High Energy Physics - Phenomenology · arXiv:1307.5064 v1 · submitted 18 Jul 2013
Confronting the Fermi Line with LHC data: an Effective Theory of Dark Matter Interaction with Photons
The paper says
“We reinterpret an ATLAS $\gamma+\missET$ analysis and the observed Fermi feature in the parameter space of our new effective theory to assess their consistency.”
from the abstract · picked out as the main claim by a classifier
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The paper
Abstract
We describe an effective theory of interaction between pairs of dark matter particles and pairs of photons. Such an interaction could accomodate χχ̄ → γγ processes which might be the cause of the observed feature in the FermiLAT spectrum, as well as γ*/Z → γχχ̄ processes, which would predict excesses at the LHC in the $\gamma+\missET$ final-state. We reinterpret an ATLAS $\gamma+\missET$ analysis and the observed Fermi feature in the parameter space of our new effective theory to assess their consistency.
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: asserted 0.61
What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.11 · human participants 0.02 · controlled comparison 0.05 · randomized assignment 0.01 · states quantitative result 0.06 · compares with prior results 0.56 · 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 |
|---|---|---|---|---|
| We describe an effective theory of interaction between pairs of dark matter particles and pairs of photons. | contribution 0.94 | 0.86 | 0.04 | asserted 0.97 |
| Such an interaction could accomodate $\chi\bar{\chi}\rightarrow\gamma\gamma$ processes which might be the cause of the observed feature in the FermiLAT spectrum, as well as $\gamma^*/Z\rightarrow \gamma\chi\bar{\chi}$ processes, which would predict excesses at the LHC in the $\gamma+\missET$ final-state. | background 0.52 | 0.10 | 0.09 | hedged possibility 0.87 |
| We reinterpret an ATLAS $\gamma+\missET$ analysis and the observed Fermi feature in the parameter space of our new effective theory to assess their consistency. | contribution 0.66 | 0.93 | 0.15 | asserted 0.61 |
What kind of paper the classifier reports this is: theoretical result 0.98 · evidence from analysis of existing data 1.00
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, 3,064 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 10 Pith papers
Reviewed papers on Pith that cite this one. The full citation record
- Probing the Axion--Photon--Dark Photon Interaction with LHC Mono-Photons and Fermi-LAT Gamma-Ray Lines hep-ph · Oct 2026
- Neutrino non-standard interactions meet precision measurements of $N_{\rm eff}$ hep-ph · Jan 2021
- Non-standard neutrino interactions and low energy experiments hep-ph · Dec 2018
- Dark matter direct detection constraints from gauge bosons loops hep-ph · Aug 2014
- Monojet versus rest of the world I: t-channel Models hep-ph · Feb 2014
- Beyond Effective Field Theory for Dark Matter Searches at the LHC hep-ph · Aug 2013
- Search for new phenomena in events with a photon and missing transverse momentum in $pp$ collisions at $\sqrt{s}=8$ TeV with the ATLAS detector hep-ex · Nov 2014
- Search for new physics in final states with a single photon and missing transverse momentum in proton-proton collisions at $\sqrt{s} =$ 13 TeV hep-ex · Sep 2018
- Search for new physics in the monophoton final state in proton-proton collisions at sqrt(s) = 13 TeV hep-ex · Jun 2017
- LHC constraints on gauge boson couplings to dark matter hep-ph · Jan 2015
How the literature uses it
19 arXiv papers cite this in 28 sentences
Papers citing it · 14 sentences without a confident label
Contests it 1 paper
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In terms of the sine ($s_w$) and cosine ($c_w$) of the weak mixing angle and the Wilson coefficients $C_B(Λ)$ and $C_W(Λ)$, the couplings $g_V_i V_j$ read [equation] These results do not coincide with the expressions reported in [ref] .
LHC constraints on gauge boson couplings to dark matter · Dependence on a single Wilson coefficient · contest 0.82
Builds on it 1 paper
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Second, to extend the studies [ref] by considering in addition the $E_T + W (→leptons)$ channel [ref] as well as the newest mono-jet data [ref] .
LHC constraints on gauge boson couplings to dark matter · Introduction · 0.96
Compares with it 1 paper
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Our Monte Carlo (MC) implementation has been validated by reproducing the numerical results of [ref] within theoretical uncertainties.
LHC constraints on gauge boson couplings to dark matter · Numerical results · 0.96
Cites it as background 10 papers
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The DM is produced with initial state radiation (ISR), whether that be a $Z$ [ref] , photon [ref] , jet [ref] , top [ref] or Higgs [ref] , allowing a measurement of the missing transverse energy (MET) carried by the DM.
Monojet versus rest of the world I: t-channel Models · Introduction · 0.94
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We consider a popular set of effective operator models for collider and indirect studies (see, for example [ref] ), the vector boson portal models .
Indirect Detection Constraints on the Model Space of Dark Matter Effective Theories · Constraints in Models with Interfering Channels · 0.95
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Although the dark matter leaves the detector without depositing energy, if it recoils against a final state parton, the resultant signature is a monojet recoiling against missing energy (MET) [ref] .
Beyond Effective Field Theory for Dark Matter Searches at the LHC · Introduction · 0.94
What it cites · 12 sentences without a confident label
Builds on 2 papers
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Recently [ref] , this has been extended to consider the case of an effective field theory which couples the dark matter fields to electroweak bosons rather than to the fermionic initial state.
Bounds on Dark Matter Interactions with Electroweak Gauge Bosons · Introduction · 0.81
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Recently [ref] , this has been extended to consider the case of an effective field theory which couples the dark matter fields to electroweak bosons rather than to the fermionic initial state.
Collider searches for dark matter in events with a Z boson and missing energy · Introduction · 0.81
Uses the method or tool of 1 paper
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We generate events in this model using madgraph5 [ref] .
MadGraph 5 : Going Beyond · Signal Efficiency and Limits · 1.00
Uses data or values from 1 paper
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The ATLAS experiment at the LHC has placed limits on dark matter production in the $γ+$ channel [ref] , where the dark matter fields couple to quark initial states and the photon has been emitted as initial state radiation.
Search for dark matter candidates and large extra dimensions in events with a photon and missing transverse momentum in pp collision data at sqrt(s) = 7 TeV with the ATLAS detector · Experimental Search · 0.84
Cites as background 3 papers
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The precise nature of this interaction is not known, but a useful general formalism is provided by effective field theories [ref] , which are strictly speaking valid only when the coupling occurs through states which are heavy compared with the typical energies involved ($∼$) and can be integrated out to give an effective four-fermion operator.
Maverick dark matter at colliders · Introduction · 0.88
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The precise nature of this interaction is not known, but a useful general formalism is provided by effective field theories [ref] , which are strictly speaking valid only when the coupling occurs through states which are heavy compared with the typical energies involved ($∼$) and can be integrated out to give an effective four-fermion operator.
Constraints on Dark Matter from Colliders · Introduction · 0.88
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The precise nature of this interaction is not known, but a useful general formalism is provided by effective field theories [ref] , which are strictly speaking valid only when the coupling occurs through states which are heavy compared with the typical energies involved ($∼$) and can be integrated out to give an effective four-fermion operator.
Missing Energy Signatures of Dark Matter at the LHC · Introduction · 0.88
Challenges and discussion
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