{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:G7LMGZ5R2ABLDD7FTKAOKVHOZI","short_pith_number":"pith:G7LMGZ5R","schema_version":"1.0","canonical_sha256":"37d6c367b1d002b18fe59a80e554eeca39a2d8b106d8436ebedf6b0ad7811960","source":{"kind":"arxiv","id":"1106.0034","version":3},"attestation_state":"computed","paper":{"title":"Theory and phenomenology of two-Higgs-doublet models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. C. Branco, Joao P. Silva, L. Lavoura, Marc Sher, M. N. Rebelo, P. M. Ferreira","submitted_at":"2011-05-31T21:32:22Z","abstract_excerpt":"We discuss theoretical and phenomenological aspects of two-Higgs-doublet extensions of the Standard Model. In general, these extensions have scalar mediated flavour changing neutral currents which are strongly constrained by experiment. Various strategies are discussed to control these flavour changing scalar currents and their phenomenological consequences are analysed. In particular, scenarios with natural flavour conservation are investigated, including the so-called type I and type II models as well as lepton-specific and inert models. Type III models are then discussed, where scalar flavo"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1106.0034","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-05-31T21:32:22Z","cross_cats_sorted":[],"title_canon_sha256":"58d52ec1f1f1957344511ec5114849c2315fab7baab7745628b1f84ee46fa760","abstract_canon_sha256":"38c5c1464fbf7dec5bdab37bac6c83c03471fe541a8d06ba282b7c11384dda94"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:45.174028Z","signature_b64":"2b0bPItJzon3wkFeAtXfhvEFOvP+5HYFoKRYHzUSxAA91rt65sqYLXPSTscKm9heKPN5viMIlwOLo/urLWn5Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"37d6c367b1d002b18fe59a80e554eeca39a2d8b106d8436ebedf6b0ad7811960","last_reissued_at":"2026-05-18T02:01:45.173206Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:45.173206Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory and phenomenology of two-Higgs-doublet models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. C. Branco, Joao P. Silva, L. Lavoura, Marc Sher, M. N. Rebelo, P. M. Ferreira","submitted_at":"2011-05-31T21:32:22Z","abstract_excerpt":"We discuss theoretical and phenomenological aspects of two-Higgs-doublet extensions of the Standard Model. In general, these extensions have scalar mediated flavour changing neutral currents which are strongly constrained by experiment. Various strategies are discussed to control these flavour changing scalar currents and their phenomenological consequences are analysed. In particular, scenarios with natural flavour conservation are investigated, including the so-called type I and type II models as well as lepton-specific and inert models. Type III models are then discussed, where scalar flavo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.0034","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1106.0034","created_at":"2026-05-18T02:01:45.173346+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.0034v3","created_at":"2026-05-18T02:01:45.173346+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.0034","created_at":"2026-05-18T02:01:45.173346+00:00"},{"alias_kind":"pith_short_12","alias_value":"G7LMGZ5R2ABL","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_16","alias_value":"G7LMGZ5R2ABLDD7F","created_at":"2026-05-18T12:26:28.662955+00:00"},{"alias_kind":"pith_short_8","alias_value":"G7LMGZ5R","created_at":"2026-05-18T12:26:28.662955+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":37,"internal_anchor_count":20,"sample":[{"citing_arxiv_id":"1910.13125","citing_title":"Detecting gravitational waves from cosmological phase transitions with LISA: an update","ref_index":106,"is_internal_anchor":true},{"citing_arxiv_id":"2404.19197","citing_title":"Does the Electron EDM Preclude Electroweak Baryogenesis ?","ref_index":64,"is_internal_anchor":true},{"citing_arxiv_id":"2305.10915","citing_title":"Optimizing The Cut And Count Method In Phenomenological Studies","ref_index":31,"is_internal_anchor":true},{"citing_arxiv_id":"2504.14529","citing_title":"Search for Dark Matter in 2HDMS at LHC and future Lepton Colliders","ref_index":69,"is_internal_anchor":true},{"citing_arxiv_id":"2605.21870","citing_title":"Deep Neural Networks for Heavy Lepton-Flavor-Violating Higgs Searches at the LHC","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2512.17002","citing_title":"Intrinsic Properties of Large CP Violation in the Complex Two-Higgs-Doublet Model","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2605.19144","citing_title":"Search for