12–16 Dec 2022
IISER Mohali
Asia/Kolkata timezone

Antineutrino-A DIS cross sections for ⟨𝐸𝜈⟩∼6𝐺𝑒𝑉 at MINER𝜈A

15 Dec 2022, 16:15
15m
LH3 (IISER Mohali)

LH3

IISER Mohali

Lecture Hall Complex, IISER Mohali, Sector 81, Knowledge city, SAS Nagar, Punjab, India

Speaker

Ms Vaniya Ansari (Aligarh Muslim University)

Description

For better understanding of neutrino properties, we require precision measurements of the oscillation parameters. Presently the systematic uncertainties in these parameters are large, to which 20-25\% arises due to the lack in the understanding of $\nu/\bar \nu$-N and $\nu/\bar \nu$-A cross sections. Future high precision measurements require the systematic uncertainties to be reduced to 2-3\% level. Theoretical as well experimental works are being performed worldwide. In the few GeV energy region, MINER$\nu$A is the best experimental effort in this direction. MINER$\nu$A uses fine-grained tracking detector commissioned for recording (anti)neutrino interactions produced by the NuMI beamline at the Fermilab. MINER$\nu$A is dedicated to extract $\nu/\bar \nu$-A cross sections on a variety of nuclear targets ($C$, $H_2O,~He,~Fe,~Pb$ and $CH$) and study nuclear medium effects by obtaining the cross section ratios. MINER$\nu$A ran in two modes, low energy ($\langle E_\nu\rangle \sim 3.5GeV$) and medium energy ($\langle E_\nu\rangle \sim 6GeV$).

In this symposium we shall present the preliminary results for charged current antineutrino deep inelastic scattering (DIS) [$\bar \nu_\mu + N(bound~inside~nuclear~target) \to \mu^+ + X(jet~of~hadrons)$] cross sections in the medium energy mode of MINER$\nu$A. The events observed are restricted to the region of 2$\leq E_{\bar \nu_\mu}\leq $50 GeV, 2 $\leq E_{\mu} \leq$ 50GeV and muon scattering angle $\theta_\mu<17^o$ with respect to the beam. Moreover, this DIS analysis employs cuts on the center of mass energy of hadronic system $W>2GeV$ and four momentum transfer squared $Q^2>1~GeV^2$. We shall discuss various techniques used in the cross section extraction at MINER$\nu$A for passive as well as active targets. The results of $\frac{\sigma^A}{E_{\bar \nu}}$ vs $E_{\bar \nu_\mu}$ and $\frac{d \sigma^A}{dx_{Bj}}$ vs $x_{Bj}$ (fraction of the momentum carried by the struct parton) for $A = Fe,~Pb,~C,~CH$ shall be presented. The ultimate aim of this study is to extract the cross section ratio of $C$, $Fe$ and $Pb$ to $CH$. This will be the first direct measurement of nuclear effects in DIS with antineutrinos.

Session Neutrino Physics

Author

Ms Vaniya Ansari (Aligarh Muslim University)

Presentation materials