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The generalized lepton sector is also flavor conserving but with the new Yukawa couplings completely decoupled from lepton mass proportionality. The model is one loop stable under renormalization group evolution and it allows to reproduce the <jats:inline-formula><jats:alternatives><jats:tex-math>$$g-2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>g<\/mml:mi>\n                    <mml:mo>-<\/mml:mo>\n                    <mml:mn>2<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> muon anomaly together with the different scenarios one can consider for the electron <jats:inline-formula><jats:alternatives><jats:tex-math>$$g-2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>g<\/mml:mi>\n                    <mml:mo>-<\/mml:mo>\n                    <mml:mn>2<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> anomaly, related to the Cesium and\/or to the Rubidium recoil measurements of the fine structure constant. Thorough parameter space analyses are performed to constrain all the model parameters in the different scenarios, either including or not including the recent CDF measurement of the W boson mass. For light new scalars with masses in the 0.2\u20131.0 TeV range, the muon anomaly receives dominant one loop contributions; it is for heavy new scalars with masses above 1.2 TeV that two loop Barr\u2013Zee diagrams are needed. The electron <jats:inline-formula><jats:alternatives><jats:tex-math>$$g-2$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:mi>g<\/mml:mi>\n                    <mml:mo>-<\/mml:mo>\n                    <mml:mn>2<\/mml:mn>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> anomaly, if any, must always be obtained with the two loop contributions. The final allowed regions are quite sensitive to the assumptions about perturbativity of Yukawa couplings, which influence unexpected observables like the allowed scalar mass ranges. On that respect, intermediate scalar masses, highly constrained by direct LHC searches, are allowed provided that the new lepton Yukawa couplings are fully scrutinized, including values up to 250 GeV. In the framework of a complete model, fully numerically analysed, we show the implications of the recent <jats:inline-formula><jats:alternatives><jats:tex-math>$$M_{W}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:msub>\n                    <mml:mi>M<\/mml:mi>\n                    <mml:mi>W<\/mml:mi>\n                  <\/mml:msub>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> measurement.<\/jats:p>","DOI":"10.1140\/epjc\/s10052-022-10893-x","type":"journal-article","created":{"date-parts":[[2022,10,14]],"date-time":"2022-10-14T20:19:56Z","timestamp":1665778796000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":30,"title":["Muon and electron $$g-2$$ anomalies in a flavor conserving 2HDM with an oblique view on the CDF $$M_W$$ value"],"prefix":"10.1140","volume":"82","author":[{"given":"Francisco J.","family":"Botella","sequence":"first","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0002-5242-3019","authenticated-orcid":false,"given":"Fernando","family":"Cornet-Gomez","sequence":"additional","affiliation":[]},{"given":"Carlos","family":"Mir\u00f3","sequence":"additional","affiliation":[]},{"given":"Miguel","family":"Nebot","sequence":"additional","affiliation":[]}],"member":"297","published-online":{"date-parts":[[2022,10,14]]},"reference":[{"key":"10893_CR1","unstructured":"Muon g-2 Collaboration, G.W. 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