{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:5MJXGGUGCO5EAJAKIBIHBCXYKX","short_pith_number":"pith:5MJXGGUG","canonical_record":{"source":{"id":"2508.11968","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-16T08:07:42Z","cross_cats_sorted":[],"title_canon_sha256":"ae5c8f50cbe1cfccb9c0809af1a626194fdd88be47f5738f021b9432fdb973e6","abstract_canon_sha256":"a4caaab01e063cb252effa0f4594c70c9201b652911caa3c58b9f439780c48a5"},"schema_version":"1.0"},"canonical_sha256":"eb13731a8613ba40240a4050708af855fbb1f3a80cdc005786b9a99d3992354f","source":{"kind":"arxiv","id":"2508.11968","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2508.11968","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"arxiv_version","alias_value":"2508.11968v1","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.11968","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"pith_short_12","alias_value":"5MJXGGUGCO5E","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"pith_short_16","alias_value":"5MJXGGUGCO5EAJAK","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"pith_short_8","alias_value":"5MJXGGUG","created_at":"2026-07-05T11:54:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:5MJXGGUGCO5EAJAKIBIHBCXYKX","target":"record","payload":{"canonical_record":{"source":{"id":"2508.11968","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-16T08:07:42Z","cross_cats_sorted":[],"title_canon_sha256":"ae5c8f50cbe1cfccb9c0809af1a626194fdd88be47f5738f021b9432fdb973e6","abstract_canon_sha256":"a4caaab01e063cb252effa0f4594c70c9201b652911caa3c58b9f439780c48a5"},"schema_version":"1.0"},"canonical_sha256":"eb13731a8613ba40240a4050708af855fbb1f3a80cdc005786b9a99d3992354f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:54:57.979125Z","signature_b64":"Dn3AtZTPABdqJLneI2zFpEHEfBfgmzBMuzL8mHJejluuMPnqeTQdLxS/qfFBB/DeeBs4fMLAKCWlteUiGN1YDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eb13731a8613ba40240a4050708af855fbb1f3a80cdc005786b9a99d3992354f","last_reissued_at":"2026-07-05T11:54:57.978693Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:54:57.978693Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2508.11968","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":"2026-07-05T11:54:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2DABMnU224VykdKjgkg2kZZ/R+kd6wA3cW/GWYc/YTNsada/c0OgS4lG/seLRn6iz7I9iImYc0fOI4AfjqQpAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T15:16:19.163258Z"},"content_sha256":"b52f393525d22a56f2146ce959eb7738265535010e7b99490fc7b9f14b1c5883","schema_version":"1.0","event_id":"sha256:b52f393525d22a56f2146ce959eb7738265535010e7b99490fc7b9f14b1c5883"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:5MJXGGUGCO5EAJAKIBIHBCXYKX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical quark mass and finite volume effects in the Dyson-Schwinger Equations","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"De-Xian Wei, Hong-Wei Zhong, Li-juan Zhou, Zhong-Yi Liu","submitted_at":"2025-08-16T08:07:42Z","abstract_excerpt":"Within the framework of Dyson-Schwinger equations(DSEs) and by means of the Multiple Reflection Expansion approximation, we study the finite volume effects of the constituent quark mass in a strong external magnetic field. Since the magnetic field has influence on the coupling constant, the coupling constant controls the strength of strongly interaction in QCD, so we adopt the magnetic-field-dependent running coupling constant in simulation. The results show that in addition to the magnetic field, the masses of constituent quarks also have a significant dependence on the volume and the running"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.11968","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2508.11968/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-05T11:54:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"q9lOpnW1n7LFAmu9wSaCjdXujmde7QVC/9jPmZFTEJ/D2HFc79bVy8Ry7E01ZZ5CkxQKM4v3SbwbRu+XAEh4DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-18T15:16:19.163938Z"},"content_sha256":"b63650bb0dea1fbc8ed467f32a05a0c15c7268efb03b06a2cea689da809ca5a4","schema_version":"1.0","event_id":"sha256:b63650bb0dea1fbc8ed467f32a05a0c15c7268efb03b06a2cea689da809ca5a4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX/bundle.json","state_url":"https://