{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:XTYN7S7AIQMR6UAXBNZ33USYNU","short_pith_number":"pith:XTYN7S7A","canonical_record":{"source":{"id":"1403.2477","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2014-03-11T05:14:16Z","cross_cats_sorted":[],"title_canon_sha256":"664a2f4ce744896e9d5617cd0b3ac5f71004a730db86cab2c95c9bd79d45b829","abstract_canon_sha256":"36e5c0dbaad45b5319488851576ef8a93cc8c68d52b7075ff2dbea25790d0aec"},"schema_version":"1.0"},"canonical_sha256":"bcf0dfcbe044191f50170b73bdd2586d246a95e7d5cd152b5e0233de55992968","source":{"kind":"arxiv","id":"1403.2477","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2477","created_at":"2026-05-18T01:55:34Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2477v2","created_at":"2026-05-18T01:55:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2477","created_at":"2026-05-18T01:55:34Z"},{"alias_kind":"pith_short_12","alias_value":"XTYN7S7AIQMR","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"XTYN7S7AIQMR6UAX","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"XTYN7S7A","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:XTYN7S7AIQMR6UAXBNZ33USYNU","target":"record","payload":{"canonical_record":{"source":{"id":"1403.2477","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2014-03-11T05:14:16Z","cross_cats_sorted":[],"title_canon_sha256":"664a2f4ce744896e9d5617cd0b3ac5f71004a730db86cab2c95c9bd79d45b829","abstract_canon_sha256":"36e5c0dbaad45b5319488851576ef8a93cc8c68d52b7075ff2dbea25790d0aec"},"schema_version":"1.0"},"canonical_sha256":"bcf0dfcbe044191f50170b73bdd2586d246a95e7d5cd152b5e0233de55992968","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:55:34.012707Z","signature_b64":"dJxBPojiZeiRAWkR4KQ4kBZgvz6pTNZIOZX1j0utNWNKSP2Ikl3nwy9s4Yg32J8CwcdMvcD1iwAVQv3K7EUmBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bcf0dfcbe044191f50170b73bdd2586d246a95e7d5cd152b5e0233de55992968","last_reissued_at":"2026-05-18T01:55:34.012125Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:55:34.012125Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.2477","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:55:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wevRHOUou1Fl//qkBBvlh4hrSm1OjtXHNtyDWd63yyXyZbegrvnloBUrOqmCRkKg6jnOXtSF7eybXmp5dRDRCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T10:24:00.160757Z"},"content_sha256":"75e0b3c4314a983442011e8e6f48dad348b2d3eca0f29bc92969e9e64c41205f","schema_version":"1.0","event_id":"sha256:75e0b3c4314a983442011e8e6f48dad348b2d3eca0f29bc92969e9e64c41205f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:XTYN7S7AIQMR6UAXBNZ33USYNU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the role of electrodynamic interactions in long-distance biomolecular recognition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.bio-ph","authors_text":"Jack A. Tuszynski, Jordane Preto, Marco Pettini","submitted_at":"2014-03-11T05:14:16Z","abstract_excerpt":"The issue of retarded long-range resonant interactions between two molecules with oscillating dipole moments is reinvestigated within the framework of classical electrodynamics. By taking advantage of a theorem in complex analysis, we present a simple method to calculate the frequencies of the normal modes, which are then used to estimate the interaction potential. The main results thus found are in perfect agreement with several results obtained from quantum computations. Moreover, when applied in a biophysical context, our findings shed new light on Frohlich's theory of selective long-range"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2477","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":""},"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":"2026-05-18T01:55:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KMWuTUCbwMG9mRy8NkSrdTelkFiJ/NIvIuJT9DnsRRvmhwlTDXmfXrTZ2OKEFZWW94CzoNzWvNz7fB70b7EpDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T10:24:00.161417Z"},"content_sha256":"29ef8b3af343cddee660b81a42f7366718c4da339805f7781142dab9aeb937ab","schema_version":"1.0","event_id":"sha256:29ef8b3af343cddee660b81a42f7366718c4da339805f7781142dab9aeb937ab"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XTYN7S7AIQMR6UAXBNZ33USYNU/bundle.json","state_url":"https://pith.science