{"arxiv_id":"1605.00206","incoming":{"papers":8,"sentences":10,"groups":[{"kind":"extends","label":"Builds on it","papers":1,"sentences":1,"quotes":[{"arxiv_id":"2308.01090","title":"Exploring CP Violation beyond the Standard Model and the PQ Quality with Electric Dipole Moments","url":"/paper/2308.01090","section":"Vector-like Quarks","sentence":"Here we will discuss this model in some details, because it has not been comprehensively studied before concerning its EDM signatures beyond the scope of [ref] .","intent_p":0.9,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2011.02531","title":"Weinberg operator contribution to the nucleon electric dipole moment in the quark model","url":"/paper/2011.02531","section":"Introduction","sentence":"The Weinberg operator is relevant in many candidates of new physics beyond standard model such as the Higgs-doublet models [ref] , supersymmetric models [ref] , and other models [ref] .","intent_p":0.83,"contests_p":null},{"arxiv_id":"1609.02445","title":"An investgation on the electron's EDM from the electron's MDM","url":"/paper/1609.02445","section":"Introduction","sentence":"Over the years that have gone by, the sensibility of this sort of experiment has received a major improvement, providing ways to investigate the frontiers of the Standard Model (SM) [ref] , in the search for new physics and in the task of constraining parameters of new paths beyond the SM.","intent_p":0.85,"contests_p":null}]}],"unlabelled_sentences":7},"outgoing":{"papers":19,"sentences":33,"groups":[{"kind":"extends","label":"Builds on","papers":3,"sentences":5,"quotes":[{"arxiv_id":"1512.04850","title":"Composite Models for the 750 GeV Diphoton Excess","url":"/paper/1512.04850","section":"Composite pseudo-Nambu-Goldstone resonance","sentence":"The minimal model of [ref] can be generalized or modified to include a hypercolored fermion carrying a nonzero $SU(2)_L$ charge [ref] , e.g. $χ$ can transform as $(N,1,2)_Y_χ$ under $SU(N)_H×SU(3)_c×SU(2)_L×U(1)_Y$.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1512.04924","title":"Footprints of New Strong Dynamics via Anomaly and the 750 GeV Diphoton","url":"/paper/1512.04924","section":"Composite pseudo-Nambu-Goldstone resonance","sentence":"The minimal model of [ref] can be generalized or modified to include a hypercolored fermion carrying a nonzero $SU(2)_L$ charge [ref] , e.g. $χ$ can transform as $(N,1,2)_Y_χ$ under $SU(N)_H×SU(3)_c×SU(2)_L×U(1)_Y$.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1602.07297","title":"Di-photon resonance and Dark Matter as heavy pions","url":"/paper/1602.07297","section":"Introduction","sentence":"Our result on the neutron EDM can be applied also to the models in which $S$ corresponds to a composite pseudo-Nambu-Goldstone boson formed by a QCD-like hypercolor dyanmics which is confining at $Λ_HC$ [ref] .","intent_p":0.81,"contests_p":null}]},{"kind":"method_or_tool","label":"Uses the method or tool of","papers":3,"sentences":3,"quotes":[{"arxiv_id":"1205.2212","title":"QCD Corrections to Neutron Electric Dipole Moment from Dimension-six Four-Quark Operators","url":"/paper/1205.2212","section":"Neutron EDM","sentence":"For this, it is convenient to redefine the coefficients as C_1(μ) = d_q(μ)/m_q Q_q, C_2(μ) = d̃_q(μ)/m_q, C_3(μ) = d_W(μ)/g_3, which are satisfying the RG equation [ref] : μ∂C/∂μ = g_3^2/16π^2 γ C, with the anomalous dimension matrix γ≡( [ γ_e γ_eq 0; 0 γ_q γ_Gq; 0 0 γ_G ] ) = ( [ 8 C_F 8 C_F 0; 0 16C_F -4 N_c 2 N_c; 0 0 N_c + 2 n_f +β_0 ] ), where $C = ( C_1, C_2,C_3)^T$, $N_c=3$ is the number of color, $C_F = 4/3$ is a quadratic Casimir, $n_f$ is the number of active light quarks, and $β_0 = (33-2n_f)/3$ is the one-loop beta function coefficient.","intent_p":0.96,"contests_p":null},{"arxiv_id":"1204.2653","title":"Reevaluation of Neutron Electric Dipole Moment with QCD Sum Rules","url":"/paper/1204.2653","section":"Neutron EDM","sentence":"For this, one can take two approaches, the Naive Dimensional Analysis (NDA) [ref] or the QCD sum rule [ref] , essentially yielding similar results.","intent_p":0.94,"contests_p":null},{"arxiv_id":"1507.05836","title":"Nucleon Electric Dipole Moments in High-Scale Supersymmetric Models","url":"/paper/1507.05836","section":"Neutron EDM","sentence":"For this, one can take two approaches, the Naive Dimensional Analysis (NDA) [ref] or the QCD sum rule [ref] , essentially yielding similar results.","intent_p":0.94,"contests_p":null}]},{"kind":"data_used","label":"Uses data or values from","papers":1,"sentences":1,"quotes":[{"arxiv_id":"1310.7534","title":"Order of Magnitude Smaller Limit on the Electric Dipole Moment of the Electron","url":"/paper/1310.7534","section":"Electron EDM","sentence":"The above result shows the electron EDM associated with the $S-H$ mixing can saturate the current experimental upper limit $8.7 ×10^-29$ cm [ref] when $sinαsinξ_SH =O(10^-3)$.","intent_p":0.8,"contests_p":null}]}],"unlabelled_sentences":24},"claims":[],"thresholds":{"intent_p":0.8,"supports_p":0.95,"contests_p":0.7},"method":"Citing sentences come from each paper's LaTeX source; every \\cite marks the sentence and the works it cites. Pith's classifier typed each sentence. A label is shown at intent probability 0.8 or more (0.95 for support), a contest at 0.7 or more. Measured accuracy against two blind model families is at https://pith.science/accuracy. The quoted sentences are the citing authors' own.","held_up":null,"_links":{"html":"https://pith.science/paper/1605.00206"}}