{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:IEOKT73UEWC7AIWDRDUJRDGTHQ","short_pith_number":"pith:IEOKT73U","canonical_record":{"source":{"id":"1112.3175","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.hist-ph","submitted_at":"2011-12-14T11:39:38Z","cross_cats_sorted":[],"title_canon_sha256":"c2a26147617fb1bf99986e0d4f82894d3fca7800d5aae40c3fcd744cb097f969","abstract_canon_sha256":"4a264a96111abe6ef37c2b88af47b37be921339cbaa98f466f225b112448af58"},"schema_version":"1.0"},"canonical_sha256":"411ca9ff742585f022c388e8988cd33c19424b5b32d25dd8f6bba1b23c0d9ba7","source":{"kind":"arxiv","id":"1112.3175","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3175","created_at":"2026-05-18T04:06:19Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3175v1","created_at":"2026-05-18T04:06:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3175","created_at":"2026-05-18T04:06:19Z"},{"alias_kind":"pith_short_12","alias_value":"IEOKT73UEWC7","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"IEOKT73UEWC7AIWD","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"IEOKT73U","created_at":"2026-05-18T12:26:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:IEOKT73UEWC7AIWDRDUJRDGTHQ","target":"record","payload":{"canonical_record":{"source":{"id":"1112.3175","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.hist-ph","submitted_at":"2011-12-14T11:39:38Z","cross_cats_sorted":[],"title_canon_sha256":"c2a26147617fb1bf99986e0d4f82894d3fca7800d5aae40c3fcd744cb097f969","abstract_canon_sha256":"4a264a96111abe6ef37c2b88af47b37be921339cbaa98f466f225b112448af58"},"schema_version":"1.0"},"canonical_sha256":"411ca9ff742585f022c388e8988cd33c19424b5b32d25dd8f6bba1b23c0d9ba7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:06:19.942229Z","signature_b64":"d2+2NEQRMuShBvNYOXKZKhDXtOFB9ZVGuqcGdnd1kE4DgMThxKnERlF3qDose95G//vlLqZ48d0ZUt4SQrMtBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"411ca9ff742585f022c388e8988cd33c19424b5b32d25dd8f6bba1b23c0d9ba7","last_reissued_at":"2026-05-18T04:06:19.941427Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:06:19.941427Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.3175","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":"2026-05-18T04:06:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i4iJGMwZlygYh+usW0PIKD+Jmbj8FGXWOfKqne9v9lGsH+zMqNb2J7QLT60YzRU9C4WDP6IamQ/1TuU8HOvKBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T23:33:59.873618Z"},"content_sha256":"8a554f20087542fe47735baedf8f5076465931a47bcb32a609026357505f8398","schema_version":"1.0","event_id":"sha256:8a554f20087542fe47735baedf8f5076465931a47bcb32a609026357505f8398"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:IEOKT73UEWC7AIWDRDUJRDGTHQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Poincare and Special Relativity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.hist-ph","authors_text":"Emily Adlam","submitted_at":"2011-12-14T11:39:38Z","abstract_excerpt":"Henri Poincare's work on mathematical features of the Lorentz transformations was an important precursor to the development of special relativity. In this paper I compare the approaches taken by Poincare and Einstein, aiming to come to an understanding of the philosophical ideas underlying their methods. In section (1) I assess Poincare's contribution, concluding that although he inspired much of the mathematical formalism of special relativity, he cannot be credited with an overall conceptual grasp of the theory. In section (2) I investigate the origins of the two approaches, tracing differen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3175","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":"2026-05-18T04:06:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ev6g04aVxRxWflyrT0WxGeNIwzN5uNsTPMgMumI9CcEJxJdJYHR5j5JDcfll5f+mbM/r/4/QRVq2g3nLMU15Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T23:33:59.874390Z"},"content_sha256":"c364c6d146abce83cb06ff44821167a3fe26376c8841865c20bf92c52726c554","schema_version":"1.0","event_id":"sha256:c364c6d146abce83cb06ff44821167a3fe26376c8841865c20bf92c52726c554"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ/bundle.json","state_url":"https://pith.science