{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:XNRXAKXK2XMXGYS23HIWTVNQM7","short_pith_number":"pith:XNRXAKXK","canonical_record":{"source":{"id":"1112.1079","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-12-05T21:00:58Z","cross_cats_sorted":[],"title_canon_sha256":"43a057dba3e621546d7ebc2399fec0de5e8df6e2faff03a0f5e56fec8209a397","abstract_canon_sha256":"1d6d7091072d3dcbf74c2be29310a19dc9993e0d27dde674a562b09a36239950"},"schema_version":"1.0"},"canonical_sha256":"bb63702aead5d973625ad9d169d5b067f8dae6e5fa0682dc91f094c3bb9fa765","source":{"kind":"arxiv","id":"1112.1079","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.1079","created_at":"2026-05-18T03:05:44Z"},{"alias_kind":"arxiv_version","alias_value":"1112.1079v3","created_at":"2026-05-18T03:05:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.1079","created_at":"2026-05-18T03:05:44Z"},{"alias_kind":"pith_short_12","alias_value":"XNRXAKXK2XMX","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"XNRXAKXK2XMXGYS2","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"XNRXAKXK","created_at":"2026-05-18T12:26:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:XNRXAKXK2XMXGYS23HIWTVNQM7","target":"record","payload":{"canonical_record":{"source":{"id":"1112.1079","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-12-05T21:00:58Z","cross_cats_sorted":[],"title_canon_sha256":"43a057dba3e621546d7ebc2399fec0de5e8df6e2faff03a0f5e56fec8209a397","abstract_canon_sha256":"1d6d7091072d3dcbf74c2be29310a19dc9993e0d27dde674a562b09a36239950"},"schema_version":"1.0"},"canonical_sha256":"bb63702aead5d973625ad9d169d5b067f8dae6e5fa0682dc91f094c3bb9fa765","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:05:44.963249Z","signature_b64":"9O0kKHYK4U3mqXX0jocLbli5lAU+jLrX6k6SMg5h1fjrrrhBEdFztNH9WtWeQjoLxcAOtYoL0OuHGTDvtKA7Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb63702aead5d973625ad9d169d5b067f8dae6e5fa0682dc91f094c3bb9fa765","last_reissued_at":"2026-05-18T03:05:44.962661Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:05:44.962661Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.1079","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:05:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qpl9/s4o2B2IFU2fKanmH2v80sFDIMewKyyLAdrHkW6lmnHB6RHUIG/XFJfZtPchDd+y63KKe/NQkGw0suxQDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T17:53:04.634338Z"},"content_sha256":"37654601c991b772ebe67980cc6f6036ecbe49eb71f05cae84ad583c78179d7f","schema_version":"1.0","event_id":"sha256:37654601c991b772ebe67980cc6f6036ecbe49eb71f05cae84ad583c78179d7f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:XNRXAKXK2XMXGYS23HIWTVNQM7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Linear response theory for long-range interacting systems in quasistationary states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Aurelio Patelli, Cesare Nardini, Shamik Gupta, Stefano Ruffo","submitted_at":"2011-12-05T21:00:58Z","abstract_excerpt":"Long-range interacting systems, while relaxing to equilibrium, often get trapped in long-lived quasistationary states which have lifetimes that diverge with the system size. In this work, we address the question of how a long-range system in a quasistationary state (QSS) responds to an external perturbation. We consider a long-range system that evolves under deterministic Hamilton dynamics. The perturbation is taken to couple to the canonical coordinates of the individual constituents. Our study is based on analyzing the Vlasov equation for the single-particle phase space distribution. The QSS"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.1079","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":""},"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":"2026-05-18T03:05:44Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bM4m/9VVXAjmybuRB1DHYp7ajIgLD477Shymf2Cb2fYoCiGLoW/Bf69ovY/IeHYItOkgHZNuh9kyv0EOyM70Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-22T17:53:04.634685Z"},"content_sha256":"9b50bbcb5a7feb5e941cbf49629eb8cc8cb629f323a8189a42a4ebc4ddc4d76b","schema_version":"1.0","event_id":"sha256:9b50bbcb5a7feb5e941cbf49629eb8cc8cb629f323a8189a42a4ebc4ddc4d76b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XNRXAKXK2XMXGYS23HIWTVNQM7/bundle.json","state_url":"https://pith.science/pith/XNRXAKXK2