{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:YDQMLU7QMFRPGBL5PKHBDSP4T3","short_pith_number":"pith:YDQMLU7Q","canonical_record":{"source":{"id":"1307.4665","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2013-07-17T15:09:23Z","cross_cats_sorted":[],"title_canon_sha256":"e54aae45a1ce2049726043b65b925eb8f3aa2ddc6dc763f5297d5438d87a3f34","abstract_canon_sha256":"03dfe35d69d84412e55511cd07be742d3cb7d5f9e335eef04d0aa87010384bae"},"schema_version":"1.0"},"canonical_sha256":"c0e0c5d3f06162f3057d7a8e11c9fc9ef10d34c728e59a585fb20d209b201555","source":{"kind":"arxiv","id":"1307.4665","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.4665","created_at":"2026-05-18T03:18:07Z"},{"alias_kind":"arxiv_version","alias_value":"1307.4665v1","created_at":"2026-05-18T03:18:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.4665","created_at":"2026-05-18T03:18:07Z"},{"alias_kind":"pith_short_12","alias_value":"YDQMLU7QMFRP","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YDQMLU7QMFRPGBL5","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YDQMLU7Q","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:YDQMLU7QMFRPGBL5PKHBDSP4T3","target":"record","payload":{"canonical_record":{"source":{"id":"1307.4665","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2013-07-17T15:09:23Z","cross_cats_sorted":[],"title_canon_sha256":"e54aae45a1ce2049726043b65b925eb8f3aa2ddc6dc763f5297d5438d87a3f34","abstract_canon_sha256":"03dfe35d69d84412e55511cd07be742d3cb7d5f9e335eef04d0aa87010384bae"},"schema_version":"1.0"},"canonical_sha256":"c0e0c5d3f06162f3057d7a8e11c9fc9ef10d34c728e59a585fb20d209b201555","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:18:07.485153Z","signature_b64":"kA4YUD4T8QH0NvGEn5klNawwTpCV/ONytaxkB7LF2itqIqZit8TL9z4J2FvQUrA1XW2OTYsxk4gSGImdSaE9CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0e0c5d3f06162f3057d7a8e11c9fc9ef10d34c728e59a585fb20d209b201555","last_reissued_at":"2026-05-18T03:18:07.484261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:18:07.484261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1307.4665","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":"2026-05-18T03:18:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wvnbokBjy6hYx9bsbqPDrUlFl9LR5GJLreIICOk3eRQfajUKNJPJ2Grl+1pCU2AIGxy4wnw2o++3nNQ5Npy+AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T09:45:43.888015Z"},"content_sha256":"b3757ac0ded87fe07089b1f99c469f77f25b530fc3b2d61bb80d541e47d41e2f","schema_version":"1.0","event_id":"sha256:b3757ac0ded87fe07089b1f99c469f77f25b530fc3b2d61bb80d541e47d41e2f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:YDQMLU7QMFRPGBL5PKHBDSP4T3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Control over multiscale systems with constraints. 3. Geometrodynamics of the evolution of systems with varying constraints","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"S. Adamenko, V. Bolotov, V. Novikov","submitted_at":"2013-07-17T15:09:23Z","abstract_excerpt":"With the use of the general variational principle of self-organization of systems with varying constraints, namely the principle of dynamical harmonization of systems presented in the first work of the cycle, we advance an approach to the control over the evolution of systems of many particles. The geometric nature of this principle is analyzed. On the basis of the de Broglie--Bohm representation of the Schr\\\"odinger equation, we establish a connection of the nonlocality and the coherence of the systems of many particles with mass entropic forces. The defining role of a coherent acceleration a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.4665","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":"2026-05-18T03:18:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+h2uT8wVEkDDfJbLZW+3DUsCGqwcHZmBvM3+v3Ao3UvpZCQOLexfY7cZbs7lnCy+Z+wuWZ5Yhy6MJVoNlSSQAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T09:45:43.888581Z"},"content_sha256":"c49065d10c41fb250a36bd4503ed0259ab12fc84eef8f106f6d47ee69620f69d","schema_version":"1.0","event_id":"sha256:c49065d10c41fb250a36bd4503ed0259ab12fc84eef8f106f6d47ee69620f69d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3/bundle.json","state_url":"https://pith.science/