{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:Q4EBEGAVG3IAZYUOGK4H2O62O6","short_pith_number":"pith:Q4EBEGAV","schema_version":"1.0","canonical_sha256":"870812181536d00ce28e32b87d3bda77b905703630f7b24923551d314de05927","source":{"kind":"arxiv","id":"hep-ph/0512203","version":2},"attestation_state":"computed","paper":{"title":"Vortices in gauge models at finite density with vector condensates","license":"","headline":"","cross_cats":["cond-mat.supr-con","hep-th"],"primary_cat":"hep-ph","authors_text":"E.V. Gorbar, Junji Jia, V.A. Miransky","submitted_at":"2005-12-15T18:47:15Z","abstract_excerpt":"There exists a class of gauge models incorporating a finite density of matter in which the Higgs mechanism is provided by condensates of gauge (or gauge and scalar) fields, i.e., there are vector condensates in this case. We describe vortex solutions in the simplest model in this class, the gauged $SU(2)\\times U(1)_Y$ $\\sigma$-model with the chemical potential for hypercharge $Y$, in which the gauge symmetry is completely broken. It is shown that there are three types of topologically stable vortices in the model, connected either with photon field or hypercharge gauge field, or with both of t"},"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":"hep-ph/0512203","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-15T18:47:15Z","cross_cats_sorted":["cond-mat.supr-con","hep-th"],"title_canon_sha256":"37a669d82835b7140f55a52f45192fc02f40ba3e01e73f71a3a75564ce2d7274","abstract_canon_sha256":"d333513f71665c64fee67ee816ac58f11172f068cc24c1be390ce0adac722641"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:52:09.468290Z","signature_b64":"nASJtBuwCMvErAjy2x324yq8orlGq4uTapGNEZJWZuGr039spwmvwgA0MPGyfF2LZQLIs7LAE33aO4zK2+d7AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"870812181536d00ce28e32b87d3bda77b905703630f7b24923551d314de05927","last_reissued_at":"2026-07-04T14:52:09.467909Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:52:09.467909Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Vortices in gauge models at finite density with vector condensates","license":"","headline":"","cross_cats":["cond-mat.supr-con","hep-th"],"primary_cat":"hep-ph","authors_text":"E.V. Gorbar, Junji Jia, V.A. Miransky","submitted_at":"2005-12-15T18:47:15Z","abstract_excerpt":"There exists a class of gauge models incorporating a finite density of matter in which the Higgs mechanism is provided by condensates of gauge (or gauge and scalar) fields, i.e., there are vector condensates in this case. We describe vortex solutions in the simplest model in this class, the gauged $SU(2)\\times U(1)_Y$ $\\sigma$-model with the chemical potential for hypercharge $Y$, in which the gauge symmetry is completely broken. It is shown that there are three types of topologically stable vortices in the model, connected either with photon field or hypercharge gauge field, or with both of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0512203","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0512203/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-ph/0512203","created_at":"2026-07-04T14:52:09.467969+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0512203v2","created_at":"2026-07-04T14:52:09.467969+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0512203","created_at":"2026-07-04T14:52:09.467969+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q4EBEGAVG3IA","created_at":"2026-07-04T14:52:09.467969+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q4EBEGAVG3IAZYUO","created_at":"2026-07-04T14:52:09.467969+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q4EBEGAV","created_at":"2026-07-04T14:52:09.467969+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6","json":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6.json","graph_json":"https://pith.science/api/pith-number/Q4EBEGAVG3IAZYUOGK4H2O62O6/graph.json","events_json":"https://pith.science/api/pith-number/Q4EBEGAVG3IAZYUOGK4H2O62O6/events.json","paper":"https://pith.science/paper/Q4EBEGAV"},"agent_actions":{"view_html":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6","download_json":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6.json","view_paper":"https://pith.science/paper/Q4EBEGAV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0512203&json=true","fetch_graph":"https://pith.science/api/pith-number/Q4EBEGAVG3IAZYUOGK4H2O62O6/graph.json","fetch_events":"https://pith.science/api/pith-number/Q4EBEGAVG3IAZYUOGK4H2O62O6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6/action/storage_attestation","attest_author":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6/action/author_attestation","sign_citation":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6/action/citation_signature","submit_replication":"https://pith.science/pith/Q4EBEGAVG3IAZYUOGK4H2O62O6/action/replication_record"}},"created_at":"2026-07-04T14:52:09.467969+00:00","updated_at":"2026-07-04T14:52:09.467969+00:00"}