High Energy Physics - Phenomenology · arXiv:hep-ph/9608472 v1 · submitted 28 Aug 1996
Higher Order Top Squark Decays
The paper says
“We discuss our numerical results in view of the upgraded Tevatron, the LHC and a 500 GeV e+e− Linear Collider.”
from the abstract · picked out as the main claim by a classifier
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The paper
Abstract
Within the Minimal Supersymmetric Standard Model we study the three body decay of the lighter top squark into a b-quark, a W-boson and the lightest neutralino and compare this decay with the flavour changing two body decay of the lighter top squark into a c-quark and the lightest neutralino. We do this for scenarios where two body decays at tree level are forbidden for the light top squark. We give the complete analysis for the three body and compare it with the mentioned two body decay. We discuss our numerical results in view of the upgraded Tevatron, the LHC and a 500 GeV e+e− Linear Collider.
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abstract compiled · 2026-09-23 · no language-model review
How the main claim is stated: asserted 0.58
What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.41 · human participants 0.01 · controlled comparison 0.42 · randomized assignment 0.01 · states quantitative result 0.06 · compares with prior results 0.75 · 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.
| Sentence | Role | The authors' own work | States the main conclusion | Strength |
|---|---|---|---|---|
| Within the Minimal Supersymmetric Standard Model we study the three body decay of the lighter top squark into a b-quark, a W-boson and the lightest neutralino and compare this decay with the flavour changing two body decay of the lighter top squark into a c-quark and the lightest neutralino. | contribution 1.00 | 0.92 | 0.11 | asserted 0.95 |
| We do this for scenarios where two body decays at tree level are forbidden for the light top squark. | method 0.56 | 0.44 | 0.03 | asserted 0.77 |
| We give the complete analysis for the three body and compare it with the mentioned two body decay. | contribution 0.90 | 0.93 | 0.07 | asserted 0.95 |
| We discuss our numerical results in view of the upgraded Tevatron, the LHC and a 500~GeV $e^+ e^-$ Linear Collider. | interpretation 0.86 | 0.68 | 0.06 | asserted 0.58 |
What kind of paper the classifier reports this is: theoretical result 0.71 · evidence from simulation or computation 0.91
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, 3,670 input tokens, $0.0002 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 3 Pith papers
Reviewed papers on Pith that cite this one. The full citation record
- Dark matter in composite Higgs models with a scotogenic EFT hep-ph · Jul 2026
- Light Stop Decay in the MSSM with Minimal Flavour Violation hep-ph · Feb 2011
- Diphoton decays of stoponium at the Large Hadron Collider hep-ph · Dec 2007
How the literature uses it
10 arXiv papers cite this in 11 sentences
Papers citing it · 8 sentences without a confident label
Builds on it 1 paper
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We extend and refine former analyses [ref] by including the recently computed SUSY-QCD corrections to the FV two-body decay [ref] [See also [ref] .] and the FV tree-level couplings in the three-body decay as well as in the four-body decay where also a non-vanishing $τ$ and bottom mass in the final state [ref] are taken into account.
Light stop decays into $W b \tilde{\chi}_1^0$ near the kinematic threshold · Introduction · 0.98
Cites it as background 1 paper
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In the few cases in which these channels are closed, the squarks will decay through flavour changing neutral channels [ref] , or through three- or four-body decay channels involving a non-resonant SUSY particle [ref] .
Effective squark/chargino/neutralino couplings: MadGraph implementation · Introduction · 0.82
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