pith.science/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX/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":"2026-08-18T15:16:19Z","links":{"resolver":"https://pith.science/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX","bundle":"https://pith.science/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX/bundle.json","state":"https://pith.science/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5MJXGGUGCO5EAJAKIBIHBCXYKX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:5MJXGGUGCO5EAJAKIBIHBCXYKX","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":"a4caaab01e063cb252effa0f4594c70c9201b652911caa3c58b9f439780c48a5","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-16T08:07:42Z","title_canon_sha256":"ae5c8f50cbe1cfccb9c0809af1a626194fdd88be47f5738f021b9432fdb973e6"},"schema_version":"1.0","source":{"id":"2508.11968","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2508.11968","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"arxiv_version","alias_value":"2508.11968v1","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.11968","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"pith_short_12","alias_value":"5MJXGGUGCO5E","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"pith_short_16","alias_value":"5MJXGGUGCO5EAJAK","created_at":"2026-07-05T11:54:57Z"},{"alias_kind":"pith_short_8","alias_value":"5MJXGGUG","created_at":"2026-07-05T11:54:57Z"}],"graph_snapshots":[{"event_id":"sha256:b63650bb0dea1fbc8ed467f32a05a0c15c7268efb03b06a2cea689da809ca5a4","target":"graph","created_at":"2026-07-05T11:54:57Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2508.11968/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Within the framework of Dyson-Schwinger equations(DSEs) and by means of the Multiple Reflection Expansion approximation, we study the finite volume effects of the constituent quark mass in a strong external magnetic field. Since the magnetic field has influence on the coupling constant, the coupling constant controls the strength of strongly interaction in QCD, so we adopt the magnetic-field-dependent running coupling constant in simulation. The results show that in addition to the magnetic field, the masses of constituent quarks also have a significant dependence on the volume and the running","authors_text":"De-Xian Wei, Hong-Wei Zhong, Li-juan Zhou, Zhong-Yi Liu","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-16T08:07:42Z","title":"Dynamical quark mass and finite volume effects in the Dyson-Schwinger Equations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.11968","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:b52f393525d22a56f2146ce959eb7738265535010e7b99490fc7b9f14b1c5883","target":"record","created_at":"2026-07-05T11:54:57Z","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":"a4caaab01e063cb252effa0f4594c70c9201b652911caa3c58b9f439780c48a5","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-16T08:07:42Z","title_canon_sha256":"ae5c8f50cbe1cfccb9c0809af1a626194fdd88be47f5738f021b9432fdb973e6"},"schema_version":"1.0","source":{"id":"2508.11968","kind":"arxiv","version":1}},"canonical_sha256":"eb13731a8613ba40240a4050708af855fbb1f3a80cdc005786b9a99d3992354f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"eb13731a8613ba40240a4050708af855fbb1f3a80cdc005786b9a99d3992354f","first_computed_at":"2026-07-05T11:54:57.978693Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:54:57.978693Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Dn3AtZTPABdqJLneI2zFpEHEfBfgmzBMuzL8mHJejluuMPnqeTQdLxS/qfFBB/DeeBs4fMLAKCWlteUiGN1YDw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:54:57.979125Z","signed_message":"canonical_sha256_bytes"},"source_id":"2508.11968","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b52f393525d22a56f2146ce959eb7738265535010e7b99490fc7b9f14b1c5883","sha256:b63650bb0dea1fbc8ed467f32a05a0c15c7268efb03b06a2cea689da809ca5a4"],"state_sha256":"0173b9ac24884ea1ac115f88119bc25531196be7778efc0f635d0f775d0784c7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0YJmYbXWCoBoGKBkVNp90Gt40EMlTcKds5psCRMNdqssUv+LP0PSD+upa0FWRqiYksaDuO1d4vCfTHtyJlU3DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-18T15:16:19.172189Z","bundle_sha256":"653ce7372f41fc6ff455ed970308777bfc34d66637e651b66e65fae1171977ef"}}