{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:RHSXU53GOYZLHKT664T4UGKWE6","short_pith_number":"pith:RHSXU53G","canonical_record":{"source":{"id":"1402.4630","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"math.FA","submitted_at":"2014-02-19T11:58:44Z","cross_cats_sorted":[],"title_canon_sha256":"734d1a2340c2def8d89cdbdcbf48bc5ddd24192763e55f72c98316d8fb084dc6","abstract_canon_sha256":"2df527529eb85617cd7003a52ca881d0439aa1a1385c8c5f91335c20b643cc04"},"schema_version":"1.0"},"canonical_sha256":"89e57a77667632b3aa7ef727ca19562784cf422a165a24b42bcf312623628e33","source":{"kind":"arxiv","id":"1402.4630","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.4630","created_at":"2026-05-18T02:58:33Z"},{"alias_kind":"arxiv_version","alias_value":"1402.4630v1","created_at":"2026-05-18T02:58:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4630","created_at":"2026-05-18T02:58:33Z"},{"alias_kind":"pith_short_12","alias_value":"RHSXU53GOYZL","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RHSXU53GOYZLHKT6","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RHSXU53G","created_at":"2026-05-18T12:28:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:RHSXU53GOYZLHKT664T4UGKWE6","target":"record","payload":{"canonical_record":{"source":{"id":"1402.4630","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"math.FA","submitted_at":"2014-02-19T11:58:44Z","cross_cats_sorted":[],"title_canon_sha256":"734d1a2340c2def8d89cdbdcbf48bc5ddd24192763e55f72c98316d8fb084dc6","abstract_canon_sha256":"2df527529eb85617cd7003a52ca881d0439aa1a1385c8c5f91335c20b643cc04"},"schema_version":"1.0"},"canonical_sha256":"89e57a77667632b3aa7ef727ca19562784cf422a165a24b42bcf312623628e33","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:58:33.609466Z","signature_b64":"ZtwuvK4PMdgov1ItCagQWlz10fKcYrA0uBnSVIpN0pf3lbjQpbyuN7C22Ss4Q9IO2GD6OiuT4Ivk9BN12+crAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"89e57a77667632b3aa7ef727ca19562784cf422a165a24b42bcf312623628e33","last_reissued_at":"2026-05-18T02:58:33.608702Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:58:33.608702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.4630","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:58:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X7iuGOXCN8eie68b6NX4pRzRxRfGWLsuF6V9HogObVz6StrDHUKxog5VvBSyVPliIorfRvzLrkWxWhV4nTCdDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T15:39:40.529615Z"},"content_sha256":"b27c04649e6b240768bcb811aeeaece0486443d30a4aef065399e82f9677d903","schema_version":"1.0","event_id":"sha256:b27c04649e6b240768bcb811aeeaece0486443d30a4aef065399e82f9677d903"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:RHSXU53GOYZLHKT664T4UGKWE6","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"New Periodic Solutions for Second Order Hamiltonian Systems with Local Lipschitz Potentials","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":[],"primary_cat":"math.FA","authors_text":"Li Bingyu, Li Fengying, Zhang Shiqing","submitted_at":"2014-02-19T11:58:44Z","abstract_excerpt":"Firstly,we generalize the classical Palais-Smale-Cerami condition for $C^1$ functional to the local Lipschitz case,then generalize the famous Benci-Rabinowitz's and Rabinowitz's Saddle Point Theorems with classical Cerami-Palais-Smale condition to the local Lipschitz functional, then we apply these Theorems to study the existence of new periodic solutions for second order Hamiltonian systems with local Lipschitz potentials which are weaker than Rabinowitz's original conditions .The key point of our proof is proving Cerami-Palais-Smale condition for local Lipschitz case,which is difficult since"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4630","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:58:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z8CD1d7sSr+iEYBSO7TcDi45gRsnaK+x4L3+as92KJhhjRu3U1KasM8qyzxpyvZfM+PoRWQwgOVKoPFQdza7BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T15:39:40.530094Z"},"content_sha256":"beaef572e75a0decd5bdb0b73167afb015bbed1e595a6f4ad3fb8dd2863edaae","schema_version":"1.0","event_id":"sha256:beaef572e75a0decd5bdb0b73167afb015bbed1e595a6f4ad3fb8dd2863edaae"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RHSXU53GOYZLHKT664T4UGKWE6/bundle.json","state_url":"https://pith.science/pith/RHSXU53GOYZLHKT664T4UGKWE6/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RHSXU53GOYZLHKT664T4UGKWE6/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-12T15:39:40Z","links":{"resolver":"https://pith.science/pith/RHSXU53GOYZLHKT664T4UGKWE6","bundle":"https://pith.science/pith/RHSXU53GOYZLHKT664T4UGKWE6/bundle.json","state":"https://pith.science/pith/RHSXU53GOYZLHKT664T4UGKWE6/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RHSXU53GOYZLHKT664T4UGKWE6/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:RHSXU53GOYZLHKT664T4UGKWE6","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":"2df527529eb85617cd7003a52ca881d0439aa1a1385c8c5f91335c20b643cc04","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"math.FA","submitted_at":"2014-02-19T11:58:44Z","title_canon_sha256":"734d1a2340c2def8d89cdbdcbf48bc5ddd24192763e55f72c98316d8fb084dc6"},"schema_version":"1.0","source":{"id":"1402.4630","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.4630","created_at":"2026-05-18T02:58:33Z"},{"alias_kind":"arxiv_version","alias_value":"1402.4630v1","created_at":"2026-05-18T02:58:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4630","created_at":"2026-05-18T02:58:33Z"},{"alias_kind":"pith_short_12","alias_value":"RHSXU53GOYZL","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_16","alias_value":"RHSXU53GOYZLHKT6","created_at":"2026-05-18T12:28:46Z"},{"alias_kind":"pith_short_8","alias_value":"RHSXU53G","created_at":"2026-05-18T12:28:46Z"}],"graph_snapshots":[{"event_id":"sha256:beaef572e75a0decd5bdb0b73167afb015bbed1e595a6f4ad3fb8dd2863edaae","target":"graph","created_at":"2026-05-18T02:58:33Z","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":"Firstly,we generalize the classical Palais-Smale-Cerami condition for $C^1$ functional to the local Lipschitz case,then generalize the famous Benci-Rabinowitz's and Rabinowitz's Saddle Point Theorems with classical Cerami-Palais-Smale condition to the local Lipschitz functional, then we apply these Theorems to study the existence of new periodic solutions for second order Hamiltonian systems with local Lipschitz potentials which are weaker than Rabinowitz's original conditions .The key point of our proof is proving Cerami-Palais-Smale condition for local Lipschitz case,which is difficult since","authors_text":"Li Bingyu, Li Fengying, Zhang Shiqing","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"math.FA","submitted_at":"2014-02-19T11:58:44Z","title":"New Periodic Solutions for Second Order Hamiltonian Systems with Local Lipschitz Potentials"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4630","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:b27c04649e6b240768bcb811aeeaece0486443d30a4aef065399e82f9677d903","target":"record","created_at":"2026-05-18T02:58:33Z","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":"2df527529eb85617cd7003a52ca881d0439aa1a1385c8c5f91335c20b643cc04","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"math.FA","submitted_at":"2014-02-19T11:58:44Z","title_canon_sha256":"734d1a2340c2def8d89cdbdcbf48bc5ddd24192763e55f72c98316d8fb084dc6"},"schema_version":"1.0","source":{"id":"1402.4630","kind":"arxiv","version":1}},"canonical_sha256":"89e57a77667632b3aa7ef727ca19562784cf422a165a24b42bcf312623628e33","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"89e57a77667632b3aa7ef727ca19562784cf422a165a24b42bcf312623628e33","first_computed_at":"2026-05-18T02:58:33.608702Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:58:33.608702Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ZtwuvK4PMdgov1ItCagQWlz10fKcYrA0uBnSVIpN0pf3lbjQpbyuN7C22Ss4Q9IO2GD6OiuT4Ivk9BN12+crAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:58:33.609466Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.4630","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b27c04649e6b240768bcb811aeeaece0486443d30a4aef065399e82f9677d903","sha256:beaef572e75a0decd5bdb0b73167afb015bbed1e595a6f4ad3fb8dd2863edaae"],"state_sha256":"f24693515789537027a5d975a08d4321405a601f7440c80baf7efe89e4738482"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KoLHWH2hOpOyGJO/QvYKovjr12JwVsUG1XoZNCcss4Bfw7UghFMm39klBBniu2mFOMGxzAcfOzrUJsZr9ukuDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T15:39:40.534364Z","bundle_sha256":"3bd148d768b43df449d2bdc72413ce4d093d9df4fc2f26ad54570335086e6cd3"}}