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3/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":"2026-06-05T09:45:43Z","links":{"resolver":"https://pith.science/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3","bundle":"https://pith.science/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3/bundle.json","state":"https://pith.science/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YDQMLU7QMFRPGBL5PKHBDSP4T3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:YDQMLU7QMFRPGBL5PKHBDSP4T3","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":"03dfe35d69d84412e55511cd07be742d3cb7d5f9e335eef04d0aa87010384bae","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2013-07-17T15:09:23Z","title_canon_sha256":"e54aae45a1ce2049726043b65b925eb8f3aa2ddc6dc763f5297d5438d87a3f34"},"schema_version":"1.0","source":{"id":"1307.4665","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.4665","created_at":"2026-05-18T03:18:07Z"},{"alias_kind":"arxiv_version","alias_value":"1307.4665v1","created_at":"2026-05-18T03:18:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.4665","created_at":"2026-05-18T03:18:07Z"},{"alias_kind":"pith_short_12","alias_value":"YDQMLU7QMFRP","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YDQMLU7QMFRPGBL5","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YDQMLU7Q","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:c49065d10c41fb250a36bd4503ed0259ab12fc84eef8f106f6d47ee69620f69d","target":"graph","created_at":"2026-05-18T03:18:07Z","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":"With the use of the general variational principle of self-organization of systems with varying constraints, namely the principle of dynamical harmonization of systems presented in the first work of the cycle, we advance an approach to the control over the evolution of systems of many particles. The geometric nature of this principle is analyzed. On the basis of the de Broglie--Bohm representation of the Schr\\\"odinger equation, we establish a connection of the nonlocality and the coherence of the systems of many particles with mass entropic forces. The defining role of a coherent acceleration a","authors_text":"S. Adamenko, V. Bolotov, V. Novikov","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2013-07-17T15:09:23Z","title":"Control over multiscale systems with constraints. 3. Geometrodynamics of the evolution of systems with varying constraints"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.4665","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:b3757ac0ded87fe07089b1f99c469f77f25b530fc3b2d61bb80d541e47d41e2f","target":"record","created_at":"2026-05-18T03:18:07Z","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":"03dfe35d69d84412e55511cd07be742d3cb7d5f9e335eef04d0aa87010384bae","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.gen-ph","submitted_at":"2013-07-17T15:09:23Z","title_canon_sha256":"e54aae45a1ce2049726043b65b925eb8f3aa2ddc6dc763f5297d5438d87a3f34"},"schema_version":"1.0","source":{"id":"1307.4665","kind":"arxiv","version":1}},"canonical_sha256":"c0e0c5d3f06162f3057d7a8e11c9fc9ef10d34c728e59a585fb20d209b201555","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c0e0c5d3f06162f3057d7a8e11c9fc9ef10d34c728e59a585fb20d209b201555","first_computed_at":"2026-05-18T03:18:07.484261Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:18:07.484261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"kA4YUD4T8QH0NvGEn5klNawwTpCV/ONytaxkB7LF2itqIqZit8TL9z4J2FvQUrA1XW2OTYsxk4gSGImdSaE9CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:18:07.485153Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.4665","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b3757ac0ded87fe07089b1f99c469f77f25b530fc3b2d61bb80d541e47d41e2f","sha256:c49065d10c41fb250a36bd4503ed0259ab12fc84eef8f106f6d47ee69620f69d"],"state_sha256":"6384989867ee3f0076028a47d227a64ef6713aa6f941f3888f43b4f780811b52"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MXb//DEbKITCkTmK13tvVlJ3HJruIMmGyWQ6wMuLLyzDQ6xLhFHkY6T8Fu6HRDvuIlm6CDopSfghQjXRP5KxDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T09:45:43.891604Z","bundle_sha256":"fa110be0cbeb120bb9fdeb085c7f786edf749b16546e6509de0845f431828baa"}}