/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ/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":"2026-06-11T23:33:59Z","links":{"resolver":"https://pith.science/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ","bundle":"https://pith.science/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ/bundle.json","state":"https://pith.science/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IEOKT73UEWC7AIWDRDUJRDGTHQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:IEOKT73UEWC7AIWDRDUJRDGTHQ","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":"4a264a96111abe6ef37c2b88af47b37be921339cbaa98f466f225b112448af58","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.hist-ph","submitted_at":"2011-12-14T11:39:38Z","title_canon_sha256":"c2a26147617fb1bf99986e0d4f82894d3fca7800d5aae40c3fcd744cb097f969"},"schema_version":"1.0","source":{"id":"1112.3175","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.3175","created_at":"2026-05-18T04:06:19Z"},{"alias_kind":"arxiv_version","alias_value":"1112.3175v1","created_at":"2026-05-18T04:06:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.3175","created_at":"2026-05-18T04:06:19Z"},{"alias_kind":"pith_short_12","alias_value":"IEOKT73UEWC7","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"IEOKT73UEWC7AIWD","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"IEOKT73U","created_at":"2026-05-18T12:26:30Z"}],"graph_snapshots":[{"event_id":"sha256:c364c6d146abce83cb06ff44821167a3fe26376c8841865c20bf92c52726c554","target":"graph","created_at":"2026-05-18T04:06:19Z","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":"Henri Poincare's work on mathematical features of the Lorentz transformations was an important precursor to the development of special relativity. In this paper I compare the approaches taken by Poincare and Einstein, aiming to come to an understanding of the philosophical ideas underlying their methods. In section (1) I assess Poincare's contribution, concluding that although he inspired much of the mathematical formalism of special relativity, he cannot be credited with an overall conceptual grasp of the theory. In section (2) I investigate the origins of the two approaches, tracing differen","authors_text":"Emily Adlam","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.hist-ph","submitted_at":"2011-12-14T11:39:38Z","title":"Poincare and Special Relativity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.3175","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":"sha256:8a554f20087542fe47735baedf8f5076465931a47bcb32a609026357505f8398","target":"record","created_at":"2026-05-18T04:06:19Z","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":"4a264a96111abe6ef37c2b88af47b37be921339cbaa98f466f225b112448af58","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.hist-ph","submitted_at":"2011-12-14T11:39:38Z","title_canon_sha256":"c2a26147617fb1bf99986e0d4f82894d3fca7800d5aae40c3fcd744cb097f969"},"schema_version":"1.0","source":{"id":"1112.3175","kind":"arxiv","version":1}},"canonical_sha256":"411ca9ff742585f022c388e8988cd33c19424b5b32d25dd8f6bba1b23c0d9ba7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"411ca9ff742585f022c388e8988cd33c19424b5b32d25dd8f6bba1b23c0d9ba7","first_computed_at":"2026-05-18T04:06:19.941427Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:06:19.941427Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"d2+2NEQRMuShBvNYOXKZKhDXtOFB9ZVGuqcGdnd1kE4DgMThxKnERlF3qDose95G//vlLqZ48d0ZUt4SQrMtBw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:06:19.942229Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.3175","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8a554f20087542fe47735baedf8f5076465931a47bcb32a609026357505f8398","sha256:c364c6d146abce83cb06ff44821167a3fe26376c8841865c20bf92c52726c554"],"state_sha256":"cf95f905768dc743c3e44e760b56ed9f6c3bb87a8738da4eefaffc65c7eccffd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Q13aXB2F9rSyVGsq4ATVRc9hFCbiPz3u+kqDVa64HsNDWWlB6lA4P/d7DO5b0wxRlvHKvYW8jnUFstWx3ondCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T23:33:59.878537Z","bundle_sha256":"7e1c5bb1d4ad53fac7203899934aed0b97db57481a4f9a5eb3abea02f91d89eb"}}