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Effective theory approach to direct detection of dark matter
High Energy Physics - Phenomenology · Submitted 8 Dec 2017
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim An effective field theory approach is presented for evaluation of the dark matter direct detection rate in this lecture note.
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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. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
An effective field theory approach is presented for evaluation of the dark matter direct detection rate in this lecture note. This is prepared for the Les Houches Summer School Effective Field Theory in Particle Physics and Cosmology, July 2017.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | An effective field theory approach is presented for evaluation of the dark matter direct detection rate in this lecture note. | contribution 0.88 | 0.67 | 0.20 | asserted 0.99 |
| s1 | This is prepared for the Les Houches Summer School Effective Field Theory in Particle Physics and Cosmology, July 2017. | background 0.98 | 0.31 | 0.02 | asserted 0.96 |
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The paper
Original abstract
An effective field theory approach is presented for evaluation of the dark matter direct detection rate in this lecture note. This is prepared for the Les Houches Summer School Effective Field Theory in Particle Physics and Cosmology, July 2017.
Human review
References
How the literature uses it
13 arXiv papers cite this in 19 sentences
Papers citing it · 10 sentences without a confident label
Uses its method or tool 5 papers
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If DM is a Majorana fermion, the relevant effective operators for the evaluation of the DM-nucleon SI scattering cross section are given by [equation] where $O _ μν^q$ is the twist-2 operator for quark $q$, [equation] We use the following relations to evaluate the SI cross section from these operators [ref] , [equation] where $N$ stands for a nucleon ($p$, $n$), and $m_N$ is its mass.
Loop corrections to dark matter direct detection in a pseudoscalar mediator dark matter model · Direct Detection · 0.89
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Following Refs. [ref] , we calculate Wilson coefficients of the scalar-type and twist-2 DM-bottom-quark effective operators which arise from the box and triangle diagrams, as well as Wilson coefficient of DM-gluon effective operator [ref] which arises at the two-loop level.
Probing Bottom-flavored Scalar Dark Matters at Loop Level · Introduction · 0.94
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We calculate effective operators for the evaluation of MDM-nucleon spin independent scattering cross section following [ref] .
Direct detections of Majorana dark matter in vector portal · Introduction · 0.99
Uses its data or values 1 paper
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Values of $f_T_q^N$ can be found in [ref] .
Dark Matter from a Conformal Dark Sector · $T <$ (MS, HB, RGB) · 1.00
Cites it as background 2 papers
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The matrix element of the scalar heavy quark density between nucleon states is a relevant contribution to the cross-section for the scalar interaction of dark matter with ordinary matter [ref] .
How perturbative are heavy sea quarks? · Heavy quark content of the nucleon · 0.80
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Hadron-level interactions can induce either elastic or inelastic scattering of the DM off a nuclear target, depending on the model of the dark sector [ref] .
Constraining Gluonic Contact Interaction of a Neutrino-philic Dark Fermion at Hadron Colliders and Direct Detection Experiments · Absorption at Nuclear Targets · 0.88
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