{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:6KYVPNMP7BMMB2YZVXQUHJ5CKA","short_pith_number":"pith:6KYVPNMP","schema_version":"1.0","canonical_sha256":"f2b157b58ff858c0eb19ade143a7a2502a0d9c68e89f1c9b66a4454be635dd00","source":{"kind":"arxiv","id":"1310.0206","version":2},"attestation_state":"computed","paper":{"title":"Supersymmetric Lifshitz-like backgrounds from N=4 SYM with heavy quark density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anton F. Faedo, Benjo Fraser, S. Prem Kumar","submitted_at":"2013-10-01T09:30:43Z","abstract_excerpt":"We examine a class of gravity backgrounds obtained by considering the backreaction of a spatially uniform density of mutually BPS Wilson lines or heavy quarks in N=4 SUSY Yang-Mills theory. The configurations preserve eight supercharges and an SO(5) subgroup of the SO(6) R-symmetry. They are obtained by considering the 1/4-BPS geometries associated to smeared string/D3-brane (F1-D3) intersections. We argue that for the (partially) localized intersection, the geometry exhibits a flow from AdS_5 x S^5 in the UV to a novel IR scaling solution displaying anisotropic Lifshitz-like scaling with dyna"},"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":"1310.0206","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-01T09:30:43Z","cross_cats_sorted":[],"title_canon_sha256":"8559fe600ad4291f58d91ae84f24f8a73a1ab1efbc1461cf2b3657258c66f830","abstract_canon_sha256":"c433489ba3714807aa46ee90bda46a9723c6d96412a11c244ecae088751cd22d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:30:40.955200Z","signature_b64":"J1mfXHXNhaA/5SpsqVrZ7TdIzxMH3rcRGNBkHEVj5A4mBi/1/FzyJ45LlyIl+W22uUpThx+nkeBzs5z/grgFBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2b157b58ff858c0eb19ade143a7a2502a0d9c68e89f1c9b66a4454be635dd00","last_reissued_at":"2026-05-18T02:30:40.954540Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:30:40.954540Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supersymmetric Lifshitz-like backgrounds from N=4 SYM with heavy quark density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Anton F. Faedo, Benjo Fraser, S. Prem Kumar","submitted_at":"2013-10-01T09:30:43Z","abstract_excerpt":"We examine a class of gravity backgrounds obtained by considering the backreaction of a spatially uniform density of mutually BPS Wilson lines or heavy quarks in N=4 SUSY Yang-Mills theory. The configurations preserve eight supercharges and an SO(5) subgroup of the SO(6) R-symmetry. They are obtained by considering the 1/4-BPS geometries associated to smeared string/D3-brane (F1-D3) intersections. We argue that for the (partially) localized intersection, the geometry exhibits a flow from AdS_5 x S^5 in the UV to a novel IR scaling solution displaying anisotropic Lifshitz-like scaling with dyna"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.0206","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":""},"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":"1310.0206","created_at":"2026-05-18T02:30:40.954635+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.0206v2","created_at":"2026-05-18T02:30:40.954635+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.0206","created_at":"2026-05-18T02:30:40.954635+00:00"},{"alias_kind":"pith_short_12","alias_value":"6KYVPNMP7BMM","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_16","alias_value":"6KYVPNMP7BMMB2YZ","created_at":"2026-05-18T12:27:36.564083+00:00"},{"alias_kind":"pith_short_8","alias_value":"6KYVPNMP","created_at":"2026-05-18T12:27:36.564083+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/6KYVPNMP7BMMB2YZVXQUHJ5CKA","json":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA.json","graph_json":"https://pith.science/api/pith-number/6KYVPNMP7BMMB2YZVXQUHJ5CKA/graph.json","events_json":"https://pith.science/api/pith-number/6KYVPNMP7BMMB2YZVXQUHJ5CKA/events.json","paper":"https://pith.science/paper/6KYVPNMP"},"agent_actions":{"view_html":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA","download_json":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA.json","view_paper":"https://pith.science/paper/6KYVPNMP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.0206&json=true","fetch_graph":"https://pith.science/api/pith-number/6KYVPNMP7BMMB2YZVXQUHJ5CKA/graph.json","fetch_events":"https://pith.science/api/pith-number/6KYVPNMP7BMMB2YZVXQUHJ5CKA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA/action/storage_attestation","attest_author":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA/action/author_attestation","sign_citation":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA/action/citation_signature","submit_replication":"https://pith.science/pith/6KYVPNMP7BMMB2YZVXQUHJ5CKA/action/replication_record"}},"created_at":"2026-05-18T02:30:40.954635+00:00","updated_at":"2026-05-18T02:30:40.954635+00:00"}