{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:OICQMQI3757FKDRXU4AHZS4XR3","short_pith_number":"pith:OICQMQI3","schema_version":"1.0","canonical_sha256":"720506411bff7e550e37a7007ccb978ed6295bbfe5093dc5f1a093c79b1451e4","source":{"kind":"arxiv","id":"1511.05484","version":1},"attestation_state":"computed","paper":{"title":"Three-dimensional super Yang-Mills with compressible quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ant\\'on F. Faedo, Arnab Kundu, Christiana Pantelidou, David Mateos, Javier Tarr\\'io","submitted_at":"2015-11-17T17:38:00Z","abstract_excerpt":"We construct the gravity dual of three-dimensional, $SU(N_{\\textrm{c}})$ super Yang-Mills theory with $N_{\\textrm{f}}$ flavors of dynamical quarks in the presence of a non-zero quark density $N_{\\textrm{q}}$. The supergravity solutions include the backreaction of $N_{\\textrm{c}}$ color D2-branes and $N_{\\textrm{f}}$ flavor D6-branes with $N_{\\textrm{q}}$ units of electric flux on their worldvolume. For massless quarks, the solutions depend non-trivially only on the dimensionless combination $\\rho=N_{\\textrm{c}}^2 N_{\\textrm{q}} / \\lambda^2 N_{\\textrm{f}}^4$, with $\\lambda=g_{\\textrm{YM}}^2 N_{"},"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":"1511.05484","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-11-17T17:38:00Z","cross_cats_sorted":[],"title_canon_sha256":"5806eb927c9ecbf2b9aec138d76c0a59de516507a9ac5f8ee66de36954a2c60c","abstract_canon_sha256":"af8c9bf82594140c3b4483baed259c63dde1633dabd6d33651f9387d01875d43"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:45.405645Z","signature_b64":"Fb1XZQhZdKVSOK+0jz6yxJwFF52ax81rwiL+UzhaP5KfHJaxow2ZQ6iz0lCKZu6zG2x/3Iai5Pb5pbzq1uUPCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"720506411bff7e550e37a7007ccb978ed6295bbfe5093dc5f1a093c79b1451e4","last_reissued_at":"2026-05-18T01:16:45.404929Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:45.404929Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three-dimensional super Yang-Mills with compressible quark matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ant\\'on F. Faedo, Arnab Kundu, Christiana Pantelidou, David Mateos, Javier Tarr\\'io","submitted_at":"2015-11-17T17:38:00Z","abstract_excerpt":"We construct the gravity dual of three-dimensional, $SU(N_{\\textrm{c}})$ super Yang-Mills theory with $N_{\\textrm{f}}$ flavors of dynamical quarks in the presence of a non-zero quark density $N_{\\textrm{q}}$. The supergravity solutions include the backreaction of $N_{\\textrm{c}}$ color D2-branes and $N_{\\textrm{f}}$ flavor D6-branes with $N_{\\textrm{q}}$ units of electric flux on their worldvolume. For massless quarks, the solutions depend non-trivially only on the dimensionless combination $\\rho=N_{\\textrm{c}}^2 N_{\\textrm{q}} / \\lambda^2 N_{\\textrm{f}}^4$, with $\\lambda=g_{\\textrm{YM}}^2 N_{"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.05484","kind":"arxiv","version":1},"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":"1511.05484","created_at":"2026-05-18T01:16:45.405029+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.05484v1","created_at":"2026-05-18T01:16:45.405029+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.05484","created_at":"2026-05-18T01:16:45.405029+00:00"},{"alias_kind":"pith_short_12","alias_value":"OICQMQI3757F","created_at":"2026-05-18T12:29:34.919912+00:00"},{"alias_kind":"pith_short_16","alias_value":"OICQMQI3757FKDRX","created_at":"2026-05-18T12:29:34.919912+00:00"},{"alias_kind":"pith_short_8","alias_value":"OICQMQI3","created_at":"2026-05-18T12:29:34.919912+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/OICQMQI3757FKDRXU4AHZS4XR3","json":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3.json","graph_json":"https://pith.science/api/pith-number/OICQMQI3757FKDRXU4AHZS4XR3/graph.json","events_json":"https://pith.science/api/pith-number/OICQMQI3757FKDRXU4AHZS4XR3/events.json","paper":"https://pith.science/paper/OICQMQI3"},"agent_actions":{"view_html":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3","download_json":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3.json","view_paper":"https://pith.science/paper/OICQMQI3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.05484&json=true","fetch_graph":"https://pith.science/api/pith-number/OICQMQI3757FKDRXU4AHZS4XR3/graph.json","fetch_events":"https://pith.science/api/pith-number/OICQMQI3757FKDRXU4AHZS4XR3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3/action/storage_attestation","attest_author":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3/action/author_attestation","sign_citation":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3/action/citation_signature","submit_replication":"https://pith.science/pith/OICQMQI3757FKDRXU4AHZS4XR3/action/replication_record"}},"created_at":"2026-05-18T01:16:45.405029+00:00","updated_at":"2026-05-18T01:16:45.405029+00:00"}