{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:IW23ZQUUKRWEODHC73NM2N6WCG","short_pith_number":"pith:IW23ZQUU","schema_version":"1.0","canonical_sha256":"45b5bcc294546c470ce2fedacd37d61186494c440114b5a58f68fd60452c460f","source":{"kind":"arxiv","id":"1803.03078","version":1},"attestation_state":"computed","paper":{"title":"Pulsating strings with mixed three-form flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Juan Miguel Nieto, Rafael Hernandez, Roberto Ruiz","submitted_at":"2018-03-08T13:22:01Z","abstract_excerpt":"Circular strings pulsating in $AdS_3 \\times S^3 \\times T^4$ with mixed R-R and NS-NS three-form fluxes can be described by an integrable deformation of the one-dimensional Neumann-Rosochatius mechanical model. In this article we find a general class of pulsating solutions to this integrable system that can be expressed in terms of elliptic functions. In the limit of strings moving in $AdS_{3}$ with pure NS-NS three-form flux, where the action reduces to the $SL(2,\\mathbb{R})$ WZW model, we find agreement with the analysis of the classical solutions of the system performed using spectral flow b"},"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":"1803.03078","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-03-08T13:22:01Z","cross_cats_sorted":[],"title_canon_sha256":"3031779a99f9b590508fce2c5c1079b69a57e5bc9eb198884cb73125719889a0","abstract_canon_sha256":"66c8057dc02353acdf5e8a476c5214866b6124fbe620ec93c0c482a28a491ef0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:15.541648Z","signature_b64":"KEgHIn5z4mdnKNicfZzaXcwCbk6Q3EWqxH/hG8a6QrrIuRBe4XVxmFNSIwpFaPdK6N2DbQdWJOxBLDr6N4MeBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45b5bcc294546c470ce2fedacd37d61186494c440114b5a58f68fd60452c460f","last_reissued_at":"2026-05-18T00:15:15.541125Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:15.541125Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pulsating strings with mixed three-form flux","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Juan Miguel Nieto, Rafael Hernandez, Roberto Ruiz","submitted_at":"2018-03-08T13:22:01Z","abstract_excerpt":"Circular strings pulsating in $AdS_3 \\times S^3 \\times T^4$ with mixed R-R and NS-NS three-form fluxes can be described by an integrable deformation of the one-dimensional Neumann-Rosochatius mechanical model. In this article we find a general class of pulsating solutions to this integrable system that can be expressed in terms of elliptic functions. In the limit of strings moving in $AdS_{3}$ with pure NS-NS three-form flux, where the action reduces to the $SL(2,\\mathbb{R})$ WZW model, we find agreement with the analysis of the classical solutions of the system performed using spectral flow b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.03078","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":"1803.03078","created_at":"2026-05-18T00:15:15.541207+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.03078v1","created_at":"2026-05-18T00:15:15.541207+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.03078","created_at":"2026-05-18T00:15:15.541207+00:00"},{"alias_kind":"pith_short_12","alias_value":"IW23ZQUUKRWE","created_at":"2026-05-18T12:32:31.084164+00:00"},{"alias_kind":"pith_short_16","alias_value":"IW23ZQUUKRWEODHC","created_at":"2026-05-18T12:32:31.084164+00:00"},{"alias_kind":"pith_short_8","alias_value":"IW23ZQUU","created_at":"2026-05-18T12:32:31.084164+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.20252","citing_title":"Non-relativistic Strings: Classical solutions and exactly solvable models","ref_index":65,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG","json":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG.json","graph_json":"https://pith.science/api/pith-number/IW23ZQUUKRWEODHC73NM2N6WCG/graph.json","events_json":"https://pith.science/api/pith-number/IW23ZQUUKRWEODHC73NM2N6WCG/events.json","paper":"https://pith.science/paper/IW23ZQUU"},"agent_actions":{"view_html":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG","download_json":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG.json","view_paper":"https://pith.science/paper/IW23ZQUU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.03078&json=true","fetch_graph":"https://pith.science/api/pith-number/IW23ZQUUKRWEODHC73NM2N6WCG/graph.json","fetch_events":"https://pith.science/api/pith-number/IW23ZQUUKRWEODHC73NM2N6WCG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG/action/storage_attestation","attest_author":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG/action/author_attestation","sign_citation":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG/action/citation_signature","submit_replication":"https://pith.science/pith/IW23ZQUUKRWEODHC73NM2N6WCG/action/replication_record"}},"created_at":"2026-05-18T00:15:15.541207+00:00","updated_at":"2026-05-18T00:15:15.541207+00:00"}