{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:AHCNQUWNQAZRLZHU4ASRTWTK66","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"e5fc7cddcf94f69755b1ee0f05de88f3fb45f88902f158a68cfd2eed9fef6165","cross_cats_sorted":["math.AP","math.DS","math.MP","nlin.PS","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-07-02T01:08:50Z","title_canon_sha256":"ba30e10dffd328db24d7688b170cc83f252dad7d0aa040b641e8dc73ed21b48b"},"schema_version":"1.0","source":{"id":"1807.00426","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.00426","created_at":"2026-05-18T00:11:54Z"},{"alias_kind":"arxiv_version","alias_value":"1807.00426v1","created_at":"2026-05-18T00:11:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.00426","created_at":"2026-05-18T00:11:54Z"},{"alias_kind":"pith_short_12","alias_value":"AHCNQUWNQAZR","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_16","alias_value":"AHCNQUWNQAZRLZHU","created_at":"2026-05-18T12:32:13Z"},{"alias_kind":"pith_short_8","alias_value":"AHCNQUWN","created_at":"2026-05-18T12:32:13Z"}],"graph_snapshots":[{"event_id":"sha256:b2f37e082f2eae54229b6dd9893f295e36334e77f89507d891c45c5623024085","target":"graph","created_at":"2026-05-18T00:11:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We consider the resonant system of amplitude equations for the conformally invariant cubic wave equation on the three-sphere. Using the local bifurcation theory, we characterize all stationary states that bifurcate from the first two eigenmodes. Thanks to the variational formulation of the resonant system and energy conservation, we also determine variational characterization and stability of the bifurcating states. For the lowest eigenmode, we obtain two orbitally stable families of the bifurcating stationary states: one is a constrained maximizer of energy and the other one is a constrained ","authors_text":"D.E. Pelinovsky, D. Hunik-Kostyra, P. Bizon","cross_cats":["math.AP","math.DS","math.MP","nlin.PS","nlin.SI"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-07-02T01:08:50Z","title":"Stationary states of the cubic conformal flow on $\\mathbb{S}^3$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.00426","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:b0ce4c4ecbf396fa9681163ff8e0e9ef7d3a97b3812f77f10a523d959ebb0334","target":"record","created_at":"2026-05-18T00:11:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"e5fc7cddcf94f69755b1ee0f05de88f3fb45f88902f158a68cfd2eed9fef6165","cross_cats_sorted":["math.AP","math.DS","math.MP","nlin.PS","nlin.SI"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2018-07-02T01:08:50Z","title_canon_sha256":"ba30e10dffd328db24d7688b170cc83f252dad7d0aa040b641e8dc73ed21b48b"},"schema_version":"1.0","source":{"id":"1807.00426","kind":"arxiv","version":1}},"canonical_sha256":"01c4d852cd803315e4f4e02519da6af7970d7912db86a334568f16e65da625f3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"01c4d852cd803315e4f4e02519da6af7970d7912db86a334568f16e65da625f3","first_computed_at":"2026-05-18T00:11:54.914012Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:11:54.914012Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AjjH6DGn5AR3dlbW1DOovI66Oo9Rf5rvBNYMSmbIq59j5egs1ygdwKvzZlLCyriS9Ux7Rbtmjq40tifOGu9QCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:11:54.914768Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.00426","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b0ce4c4ecbf396fa9681163ff8e0e9ef7d3a97b3812f77f10a523d959ebb0334","sha256:b2f37e082f2eae54229b6dd9893f295e36334e77f89507d891c45c5623024085"],"state_sha256":"72b9942cfcb6c27d39ac1c313f8238b906e0429578d611fe8b33a7b4e32f969c"}