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High Energy Physics - Phenomenology · arXiv:hep-ph/9310209 v1 · submitted 1 Oct 1993

A new signal for scalar top bound state production

M. Drees, M.M. Nojiri

The paper says

“Nevertheless the branching ratio into two photons is often large enough to yield a detectable signal.”

from the abstract · picked out as the main claim by a classifier

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The paper

Abstract

We study the production and decay of a scalar \stst\ bound state \sigst\ at hadron supercolliders, where \st\ is the lighter stop eigenstate. If \st\ has no tree–level 2–body decays, the dominant decay modes of \sigst\ are gg or, if $m_h < \mst \ll \mstt$, a pair of light scalar Higgs bosons h. Nevertheless the branching ratio into two photons is often large enough to yield a detectable signal.

The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. No sentence in this record was written by a model.

abstract compiled · 2026-09-23 · no language-model review

How the main claim is stated: hedged possibility 0.51

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.33 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.10 · compares with prior results 0.06 · mentions code or data availability 0.02

The abstract, sentence by sentence

This table labels the abstract only (arXiv listing abstract v1). The number is the probability the classifier gave the label.

SentenceRoleThe authors' own workStates the main conclusionStrength
We study the production and decay of a scalar \stst\ bound state \sigst\ at hadron supercolliders, where \st\ is the lighter stop eigenstate. contribution 1.00 0.78 0.08 asserted 0.90
If \st\ has no tree--level 2--body decays, the dominant decay modes of \sigst\ are $gg$ or, if $m_h < \mst \ll \mstt$, a pair of light scalar Higgs bosons $h$. result 0.94 0.34 0.15 asserted 0.83
Nevertheless the branching ratio into two photons is often large enough to yield a detectable signal. result 0.82 0.61 0.43 hedged possibility 0.51

What kind of paper the classifier reports this is: theoretical result 0.98 · evidence from argument 0.47

What was examined, and what was not

Sources read

  • arXiv listing abstract v1

Not examined

  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers

Levels run

  • P abstract

Not run

  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

How the labels were made

Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 2,994 input tokens, $0.0001 reported.

Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. This record as JSON

Cited by 5 Pith papers
How the literature uses it

9 arXiv papers cite this in 9 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 5 sentences without a confident label

Contests it 1 paper
Builds on it 1 paper
  • In [ref] we computed the bound state annihilation signals, at leading order and in the Coulomb approximation, for a variety of particles.[For other studies of bound state phenomenology at the LHC, see [ref] .] Here we update our work to include the results of the 8 TeV and the early 13 TeV searches by ATLAS and CMS.

    Resonances from QCD bound states and the 750 GeV diphoton excess · Introduction · 0.98

Cites it as background 2 papers
  • A resonant $γγ$ signal can also arise within the MSSM from the annihilation of a squark-antisquark near-threshold QCD bound state, most famously the stoponium [ref] .

    Interpreting a 750 GeV Diphoton Resonance · The fate of the MSSM · 0.82

  • We will now analyze to what extent the bound state signals discussed in the previous sections will be detectable at the LHC.[LHC signals of gluinonium have been also studied in [ref] and squarkonium in [ref] .] To that end, it is informative to consider the existing experimental constraints on the masses of the various UED and MSSM particles.

    Distinguishing spins at the LHC using bound state signals · Detection prospects · 0.95

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