{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:OAR32PQWDQ5MK7SLMYFVR2E25D","short_pith_number":"pith:OAR32PQW","canonical_record":{"source":{"id":"physics/0401013","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.comp-ph","submitted_at":"2004-01-06T14:04:53Z","cross_cats_sorted":[],"title_canon_sha256":"fd1cbbe5b383c0a932689454cd33fe035b149543b76d207816ca779776c019f0","abstract_canon_sha256":"f38f8d13a94c6089420f6b971c1c67b8786dc3ed5526a2c2bc052f19e415faf2"},"schema_version":"1.0"},"canonical_sha256":"7023bd3e161c3ac57e4b660b58e89ae8efc1a2899b694aff70a7735cb77fcf20","source":{"kind":"arxiv","id":"physics/0401013","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0401013","created_at":"2026-05-18T01:38:08Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0401013v1","created_at":"2026-05-18T01:38:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0401013","created_at":"2026-05-18T01:38:08Z"},{"alias_kind":"pith_short_12","alias_value":"OAR32PQWDQ5M","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"OAR32PQWDQ5MK7SL","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"OAR32PQW","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:OAR32PQWDQ5MK7SLMYFVR2E25D","target":"record","payload":{"canonical_record":{"source":{"id":"physics/0401013","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.comp-ph","submitted_at":"2004-01-06T14:04:53Z","cross_cats_sorted":[],"title_canon_sha256":"fd1cbbe5b383c0a932689454cd33fe035b149543b76d207816ca779776c019f0","abstract_canon_sha256":"f38f8d13a94c6089420f6b971c1c67b8786dc3ed5526a2c2bc052f19e415faf2"},"schema_version":"1.0"},"canonical_sha256":"7023bd3e161c3ac57e4b660b58e89ae8efc1a2899b694aff70a7735cb77fcf20","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:08.573652Z","signature_b64":"sSsIc5lu61a28tKP3ucA4bnJ6IVYR1v0M2Jk/QI4Fdd+jybyAcI7uIn/zEvkfbkxkG7XL78pKQMhIDgTkf+dBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7023bd3e161c3ac57e4b660b58e89ae8efc1a2899b694aff70a7735cb77fcf20","last_reissued_at":"2026-05-18T01:38:08.572999Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:08.572999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"physics/0401013","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":"2026-05-18T01:38:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3VzIrEx+Vr2guKo0cTJM49tn1OBMqYJQXy4gU7da5856/wUIzhspwM1WQ+HU7YXUjDOavVuCpeYcrLHRChuzDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T22:23:48.396444Z"},"content_sha256":"bfbbe86868c770f5f0bb3278459dae0efea0caa6c1aa0b59fb2334b49b046f9d","schema_version":"1.0","event_id":"sha256:bfbbe86868c770f5f0bb3278459dae0efea0caa6c1aa0b59fb2334b49b046f9d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:OAR32PQWDQ5MK7SLMYFVR2E25D","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Existence of Dynamical Scaling in the Temporal Signal of Time Projection Chamber","license":"","headline":"","cross_cats":[],"primary_cat":"physics.comp-ph","authors_text":"A. K. Mohanty, D. Favretto, F. Carminati, K. Safarik","submitted_at":"2004-01-06T14:04:53Z","abstract_excerpt":"The temporal signals from a large gas detector may show dynamical scaling due to many correlated space points created by the charged particles while passing through the tracking medium. This has been demonstrated through simulation using realistic parameters of a Time Projection Chamber (TPC) being fabricated to be used in ALICE collider experiment at CERN. An interesting aspect of this dynamical behavior is the existence of an universal scaling which does not depend on the multiplicity of the collision. This aspect can be utilised further to study physics at the device level and also for the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0401013","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":"2026-05-18T01:38:08Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TCqLQpYLbaPlN91UgOESkJE6FIz356boO2xF8+2EUHg9A/Ley/A59N20MZSt/qSvjdcZkc9+RnVeUG/YbmFxBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T22:23:48.397102Z"},"content_sha256":"47b3d057ee4571f0dfef0c28555da3341fccf4d3d434bc2beaf86e9787ae684b","schema_version":"1.0","event_id":"sha256:47b3d057ee4571f0dfef0c28555da3341fccf4d3d434bc2beaf86e9787ae684b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OAR32PQWDQ5MK7SLMYFVR2E25D/bundle.json","state_url":"https://pith.science/pith/OAR32PQWDQ5MK7