Higgs boson decays into two neutral scalars with unequal masses in final states with b quarks and tau leptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16756","citing_title":"Higgs Physics with the XFEL Compton $\\boldsymbol{\\gamma\\gamma}$ Collider Concept at $\\boldsymbol{\\sqrt{s}=125}$ GeV","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16655","citing_title":"Search for the nonresonant production of a pair of additional Higgs bosons in the Type-X two-Higgs-doublet model in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":14,"is_internal_anchor":true},{"citing_arxiv_id":"2508.06947","citing_title":"Search for light pseudoscalar boson pairs produced from Higgs boson decays using the 4$\\tau$ and 2$\\mu$2$\\tau$ final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","ref_index":7,"is_internal_anchor":true},{"citing_arxiv_id":"2509.01677","citing_title":"Machine Learning in the 2HDM2S model for Dark Matter","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2509.08043","citing_title":"Testing Viability of Benchmark Dark Matter Models for the Galactic Center Excess","ref_index":70,"is_internal_anchor":true},{"citing_arxiv_id":"2510.21420","citing_title":"The Standard Model partial unification scale as a guide to new physics model building","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2511.21874","citing_title":"Model-independent probes of CP violation in the heavy scalar sector at muon colliders","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2512.18959","citing_title":"Scalar-Mediated Inelastic Dark Matter as a Solution to Small-Scale Structure Anomalies","ref_index":50,"is_internal_anchor":true},{"citing_arxiv_id":"2601.02808","citing_title":"Two Higgs doublet model with a complex singlet scalar and Multi-critical Point Principle","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2602.17643","citing_title":"Revisiting the Higgs-mass calculation in the scale-invariant THDM","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2603.29076","citing_title":"Probing Heavy Neutral Higgs Bosons via Single Vector-Like Bottom Quark Production at the HL-LHC","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13078","citing_title":"Possibility of Probing an Extra Higgs Boson at the Compact Linear Collider","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2605.13336","citing_title":"Probing Boosted Light Scalars in the Type-I 2HDM","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2604.27471","citing_title":"Constraints on a Light Singlet Scalar from Combined Exotic Higgs Decays","ref_index":12,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26817","citing_title":"When Two Loops Matter: Electroweak Precision in the SMEFT","ref_index":79,"is_internal_anchor":false},{"citing_arxiv_id":"2604.24924","citing_title":"Forward backward CP asymmetry in $\\tau^- \\to K \\pi \\nu_{\\tau}$ in the Left-Right Inverse seesaw model","ref_index":63,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22278","citing_title":"A Flavor Specific Chiral $U(1)_X$ Framework for Explaining the ATOMKI Anomaly","ref_index":75,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21670","citing_title":"Effective field theory interpretation of ATLAS measurements involving the Higgs boson, electroweak bosons and the top quark","ref_index":34,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI","json":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI.json","graph_json":"https://pith.science/api/pith-number/G7LMGZ5R2ABLDD7FTKAOKVHOZI/graph.json","events_json":"https://pith.science/api/pith-number/G7LMGZ5R2ABLDD7FTKAOKVHOZI/events.json","paper":"https://pith.science/paper/G7LMGZ5R"},"agent_actions":{"view_html":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI","download_json":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI.json","view_paper":"https://pith.science/paper/G7LMGZ5R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.0034&json=true","fetch_graph":"https://pith.science/api/pith-number/G7LMGZ5R2ABLDD7FTKAOKVHOZI/graph.json","fetch_events":"https://pith.science/api/pith-number/G7LMGZ5R2ABLDD7FTKAOKVHOZI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI/action/storage_attestation","attest_author":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI/action/author_attestation","sign_citation":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI/action/citation_signature","submit_replication":"https://pith.science/pith/G7LMGZ5R2ABLDD7FTKAOKVHOZI/action/replication_record"}},"created_at":"2026-05-18T02:01:45.173346+00:00","updated_at":"2026-05-18T02:01:45.173346+00:00"}