{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:LVOQN6ICNMWLZ4LRI2JBMCBMYC","short_pith_number":"pith:LVOQN6IC","schema_version":"1.0","canonical_sha256":"5d5d06f9026b2cbcf171469216082cc0a6a43868ce112068ce34903ebedd4ec1","source":{"kind":"arxiv","id":"1909.12632","version":3},"attestation_state":"computed","paper":{"title":"Neumann-Rosochatius system for strings in ABJ Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Adrita Chakraborty, Kamal L. Panigrahi","submitted_at":"2019-09-27T11:38:24Z","abstract_excerpt":"Neumann-Rosochatius system is a well known one dimensional integrable system. We study the rotating and pulsating string in $AdS_4 \\times \\mathbb{CP}^3$ with a $B_{\\rm{NS}}$ holonomy turned on over $\\mathbb{CP}^1 \\subset \\mathbb{CP}^3$, or the so called Aharony-Bergman-Jafferis (ABJ) background. We observe that the string equations of motion in both cases are integrable and the Lagrangians reduce to a form similar to that of deformed Neuman-Rosochatius system. We find out the scaling relations among various conserved charges and comment on the finite size effect for the dyonic giant magnons on"},"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":"1909.12632","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-09-27T11:38:24Z","cross_cats_sorted":[],"title_canon_sha256":"a07f4f66cab8a1719caab5b69381b1acb851a4ae9d503193a523cb7173ad6802","abstract_canon_sha256":"8dd058099fbfd0948d033a4631a25e78b27ebe6af5a4e8ffd951759eb70e67cb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:36:38.224367Z","signature_b64":"mt/RZWTnFfy1PtChdVlkwrGYTUeW26sGb0BhhkKN3uepvoejOZdYm+2qdsufchdjkRLcR4jBlsRY0cWNZKVgDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d5d06f9026b2cbcf171469216082cc0a6a43868ce112068ce34903ebedd4ec1","last_reissued_at":"2026-07-05T00:36:38.223962Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:36:38.223962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Neumann-Rosochatius system for strings in ABJ Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Adrita Chakraborty, Kamal L. Panigrahi","submitted_at":"2019-09-27T11:38:24Z","abstract_excerpt":"Neumann-Rosochatius system is a well known one dimensional integrable system. We study the rotating and pulsating string in $AdS_4 \\times \\mathbb{CP}^3$ with a $B_{\\rm{NS}}$ holonomy turned on over $\\mathbb{CP}^1 \\subset \\mathbb{CP}^3$, or the so called Aharony-Bergman-Jafferis (ABJ) background. We observe that the string equations of motion in both cases are integrable and the Lagrangians reduce to a form similar to that of deformed Neuman-Rosochatius system. We find out the scaling relations among various conserved charges and comment on the finite size effect for the dyonic giant magnons on"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.12632","kind":"arxiv","version":3},"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/1909.12632/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":"1909.12632","created_at":"2026-07-05T00:36:38.224017+00:00"},{"alias_kind":"arxiv_version","alias_value":"1909.12632v3","created_at":"2026-07-05T00:36:38.224017+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.12632","created_at":"2026-07-05T00:36:38.224017+00:00"},{"alias_kind":"pith_short_12","alias_value":"LVOQN6ICNMWL","created_at":"2026-07-05T00:36:38.224017+00:00"},{"alias_kind":"pith_short_16","alias_value":"LVOQN6ICNMWLZ4LR","created_at":"2026-07-05T00:36:38.224017+00:00"},{"alias_kind":"pith_short_8","alias_value":"LVOQN6IC","created_at":"2026-07-05T00:36:38.224017+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":68,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC","json":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC.json","graph_json":"https://pith.science/api/pith-number/LVOQN6ICNMWLZ4LRI2JBMCBMYC/graph.json","events_json":"https://pith.science/api/pith-number/LVOQN6ICNMWLZ4LRI2JBMCBMYC/events.json","paper":"https://pith.science/paper/LVOQN6IC"},"agent_actions":{"view_html":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC","download_json":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC.json","view_paper":"https://pith.science/paper/LVOQN6IC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1909.12632&json=true","fetch_graph":"https://pith.science/api/pith-number/LVOQN6ICNMWLZ4LRI2JBMCBMYC/graph.json","fetch_events":"https://pith.science/api/pith-number/LVOQN6ICNMWLZ4LRI2JBMCBMYC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC/action/storage_attestation","attest_author":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC/action/author_attestation","sign_citation":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC/action/citation_signature","submit_replication":"https://pith.science/pith/LVOQN6ICNMWLZ4LRI2JBMCBMYC/action/replication_record"}},"created_at":"2026-07-05T00:36:38.224017+00:00","updated_at":"2026-07-05T00:36:38.224017+00:00"}