cs.LGJul 15, 2026

Mono-Z Dark Matter Search with Neural Spline Flows Using CMS Run 2015D Open Data

Authors: Hitesh RasineniBhavishya Chebrolu

Organizations: VIT-AP University, Amaravati, India · 1VIT-AP University, Amaravati, 522241, India · Mohan Babu University, Tirupati, India · 2Mohan Babu University, Tirupati, 517102, India

Abstract

We report a search for dark matter (DM) produced in association with a leptonically decaying ZZ boson at s=13\sqrt{s}=13 TeV using CMS Run 2015D open data corresponding to an integrated luminosity of 2.32fb12.32\,\mathrm{fb}^{-1} together with simplified-model Monte Carlo simulation. Events are selected in the mono-Z+Z\rightarrow\ell^+\ell^- final state in both the μμμμ and eeee channels. Forty kinematic observables are extracted from MINIAOD and MINIAODSIM, cleaned with physics-motivated selections, and reduced to a 37-dimensional feature vector. Five Neural Spline Flows are trained independently to model Standard Model background and mediator-specific DM signal densities. The per-event test statistic is constructed from the log-likelihood ratio between the signal and background density estimates, providing sensitivity across the full kinematic phase space without requiring a hard upper MET\mathrm{MET} threshold. A simultaneous profile-likelihood fit combining the two channels yields observed (expected) 95% confidence level upper limits on the signal-strength parameter of μ<0.0177μ<0.0177 (0.00180.0018) for the scalar mediator, μ<0.0362μ<0.0362 (0.00390.0039) for the vector mediator, and μ<0.0498μ<0.0498 (0.00690.0069) for the axial-vector mediator. The observed limits are weaker than expected because of a residual high-MET\mathrm{MET} background-modeling discrepancy rather than evidence for a DM signal. To our knowledge, this is the first application of Neural Spline Flow likelihood-ratio scoring to a mono-ZZ dark matter search using CMS Run 2015D open data simultaneously in the μμμμ and eeee channels.

Explore similar work

Jul 9, 2026hep-ph

Revisiting One-Zero and Two-Zero Neutrino Mass Textures in Light of Recent Oscillation and Cosmological Data

We revisit one-zero and two-zero textures of the neutrino mass matrix under current experimental and cosmological constraints. We identify the phenomenologically viable texture structures using the latest results on neutrino oscillation parameters, the cosmological bound on the sum of neutrino masses, the kinematic bound on the effective electron-neutrino mass, and limits from neutrinoless double-beta decay. For two-zero textures, several structures are still allowed if only the CMB bound on the neutrino mass sum is imposed. Among them, the BB-series textures show a characteristic prediction for the Dirac CP phase, with δCPδ_{\rm CP} lying around π/2π/2 and 3π/23π/2, and are within the reach of future neutrinoless double-beta decay searches. When the stronger CMB+BAO constraint is included, however, only the AA-series textures remain viable. Therefore, we also analyze one-zero textures by using machine learning techniques, particularly flow matching. It turns out that some of the texture structures are already excluded by current data, while the allowed ones give distinct predictions for imi\sum_i m_i, mνeeffm_{ν_e}^{\rm eff}, mee\langle m_{ee}\rangle, and δCPδ_{\rm CP}. We further discuss how the one-zero texture structures can arise from non-invertible selection rules.
Haruto Kitagawa, Coh Miyao, Satsuki Nishimura +1
May 18, 2026hep-ph

Probing SMEFT Operators through t\bar{t}t\bar{t} Production with Hyper-Graph Neural Networks at the LHC

We present a phenomenological study of ttˉttˉt\bar{t}t\bar{t} production in proton-proton collisions at s=13\sqrt{s} = 13~TeV, using a Hyper-Graph Neural Network (H-GNN) to discriminate multilepton signal events from the dominant SM backgrounds, namely ttˉWt\bar{t}W, ttˉZt\bar{t}Z, ttˉHt\bar{t}H, ttˉVVt\bar{t}VV, single-top associated production, and diboson and triboson processes. In the H-GNN architecture each event is represented as a hypergraph whose nodes correspond to reconstructed jets and leptons and whose hyperedges encode higher-order correlations among arbitrary subsets of these objects, allowing the network to learn the many-body kinematic structures that characterize the ttˉttˉt\bar{t}t\bar{t} final state. Combining same-sign di-lepton, tri-lepton, and four-lepton channels following a CMS-like event selection, the H-GNN attains an area under the ROC curve of 0.9510.951 for the ttˉttˉt\bar{t}t\bar{t} signal and yields a statistical significance of Z=9.11Z = 9.11 at an integrated luminosity of L=140 fb1\mathcal{L} = 140~\mathrm{fb}^{-1}, to be compared with Z=8.62Z = 8.62 for a SPANet baseline, Z=7.37Z = 7.37 for a Particle Transformer baseline, and Z=5.13Z = 5.13 obtained by the ATLAS analysis, evaluated under identical event selection. We exploit the improved signal extraction to derive one- and two-parameter 95%95\% confidence level limits on the Wilson coefficients of the dimension-six operators OΦu\mathcal{O}_{Φu}, Ott(1)\mathcal{O}^{(1)}_{tt}, Oqq(1)\mathcal{O}^{(1)}_{qq}, Oqt(1)\mathcal{O}^{(1)}_{qt}, and Oqt(8)\mathcal{O}^{(8)}_{qt}, and we project the expected sensitivity at the HL-LHC integrated luminosities of 1000 fb11000~\mathrm{fb}^{-1} and 3000 fb13000~\mathrm{fb}^{-1} with 50%50\% uncertainty on the background estimation.
Amir Subba, Sanmay Ganguly
Sep 9, 2026hep-ph

Searching for New Physics with Reinforcement Learning

Finding new physics (NP) is the most important problem in particle physics today. Studying ``anomalies'', i.e., measurements of low-energy observables whose values disagree with the predictions of the Standard Model (SM), is a powerful search strategy. The SM Effective Field Theory (SMEFT) provides a general model-independent framework for parameterizing NP; it is natural to try to find the SMEFT operator(s) that can explain such anomalies. This is a challenging task because (i) the number of SMEFT operators is enormous, and (ii) at loop level there are very complicated correlations among the operators. Analyses by humans typically rely on phenomenological intuition to decide which operators are relevant. This is often biased and does not explore the complete SMEFT operator space. Interestingly, reinforcement learning (RL) techniques excel at tasks that require decision making to achieve their goals. In this paper, we introduce an RL method that can be used to find the SMEFT operators that explain any anomalies. We test it on the CDF WW-mass anomaly, and show that it reproduces (and improves upon) known results. We then consider a far more complicated situation with multiple anomalies and show that, even here, this method is able to find the SMEFT operators that explain the data. Our RL method can therefore be used to efficiently search for NP at the level of SMEFT.
Jacky Kumar, Marianne Bouchard, David London