{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:M3TR5RF2P6V2M5672HG6UKAFBF","short_pith_number":"pith:M3TR5RF2","schema_version":"1.0","canonical_sha256":"66e71ec4ba7faba677dfd1cdea28050969608e2a41dd182b946ff5ea6f8ae5df","source":{"kind":"arxiv","id":"hep-th/0606126","version":2},"attestation_state":"computed","paper":{"title":"Finite-size Effects from Giant Magnons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gleb Arutyunov, Marija Zamaklar, Sergey Frolov","submitted_at":"2006-06-14T16:48:06Z","abstract_excerpt":"In order to analyze finite-size effects for the gauge-fixed string sigma model on AdS_5 x S^5, we construct one-soliton solutions carrying finite angular momentum J. In the infinite J limit the solutions reduce to the recently constructed one-magnon configuration of Hofman and Maldacena. The solutions do not satisfy the level-matching condition and hence exhibit a dependence on the gauge choice, which however disappears as the size J is taken to infinity. Interestingly, the solutions do not conserve all the global charges of the psu(2,2|4) algebra of the sigma model, implying that the symmetry"},"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":"hep-th/0606126","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-06-14T16:48:06Z","cross_cats_sorted":[],"title_canon_sha256":"5ab5f2627baffb9d659c6510a67c6932630cd7813b789331cc19fc0b02d5c602","abstract_canon_sha256":"fae670f90f113802dd28282bf0901c73527ce2b3b64b184d17688473c7511e05"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:22:40.222762Z","signature_b64":"gUfKqKTiSAKb4Pp4LhBBtNFTXpER6iIFNS79J7c5r7f/J7DJhIk+K278vkj7a0ZgweBDDWbEDP6LugjFH17BBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66e71ec4ba7faba677dfd1cdea28050969608e2a41dd182b946ff5ea6f8ae5df","last_reissued_at":"2026-07-04T15:22:40.222331Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:22:40.222331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite-size Effects from Giant Magnons","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gleb Arutyunov, Marija Zamaklar, Sergey Frolov","submitted_at":"2006-06-14T16:48:06Z","abstract_excerpt":"In order to analyze finite-size effects for the gauge-fixed string sigma model on AdS_5 x S^5, we construct one-soliton solutions carrying finite angular momentum J. In the infinite J limit the solutions reduce to the recently constructed one-magnon configuration of Hofman and Maldacena. The solutions do not satisfy the level-matching condition and hence exhibit a dependence on the gauge choice, which however disappears as the size J is taken to infinity. Interestingly, the solutions do not conserve all the global charges of the psu(2,2|4) algebra of the sigma model, implying that the symmetry"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0606126","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0606126/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":"hep-th/0606126","created_at":"2026-07-04T15:22:40.222399+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0606126v2","created_at":"2026-07-04T15:22:40.222399+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0606126","created_at":"2026-07-04T15:22:40.222399+00:00"},{"alias_kind":"pith_short_12","alias_value":"M3TR5RF2P6V2","created_at":"2026-07-04T15:22:40.222399+00:00"},{"alias_kind":"pith_short_16","alias_value":"M3TR5RF2P6V2M567","created_at":"2026-07-04T15:22:40.222399+00:00"},{"alias_kind":"pith_short_8","alias_value":"M3TR5RF2","created_at":"2026-07-04T15:22:40.222399+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.08411","citing_title":"Particle production in a light-cone gauge fixed Jordanian deformation of $AdS_5\\times S^5$","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF","json":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF.json","graph_json":"https://pith.science/api/pith-number/M3TR5RF2P6V2M5672HG6UKAFBF/graph.json","events_json":"https://pith.science/api/pith-number/M3TR5RF2P6V2M5672HG6UKAFBF/events.json","paper":"https://pith.science/paper/M3TR5RF2"},"agent_actions":{"view_html":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF","download_json":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF.json","view_paper":"https://pith.science/paper/M3TR5RF2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0606126&json=true","fetch_graph":"https://pith.science/api/pith-number/M3TR5RF2P6V2M5672HG6UKAFBF/graph.json","fetch_events":"https://pith.science/api/pith-number/M3TR5RF2P6V2M5672HG6UKAFBF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF/action/storage_attestation","attest_author":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF/action/author_attestation","sign_citation":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF/action/citation_signature","submit_replication":"https://pith.science/pith/M3TR5RF2P6V2M5672HG6UKAFBF/action/replication_record"}},"created_at":"2026-07-04T15:22:40.222399+00:00","updated_at":"2026-07-04T15:22:40.222399+00:00"}