{"arxiv_id":"hep-ph/0402023","incoming":{"papers":36,"sentences":47,"groups":[{"kind":"method_or_tool","label":"Uses its method or tool","papers":2,"sentences":2,"quotes":[{"arxiv_id":"2303.02822","title":"Quantifying Limits on CP Violating Phases from EDMs in Supersymmetry","url":"/paper/2303.02822","section":"Supersymmetric contribution to the (C)EDMs","sentence":"[Our notation is also specified in Appendix [ref].] We have updated the code used in [ref] , taking into account all the updates discussed in Section [ref] and the 2-loop contributions described in Appendix [ref].","intent_p":0.8,"contests_p":null},{"arxiv_id":"1208.4106","title":"Neutralino Decays in the Complex MSSM at One-Loop: a Comparison of On-Shell Renormalization Schemes","url":"/paper/1208.4106","section":"Numerical analysis","sentence":"[In addition, the heavy quarks [ref] , the electron [ref] and the deuteron [ref] EDM's should be taken into account.] Using [ref] , we have calculated these EDM's, and find that in the scenarios studied the bounds due to the Thallium EDM are the most constraining, $≲π/100$.","intent_p":0.85,"contests_p":null}]},{"kind":"data_used","label":"Uses its data or values","papers":3,"sentences":3,"quotes":[{"arxiv_id":"2404.00516","title":"Electric Dipole Moments in 5+3 Flavor Weak Effective Theory","url":"/paper/2404.00516","section":"Nucleon EDMs","sentence":"In Refs. [ref] , the $u$ and $d$ qCEDM contribution to the neutron and proton EDMs was estimated to be [equation] with roughly 50% uncertainty.","intent_p":0.99,"contests_p":null},{"arxiv_id":"1909.09373","title":"Bounds on CP-violating Higgs-gluon interactions: the case of vanishing light-quark Yukawa couplings","url":"/paper/1909.09373","section":"Dimension-six contribution","sentence":"The EDM contributions from down and up quarks have been calculated with an accuracy of $5%$ using lattice QCD (LQCD) [ref] , while QCD sum-rule calculations [ref] allow to determine the contributions from the down-quark and up-quark CEDMs with uncertainties of $50%$.","intent_p":0.84,"contests_p":null},{"arxiv_id":"2203.08103","title":"Electric dipole moments and the search for new physics","url":"/paper/2203.08103","section":"Theoretical framework: status and challenges","sentence":"The quoted matrix elements of the quark cEDM operators are obtained via QCD sum rules [ref] .","intent_p":0.85,"contests_p":null}]},{"kind":"comparison","label":"Compares with it","papers":3,"sentences":4,"quotes":[{"arxiv_id":"1412.5471","title":"P- and T-Violating Lagrangians in Chiral Effective Field Theory and Nuclear Electric Dipole Moments","url":"/paper/1412.5471","section":"Results of the numerical EDM computation","sentence":"While the predictions involving the coefficient $Δ_3$ are novel and the $C_1,2$ contributions exceed the ones based on phenomenological $P$- and $T$-conserving potentials by more than roughly one order in magnitude, the single-nucleon and $g_0,1$-induced contributions are largely consistent with those in [ref] based on phenomenological $P$- and $T$-conserving potentials.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1912.01641","title":"Deuteron electric dipole moment from holographic QCD","url":"/paper/1912.01641","section":"Conclusion","sentence":"Using the deuteron description emerging from the same model and the results for the EDMs of nucleons, we were able to estimate the EDM of the deuteron bound state, obtaining a value close to the estimate given in Ref. [ref] : even if this numerical closeness may be regarded as an accident, considering the many approximations implicit in our computations (and the lack of the inclusion of two-body contributions which are expected to give comparable EDMs), it is still remarkable that we obtain the correct order of magnitude and sign, despite this term being formally subleading in $λ$ and $$ before phenomenological extrapolation of the parameters.","intent_p":1.0,"contests_p":null},{"arxiv_id":"1909.08955","title":"Sum rules for CP-violating operators of Weinberg type","url":"/paper/1909.08955","section":"Conclusions","sentence":"Sum-rule studies of the $θ$-term and CEDM contributions to the nEDM [ref] have also found uncertainties of a similar magnitude.","intent_p":0.93,"contests_p":null}]},{"kind":"background","label":"Cites it as background","papers":6,"sentences":6,"quotes":[{"arxiv_id":"2308.01090","title":"Exploring CP Violation beyond the Standard Model and the PQ Quality with Electric Dipole Moments","url":"/paper/2308.01090","section":"Introduction","sentence":"Previous studies along this line include [ref] .","intent_p":0.87,"contests_p":null},{"arxiv_id":"1912.01641","title":"Deuteron electric dipole moment from holographic QCD","url":"/paper/1912.01641","section":"Introduction","sentence":"Theoretical estimates are essentially obtained through QCD sum rules [ref] and via models of nuclear potential [ref] [For a review on the topic of EDMs of light nuclei, see [ref] ] : the tool that provided most estimates for $$, the chiral Lagrangian, tends to produce electric dipole moments that are equal in magnitude and opposite in sign for the neutron and the proton, so that the single nucleon contributions, which are expected to be important, tend to cancel each other inside the deuteron: nevertheless some results in this context are available for the $θ$ induced EDM as lower bounds [ref] , while two-nucleon terms can also be computed [ref] .","intent_p":0.84,"contests_p":null},{"arxiv_id":"1412.5471","title":"P- and T-Violating Lagrangians in Chiral Effective Field Theory and Nuclear Electric Dipole Moments","url":"/paper/1412.5471","section":"Results of the numerical EDM computation","sentence":"The computation of the EDMs of the deuteron, helion and triton with phenomenological $P$- and $T$-conserving wave functions have been performed by various groups over the past years [ref] .","intent_p":0.92,"contests_p":null},{"arxiv_id":"1204.4001","title":"Heavy Scalar Tau Decays in the Complex MSSM: A Full One-Loop Analysis","url":"/paper/1204.4001","section":"Full one-loop results for varying $$","sentence":"Experimental constraints on the (combinations of) complex phases arise in particular from their contributions to electric dipole moments of the electron and the neutron (see EDMrev2,EDMPilaftsis and references therein), of the deuteron [ref] and of heavy quarks [ref] .","intent_p":0.85,"contests_p":null},{"arxiv_id":"1112.2830","title":"Gluino Decays in the Complex MSSM: A Full One-Loop Analysis","url":"/paper/1112.2830","section":"Full one-loop results for varying $$","sentence":"Experimental constraints on the (combinations of) complex phases arise in particular from their contributions to electric dipole moments of heavy quarks [ref] , of the electron and the neutron (see EDMrev2,EDMPilaftsis and references therein), and of deuteron [ref] , EDMrev1,EDMrev2,EDMrev3 for reviews.","intent_p":0.87,"contests_p":null}]}],"unlabelled_sentences":32},"outgoing":{"papers":0,"sentences":0,"groups":[],"unlabelled_sentences":0},"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/hep-ph/0402023"}}