SLMYFVR2E25D/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OAR32PQWDQ5MK7SLMYFVR2E25D/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":"2026-05-30T22:23:48Z","links":{"resolver":"https://pith.science/pith/OAR32PQWDQ5MK7SLMYFVR2E25D","bundle":"https://pith.science/pith/OAR32PQWDQ5MK7SLMYFVR2E25D/bundle.json","state":"https://pith.science/pith/OAR32PQWDQ5MK7SLMYFVR2E25D/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OAR32PQWDQ5MK7SLMYFVR2E25D/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:OAR32PQWDQ5MK7SLMYFVR2E25D","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":"f38f8d13a94c6089420f6b971c1c67b8786dc3ed5526a2c2bc052f19e415faf2","cross_cats_sorted":[],"license":"","primary_cat":"physics.comp-ph","submitted_at":"2004-01-06T14:04:53Z","title_canon_sha256":"fd1cbbe5b383c0a932689454cd33fe035b149543b76d207816ca779776c019f0"},"schema_version":"1.0","source":{"id":"physics/0401013","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"physics/0401013","created_at":"2026-05-18T01:38:08Z"},{"alias_kind":"arxiv_version","alias_value":"physics/0401013v1","created_at":"2026-05-18T01:38:08Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.physics/0401013","created_at":"2026-05-18T01:38:08Z"},{"alias_kind":"pith_short_12","alias_value":"OAR32PQWDQ5M","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"OAR32PQWDQ5MK7SL","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"OAR32PQW","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:47b3d057ee4571f0dfef0c28555da3341fccf4d3d434bc2beaf86e9787ae684b","target":"graph","created_at":"2026-05-18T01:38:08Z","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 temporal signals from a large gas detector may show dynamical scaling due to many correlated space points created by the charged particles while passing through the tracking medium. This has been demonstrated through simulation using realistic parameters of a Time Projection Chamber (TPC) being fabricated to be used in ALICE collider experiment at CERN. An interesting aspect of this dynamical behavior is the existence of an universal scaling which does not depend on the multiplicity of the collision. This aspect can be utilised further to study physics at the device level and also for the ","authors_text":"A. K. Mohanty, D. Favretto, F. Carminati, K. Safarik","cross_cats":[],"headline":"","license":"","primary_cat":"physics.comp-ph","submitted_at":"2004-01-06T14:04:53Z","title":"Existence of Dynamical Scaling in the Temporal Signal of Time Projection Chamber"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"physics/0401013","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:bfbbe86868c770f5f0bb3278459dae0efea0caa6c1aa0b59fb2334b49b046f9d","target":"record","created_at":"2026-05-18T01:38:08Z","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":"f38f8d13a94c6089420f6b971c1c67b8786dc3ed5526a2c2bc052f19e415faf2","cross_cats_sorted":[],"license":"","primary_cat":"physics.comp-ph","submitted_at":"2004-01-06T14:04:53Z","title_canon_sha256":"fd1cbbe5b383c0a932689454cd33fe035b149543b76d207816ca779776c019f0"},"schema_version":"1.0","source":{"id":"physics/0401013","kind":"arxiv","version":1}},"canonical_sha256":"7023bd3e161c3ac57e4b660b58e89ae8efc1a2899b694aff70a7735cb77fcf20","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7023bd3e161c3ac57e4b660b58e89ae8efc1a2899b694aff70a7735cb77fcf20","first_computed_at":"2026-05-18T01:38:08.572999Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:38:08.572999Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sSsIc5lu61a28tKP3ucA4bnJ6IVYR1v0M2Jk/QI4Fdd+jybyAcI7uIn/zEvkfbkxkG7XL78pKQMhIDgTkf+dBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:38:08.573652Z","signed_message":"canonical_sha256_bytes"},"source_id":"physics/0401013","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bfbbe86868c770f5f0bb3278459dae0efea0caa6c1aa0b59fb2334b49b046f9d","sha256:47b3d057ee4571f0dfef0c28555da3341fccf4d3d434bc2beaf86e9787ae684b"],"state_sha256":"a963270b3d2d55c0393113cafac0703d39e74f111ae871e598f5c45128eb3016"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q7Y1V5xMcVGOvdOGQzQd8bLRoQQ38HG7yooopFduDXJkOLGNdA9DKHwJdiEQaFCVKratCckczWF34zEc6d7PDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T22:23:48.400468Z","bundle_sha256":"0c233c6fb2ec49b6f4c2b92c5371c7afc7d943b98c789f0a02e9eb9f7965413c"}}