{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:7HL3V2RRI475TMNHXQV57FSPLQ","short_pith_number":"pith:7HL3V2RR","schema_version":"1.0","canonical_sha256":"f9d7baea31473fd9b1a7bc2bdf964f5c08fde00d704aca9ab46268cfe9b20b1c","source":{"kind":"arxiv","id":"1906.10714","version":1},"attestation_state":"computed","paper":{"title":"A non-integrable quench from AdS/dCFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"Charlotte Kristjansen, Kasper E. Vardinghus, Marius de Leeuw","submitted_at":"2019-06-25T18:13:23Z","abstract_excerpt":"We study the matrix product state which appears as the boundary state of the AdS/dCFT set-up where a probe D7 brane wraps two two-spheres stabilized by fluxes. The matrix product state plays a dual role, on one hand acting as a tool for computing one-point functions in a domain wall version of N=4 SYM and on the other hand acting as the initial state in the study of quantum quenches of the Heisenberg spin chain. We derive a number of selection rules for the overlaps between the matrix product state and the eigenstates of the Heisenberg spin chain and in particular demonstrate that the matrix p"},"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":"1906.10714","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-06-25T18:13:23Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"d10ab6d231b534a3b7ac28727bad18fcd5977ad3c4a4a1985fe85c5f3f26701d","abstract_canon_sha256":"c63faffe3b72dfa2bca5b12b2ce45ce80fbb0c83c2e6a876b5ea94bd1436135f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:05:11.800254Z","signature_b64":"5/IQGn1MclfVok+ez/t455kGS0Z6dBLuLeoycHOAOL9yk4XUhcxMzrqbJRvqVLCLT9wg/HLkGCc2+y4avSQhDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f9d7baea31473fd9b1a7bc2bdf964f5c08fde00d704aca9ab46268cfe9b20b1c","last_reissued_at":"2026-07-05T00:05:11.799872Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:05:11.799872Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A non-integrable quench from AdS/dCFT","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"hep-th","authors_text":"Charlotte Kristjansen, Kasper E. Vardinghus, Marius de Leeuw","submitted_at":"2019-06-25T18:13:23Z","abstract_excerpt":"We study the matrix product state which appears as the boundary state of the AdS/dCFT set-up where a probe D7 brane wraps two two-spheres stabilized by fluxes. The matrix product state plays a dual role, on one hand acting as a tool for computing one-point functions in a domain wall version of N=4 SYM and on the other hand acting as the initial state in the study of quantum quenches of the Heisenberg spin chain. We derive a number of selection rules for the overlaps between the matrix product state and the eigenstates of the Heisenberg spin chain and in particular demonstrate that the matrix p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.10714","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1906.10714/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":"1906.10714","created_at":"2026-07-05T00:05:11.799927+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.10714v1","created_at":"2026-07-05T00:05:11.799927+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.10714","created_at":"2026-07-05T00:05:11.799927+00:00"},{"alias_kind":"pith_short_12","alias_value":"7HL3V2RRI475","created_at":"2026-07-05T00:05:11.799927+00:00"},{"alias_kind":"pith_short_16","alias_value":"7HL3V2RRI475TMNH","created_at":"2026-07-05T00:05:11.799927+00:00"},{"alias_kind":"pith_short_8","alias_value":"7HL3V2RR","created_at":"2026-07-05T00:05:11.799927+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.11985","citing_title":"String theory methods for defect CFTs","ref_index":73,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ","json":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ.json","graph_json":"https://pith.science/api/pith-number/7HL3V2RRI475TMNHXQV57FSPLQ/graph.json","events_json":"https://pith.science/api/pith-number/7HL3V2RRI475TMNHXQV57FSPLQ/events.json","paper":"https://pith.science/paper/7HL3V2RR"},"agent_actions":{"view_html":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ","download_json":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ.json","view_paper":"https://pith.science/paper/7HL3V2RR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.10714&json=true","fetch_graph":"https://pith.science/api/pith-number/7HL3V2RRI475TMNHXQV57FSPLQ/graph.json","fetch_events":"https://pith.science/api/pith-number/7HL3V2RRI475TMNHXQV57FSPLQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ/action/storage_attestation","attest_author":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ/action/author_attestation","sign_citation":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ/action/citation_signature","submit_replication":"https://pith.science/pith/7HL3V2RRI475TMNHXQV57FSPLQ/action/replication_record"}},"created_at":"2026-07-05T00:05:11.799927+00:00","updated_at":"2026-07-05T00:05:11.799927+00:00"}