{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:K7NGEQ66II7HD36SIUBFZHTMXE","short_pith_number":"pith:K7NGEQ66","canonical_record":{"source":{"id":"1608.01318","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-03T20:00:05Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9d6b90c39afbf13677a2c33eff54ca8c49ee2845a3997e854e10eb6190b31422","abstract_canon_sha256":"34e8f535e3a75b0d507e05e69efb64b39a084cae2d628b207e550804269db75f"},"schema_version":"1.0"},"canonical_sha256":"57da6243de423e71efd245025c9e6cb930c3e4e0c5cfbb3e762ac03f4811c93e","source":{"kind":"arxiv","id":"1608.01318","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.01318","created_at":"2026-05-18T00:55:45Z"},{"alias_kind":"arxiv_version","alias_value":"1608.01318v1","created_at":"2026-05-18T00:55:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.01318","created_at":"2026-05-18T00:55:45Z"},{"alias_kind":"pith_short_12","alias_value":"K7NGEQ66II7H","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"K7NGEQ66II7HD36S","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"K7NGEQ66","created_at":"2026-05-18T12:30:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:K7NGEQ66II7HD36SIUBFZHTMXE","target":"record","payload":{"canonical_record":{"source":{"id":"1608.01318","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-03T20:00:05Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"9d6b90c39afbf13677a2c33eff54ca8c49ee2845a3997e854e10eb6190b31422","abstract_canon_sha256":"34e8f535e3a75b0d507e05e69efb64b39a084cae2d628b207e550804269db75f"},"schema_version":"1.0"},"canonical_sha256":"57da6243de423e71efd245025c9e6cb930c3e4e0c5cfbb3e762ac03f4811c93e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:55:45.641533Z","signature_b64":"7ueqhc2yS9svIHY4XaJenjjpRn1Lw9buNnUI0LKwZJQyUsIzbjDWYzdvJuGg71K2iDoFdAoRpRG3vdwa2oaOAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"57da6243de423e71efd245025c9e6cb930c3e4e0c5cfbb3e762ac03f4811c93e","last_reissued_at":"2026-05-18T00:55:45.641023Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:55:45.641023Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.01318","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":"2026-05-18T00:55:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Zm7GXuM73j434nLNWA5qQzvseoWOpBHiJ5Bvr7C6Ek3tjAyEnEnGmsU9ZaRl1Iivq13PxWkaVx498bQ8JyO4Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T07:05:09.885660Z"},"content_sha256":"74a74960aacfc11dcf9488e415b00aa884e1e8392e27609112e79e48cc2f464b","schema_version":"1.0","event_id":"sha256:74a74960aacfc11dcf9488e415b00aa884e1e8392e27609112e79e48cc2f464b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:K7NGEQ66II7HD36SIUBFZHTMXE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Top Quark Mass Calibration for Monte Carlo Event Generators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Andre H. Hoang, Bahman Dehnadi, Iain W. Stewart, Mathias Butenschoen, Moritz Preisser, Vicent Mateu","submitted_at":"2016-08-03T20:00:05Z","abstract_excerpt":"The most precise top quark mass measurements use kinematic reconstruction methods, determining the top mass parameter of a Monte Carlo event generator, $m_t^{\\rm MC}$. Due to hadronization and parton shower dynamics, relating $m_t^{\\rm MC}$ to a field theory mass is difficult. We present a calibration procedure to determine this relation using hadron level QCD predictions for observables with kinematic mass sensitivity. Fitting $e^+e^-$ 2-Jettiness calculations at NLL/NNLL order to Pythia 8.205, $m_t^{\\rm MC}$ differs from the pole mass by $900$/$600$ MeV, and agrees with the MSR mass within u"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.01318","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":"2026-05-18T00:55:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WkBTQBfl4ffcCOJSbe5bxBAYUMG5Xh+vpWYptLX8PU//hF5gWIA9EWxFQO4kjG3FdMQ5f8rL2fq0Mmy+8cILBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T07:05:09.886296Z"},"content_sha256":"02a0a0c553fca63b8fad7cd64c961fef0bf6da48890e48101be53eacf7f9ea77","schema_version":"1.0","event_id":"sha256:02a0a0c553fca63b8fad7cd64c961fef0bf6da48890e48101be53eacf7f9ea77"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/K7NGEQ66II7HD36SIUBFZHTMXE/bundle.json","state_url":"https://pith.science/pith/K7NGEQ66