/pith/XTYN7S7AIQMR6UAXBNZ33USYNU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XTYN7S7AIQMR6UAXBNZ33USYNU/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":"2026-05-26T10:24:00Z","links":{"resolver":"https://pith.science/pith/XTYN7S7AIQMR6UAXBNZ33USYNU","bundle":"https://pith.science/pith/XTYN7S7AIQMR6UAXBNZ33USYNU/bundle.json","state":"https://pith.science/pith/XTYN7S7AIQMR6UAXBNZ33USYNU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XTYN7S7AIQMR6UAXBNZ33USYNU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:XTYN7S7AIQMR6UAXBNZ33USYNU","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":"36e5c0dbaad45b5319488851576ef8a93cc8c68d52b7075ff2dbea25790d0aec","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2014-03-11T05:14:16Z","title_canon_sha256":"664a2f4ce744896e9d5617cd0b3ac5f71004a730db86cab2c95c9bd79d45b829"},"schema_version":"1.0","source":{"id":"1403.2477","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2477","created_at":"2026-05-18T01:55:34Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2477v2","created_at":"2026-05-18T01:55:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2477","created_at":"2026-05-18T01:55:34Z"},{"alias_kind":"pith_short_12","alias_value":"XTYN7S7AIQMR","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"XTYN7S7AIQMR6UAX","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"XTYN7S7A","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:29ef8b3af343cddee660b81a42f7366718c4da339805f7781142dab9aeb937ab","target":"graph","created_at":"2026-05-18T01:55:34Z","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":"The issue of retarded long-range resonant interactions between two molecules with oscillating dipole moments is reinvestigated within the framework of classical electrodynamics. By taking advantage of a theorem in complex analysis, we present a simple method to calculate the frequencies of the normal modes, which are then used to estimate the interaction potential. The main results thus found are in perfect agreement with several results obtained from quantum computations. Moreover, when applied in a biophysical context, our findings shed new light on Frohlich's theory of selective long-range","authors_text":"Jack A. Tuszynski, Jordane Preto, Marco Pettini","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2014-03-11T05:14:16Z","title":"On the role of electrodynamic interactions in long-distance biomolecular recognition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2477","kind":"arxiv","version":2},"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":"sha256:75e0b3c4314a983442011e8e6f48dad348b2d3eca0f29bc92969e9e64c41205f","target":"record","created_at":"2026-05-18T01:55:34Z","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":"36e5c0dbaad45b5319488851576ef8a93cc8c68d52b7075ff2dbea25790d0aec","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.bio-ph","submitted_at":"2014-03-11T05:14:16Z","title_canon_sha256":"664a2f4ce744896e9d5617cd0b3ac5f71004a730db86cab2c95c9bd79d45b829"},"schema_version":"1.0","source":{"id":"1403.2477","kind":"arxiv","version":2}},"canonical_sha256":"bcf0dfcbe044191f50170b73bdd2586d246a95e7d5cd152b5e0233de55992968","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bcf0dfcbe044191f50170b73bdd2586d246a95e7d5cd152b5e0233de55992968","first_computed_at":"2026-05-18T01:55:34.012125Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:55:34.012125Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dJxBPojiZeiRAWkR4KQ4kBZgvz6pTNZIOZX1j0utNWNKSP2Ikl3nwy9s4Yg32J8CwcdMvcD1iwAVQv3K7EUmBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:55:34.012707Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.2477","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:75e0b3c4314a983442011e8e6f48dad348b2d3eca0f29bc92969e9e64c41205f","sha256:29ef8b3af343cddee660b81a42f7366718c4da339805f7781142dab9aeb937ab"],"state_sha256":"8af713fa9329e8fc2fde8cf54d467c8647aea37683581f846c7cf1a879140d19"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9w8HVNSMrR3xZwaL5WN7oQyEJFnQS/rdq+E7doYjo7fW/7bW2oNuyaqBCZ06keytUlGJSbhfeofLW9RAEKmZCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T10:24:00.164218Z","bundle_sha256":"002af96acd239a052a1d94a97b1d02acd5020b987579dbd2d184c7c503f19ba4"}}