\rm \overline{d}}), e del nucleo di 3He{\rm ^{3}He} e di anti-3He{\rm ^{3}He} con l'esperimento ALICE ad LHC in collisioni Pb--Pb a un'energia nel centro di massa per coppia di nucleoni sNN=2.76 TeV\sqrt{s_{\rm NN}}=2.76~{\rm TeV}. Le misure sono pari a Δμddˉ/μd=[0.9±0.5(stat.)±1.4(syst.)]×104{\Delta \mu}_{\rm{d\bar{d}}}/{\mu}_{\rm{d}} = [0.9 \pm 0.5 (\rm{stat.}) \pm 1.4 (\rm{syst.})] \times 10^{-4} e Δμ3He3He/μ3He=[1.2±0.9(stat.)±1.0(syst.)]×103{\Delta \mu}_{\rm{^{3}He ^{3}\overline{He}}}/{\mu}_{\rm{^{3}He}} = [-1.2 \pm 0.9 (\rm{stat.}) \pm 1.0 (\rm{syst.})] \times 10^{-3}. Combinando questi risultati con le misure esistenti delle masse dei (anti-)nucleoni, sono state estratte le corrispondenti differenze di energia di legame Δεddˉ/εd=0.04±0.05(stat.)±0.12(syst.){\Delta \varepsilon}_{\rm{d\bar{d}}}/{\varepsilon}_{\rm{d}} = -0.04 \pm 0.05(\rm{stat.}) \pm 0.12(\rm{syst.}) e Δε3He3He/ε3He=0.24±0.16(stat.)±0.18(syst.){\Delta \varepsilon}_{\rm{^{3}He ^{3}\overline{He}}}/{\varepsilon}_{\rm{^{3}He}} = 0.24 \pm 0.16(\rm{stat.}) \pm 0.18(\rm{syst.}). I risultati verificano, con una precisione senza precedenti, l'invarianza CPT nel settore dei nuclei leggeri.With this work a measurement of the difference Δμ=Δ(m/z)\Delta \mu = \Delta (m / |z|) between the mass-over-charge ratio of deuteron (d) and anti-deuteron (d{\rm \overline{d}}), and 3He{\rm ^{3}He} and 3He{\rm ^{3}\overline{He}} nuclei, carried out with the ALICE experiment in Pb--Pb collisions at a centre-of-mass energy per nucleon pair sNN= 2.76 TeV\sqrt{s_{\rm NN}}=~2.76~\rm{TeV} has been performed. The measurement yields Δμddˉ/μd=[0.9±0.5(stat.)±1.4(syst.)]×104{\Delta \mu}_{\rm{d\bar{d}}}/{\mu}_{\rm{d}} = [0.9 \pm 0.5 (\rm{stat.}) \pm 1.4 (\rm{syst.})] \times 10^{-4} and Δμ3He3He/μ3He=[1.2±0.9(stat.)±1.0(syst.)]×103{\Delta \mu}_{\rm{^{3}He ^{3}\overline{He}}}/{\mu}_{\rm{^{3}He}} = [-1.2 \pm 0.9 (\rm{stat.}) \pm 1.0 (\rm{syst.})] \times 10^{-3}. Combining these results with existing measurements of the masses of the (anti-)nucleons, the relative binding energy differences are extracted, Δεddˉ/εd=0.04±0.05(stat.)±0.12(syst.){\Delta \varepsilon}_{\rm{d\bar{d}}}/{\varepsilon}_{\rm{d}} = -0.04 \pm 0.05(\rm{stat.}) \pm 0.12(\rm{syst.}) and Δε3He3He/ε3He=0.24±0.16(stat.)±0.18(syst.){\Delta \varepsilon}_{\rm{^{3}He ^{3}\overline{He}}}/{\varepsilon}_{\rm{^{3}He}} = 0.24 \pm 0.16(\rm{stat.}) \pm 0.18(\rm{syst.}). These results test, to an unprecedented precision, the CPT invariance in the sector of light nuclei

    Similar works