II7HD36SIUBFZHTMXE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/K7NGEQ66II7HD36SIUBFZHTMXE/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":"2026-05-27T07:05:09Z","links":{"resolver":"https://pith.science/pith/K7NGEQ66II7HD36SIUBFZHTMXE","bundle":"https://pith.science/pith/K7NGEQ66II7HD36SIUBFZHTMXE/bundle.json","state":"https://pith.science/pith/K7NGEQ66II7HD36SIUBFZHTMXE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/K7NGEQ66II7HD36SIUBFZHTMXE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:K7NGEQ66II7HD36SIUBFZHTMXE","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":"34e8f535e3a75b0d507e05e69efb64b39a084cae2d628b207e550804269db75f","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-03T20:00:05Z","title_canon_sha256":"9d6b90c39afbf13677a2c33eff54ca8c49ee2845a3997e854e10eb6190b31422"},"schema_version":"1.0","source":{"id":"1608.01318","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.01318","created_at":"2026-05-18T00:55:45Z"},{"alias_kind":"arxiv_version","alias_value":"1608.01318v1","created_at":"2026-05-18T00:55:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.01318","created_at":"2026-05-18T00:55:45Z"},{"alias_kind":"pith_short_12","alias_value":"K7NGEQ66II7H","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_16","alias_value":"K7NGEQ66II7HD36S","created_at":"2026-05-18T12:30:25Z"},{"alias_kind":"pith_short_8","alias_value":"K7NGEQ66","created_at":"2026-05-18T12:30:25Z"}],"graph_snapshots":[{"event_id":"sha256:02a0a0c553fca63b8fad7cd64c961fef0bf6da48890e48101be53eacf7f9ea77","target":"graph","created_at":"2026-05-18T00:55:45Z","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 most precise top quark mass measurements use kinematic reconstruction methods, determining the top mass parameter of a Monte Carlo event generator, $m_t^{\\rm MC}$. Due to hadronization and parton shower dynamics, relating $m_t^{\\rm MC}$ to a field theory mass is difficult. We present a calibration procedure to determine this relation using hadron level QCD predictions for observables with kinematic mass sensitivity. Fitting $e^+e^-$ 2-Jettiness calculations at NLL/NNLL order to Pythia 8.205, $m_t^{\\rm MC}$ differs from the pole mass by $900$/$600$ MeV, and agrees with the MSR mass within u","authors_text":"Andre H. Hoang, Bahman Dehnadi, Iain W. Stewart, Mathias Butenschoen, Moritz Preisser, Vicent Mateu","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-03T20:00:05Z","title":"Top Quark Mass Calibration for Monte Carlo Event Generators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.01318","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":"sha256:74a74960aacfc11dcf9488e415b00aa884e1e8392e27609112e79e48cc2f464b","target":"record","created_at":"2026-05-18T00:55:45Z","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":"34e8f535e3a75b0d507e05e69efb64b39a084cae2d628b207e550804269db75f","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-08-03T20:00:05Z","title_canon_sha256":"9d6b90c39afbf13677a2c33eff54ca8c49ee2845a3997e854e10eb6190b31422"},"schema_version":"1.0","source":{"id":"1608.01318","kind":"arxiv","version":1}},"canonical_sha256":"57da6243de423e71efd245025c9e6cb930c3e4e0c5cfbb3e762ac03f4811c93e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"57da6243de423e71efd245025c9e6cb930c3e4e0c5cfbb3e762ac03f4811c93e","first_computed_at":"2026-05-18T00:55:45.641023Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:55:45.641023Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7ueqhc2yS9svIHY4XaJenjjpRn1Lw9buNnUI0LKwZJQyUsIzbjDWYzdvJuGg71K2iDoFdAoRpRG3vdwa2oaOAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:55:45.641533Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.01318","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:74a74960aacfc11dcf9488e415b00aa884e1e8392e27609112e79e48cc2f464b","sha256:02a0a0c553fca63b8fad7cd64c961fef0bf6da48890e48101be53eacf7f9ea77"],"state_sha256":"9c2408f9d9aa3cf0e632f6d225bc68da1a085a6ad0cb948a9f85e7a304b59d61"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BMWlvQSvs0QT8ZWENUBIZ1BttxthODZkiNpCjB8xv0fSgAriqPqKzTI7JQu0ndVttSzCkbtHG9ftK8DoNfbnAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T07:05:09.889723Z","bundle_sha256":"fbbcd012af3db9066cb70535d575c7d7c4a3053a593f221b105ed305f36fb2fc"}}