XMXGYS23HIWTVNQM7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XNRXAKXK2XMXGYS23HIWTVNQM7/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":"2026-06-22T17:53:04Z","links":{"resolver":"https://pith.science/pith/XNRXAKXK2XMXGYS23HIWTVNQM7","bundle":"https://pith.science/pith/XNRXAKXK2XMXGYS23HIWTVNQM7/bundle.json","state":"https://pith.science/pith/XNRXAKXK2XMXGYS23HIWTVNQM7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XNRXAKXK2XMXGYS23HIWTVNQM7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:XNRXAKXK2XMXGYS23HIWTVNQM7","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":"1d6d7091072d3dcbf74c2be29310a19dc9993e0d27dde674a562b09a36239950","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-12-05T21:00:58Z","title_canon_sha256":"43a057dba3e621546d7ebc2399fec0de5e8df6e2faff03a0f5e56fec8209a397"},"schema_version":"1.0","source":{"id":"1112.1079","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.1079","created_at":"2026-05-18T03:05:44Z"},{"alias_kind":"arxiv_version","alias_value":"1112.1079v3","created_at":"2026-05-18T03:05:44Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.1079","created_at":"2026-05-18T03:05:44Z"},{"alias_kind":"pith_short_12","alias_value":"XNRXAKXK2XMX","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_16","alias_value":"XNRXAKXK2XMXGYS2","created_at":"2026-05-18T12:26:47Z"},{"alias_kind":"pith_short_8","alias_value":"XNRXAKXK","created_at":"2026-05-18T12:26:47Z"}],"graph_snapshots":[{"event_id":"sha256:9b50bbcb5a7feb5e941cbf49629eb8cc8cb629f323a8189a42a4ebc4ddc4d76b","target":"graph","created_at":"2026-05-18T03:05:44Z","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":"Long-range interacting systems, while relaxing to equilibrium, often get trapped in long-lived quasistationary states which have lifetimes that diverge with the system size. In this work, we address the question of how a long-range system in a quasistationary state (QSS) responds to an external perturbation. We consider a long-range system that evolves under deterministic Hamilton dynamics. The perturbation is taken to couple to the canonical coordinates of the individual constituents. Our study is based on analyzing the Vlasov equation for the single-particle phase space distribution. The QSS","authors_text":"Aurelio Patelli, Cesare Nardini, Shamik Gupta, Stefano Ruffo","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-12-05T21:00:58Z","title":"Linear response theory for long-range interacting systems in quasistationary states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.1079","kind":"arxiv","version":3},"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":"sha256:37654601c991b772ebe67980cc6f6036ecbe49eb71f05cae84ad583c78179d7f","target":"record","created_at":"2026-05-18T03:05:44Z","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":"1d6d7091072d3dcbf74c2be29310a19dc9993e0d27dde674a562b09a36239950","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-12-05T21:00:58Z","title_canon_sha256":"43a057dba3e621546d7ebc2399fec0de5e8df6e2faff03a0f5e56fec8209a397"},"schema_version":"1.0","source":{"id":"1112.1079","kind":"arxiv","version":3}},"canonical_sha256":"bb63702aead5d973625ad9d169d5b067f8dae6e5fa0682dc91f094c3bb9fa765","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bb63702aead5d973625ad9d169d5b067f8dae6e5fa0682dc91f094c3bb9fa765","first_computed_at":"2026-05-18T03:05:44.962661Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:05:44.962661Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9O0kKHYK4U3mqXX0jocLbli5lAU+jLrX6k6SMg5h1fjrrrhBEdFztNH9WtWeQjoLxcAOtYoL0OuHGTDvtKA7Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:05:44.963249Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.1079","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:37654601c991b772ebe67980cc6f6036ecbe49eb71f05cae84ad583c78179d7f","sha256:9b50bbcb5a7feb5e941cbf49629eb8cc8cb629f323a8189a42a4ebc4ddc4d76b"],"state_sha256":"96f670f8c22d135489de7096fb848c84c450d58e0811366f1d8a01d22c5ab204"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Lxx/Cy3e+fPetDSLEJeSh6gIwePKwgtTqJ46vPIFz1CuSAQ0l51LE7O4iq+2Xt397I5CAXrQ5HfEH7BVbEqhAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-22T17:53:04.636658Z","bundle_sha256":"1d90e7b7722a402c030eaf06d40c80e17a6951c26b6cd94efcdbf730d330564a"}}