{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:GBOAVTH7KI7SS3SS6MDLKNGZOZ","short_pith_number":"pith:GBOAVTH7","canonical_record":{"source":{"id":"1507.08395","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2015-07-30T06:40:15Z","cross_cats_sorted":[],"title_canon_sha256":"2d43b39856842933abf271484f6e5ef08b8975e29a07c002b80ecddde000004d","abstract_canon_sha256":"93de3cad501c25e50f869d1f50664ccb4e7a0eb537a97bcf49baa4a4152d4464"},"schema_version":"1.0"},"canonical_sha256":"305c0accff523f296e52f306b534d9764a26b8e0a2aaf598e3f476b89a7f1287","source":{"kind":"arxiv","id":"1507.08395","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.08395","created_at":"2026-05-18T01:35:59Z"},{"alias_kind":"arxiv_version","alias_value":"1507.08395v2","created_at":"2026-05-18T01:35:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.08395","created_at":"2026-05-18T01:35:59Z"},{"alias_kind":"pith_short_12","alias_value":"GBOAVTH7KI7S","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"GBOAVTH7KI7SS3SS","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"GBOAVTH7","created_at":"2026-05-18T12:29:22Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:GBOAVTH7KI7SS3SS6MDLKNGZOZ","target":"record","payload":{"canonical_record":{"source":{"id":"1507.08395","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2015-07-30T06:40:15Z","cross_cats_sorted":[],"title_canon_sha256":"2d43b39856842933abf271484f6e5ef08b8975e29a07c002b80ecddde000004d","abstract_canon_sha256":"93de3cad501c25e50f869d1f50664ccb4e7a0eb537a97bcf49baa4a4152d4464"},"schema_version":"1.0"},"canonical_sha256":"305c0accff523f296e52f306b534d9764a26b8e0a2aaf598e3f476b89a7f1287","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:35:59.346578Z","signature_b64":"0jqvyyFJLUcj40meNGYyN9Bydjk8gHLBmYNuqWyQjVu6uideFBuSGH3Z5/4YyJYF4c6AdCDn544KCrEM+MUpBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"305c0accff523f296e52f306b534d9764a26b8e0a2aaf598e3f476b89a7f1287","last_reissued_at":"2026-05-18T01:35:59.346086Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:35:59.346086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1507.08395","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":"2026-05-18T01:35:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3LH8jHAdjbjmdRNYQ0pQWqoYClO59qEB36PkfNBEJiLrCqCpnKeleW9L7Jh75fuSmp1aJMGUvppCCjXqdnW1AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T22:46:10.077900Z"},"content_sha256":"51d303ca118bcbdbf4f04b244bdb215dcb634474716d954cef60cb922fa42e65","schema_version":"1.0","event_id":"sha256:51d303ca118bcbdbf4f04b244bdb215dcb634474716d954cef60cb922fa42e65"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:GBOAVTH7KI7SS3SS6MDLKNGZOZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Description of Heavy Quark $\\overline{MS}$ Mass by Lippmann Schwinger Equation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"M. Monemzadeh, M. R. Hadizadeh, N. Tazimi","submitted_at":"2015-07-30T06:40:15Z","abstract_excerpt":"Quark masses are of great prominence in high-energy physics. In this paper, we have studied the heavy meson systems via solving the Lippmann-Schwinger equation by using the Martin potential for heavy quark masses. We have also attempted to use Martin potential to find an acceptable mass spectrum for heavy quarkonia. We obtained this spectrum via minimal phenomenological model (M. Melles, Phys. Rev. D \\textbf{62}: 074019 2000). The mass spectra for $b\\bar{b}$ and $c\\bar{c}$ are calculated without taking into account the relativistic corrections and spin-dependent effects. The obtained mass spec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.08395","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":"2026-05-18T01:35:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2jjRzbGeKtDjuBzR6M6ZcgmAKJ9Hhi+XN8x0vbIXScv55uHESYlYchC3hpf6wt5CY6p4kqsO/64aHxwFEUUKAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T22:46:10.078620Z"},"content_sha256":"a040be31b8a0ce0f7af63ad0b59c6d82ac51f2ff61b783cb1b2a693b13409c86","schema_version":"1.0","event_id":"sha256:a040be31b8a0ce0f7af63ad0b59c6d82ac51f2ff61b783cb1b2a693b13409c86"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ/bundle.json","state_url":"https://pith.science/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ/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":"2026-06-11T22:46:10Z","links":{"resolver":"https://pith.science/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ","bundle":"https://pith.science/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ/bundle.json","state":"https://pith.science/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GBOAVTH7KI7SS3SS6MDLKNGZOZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:GBOAVTH7KI7SS3SS6MDLKNGZOZ","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":"93de3cad501c25e50f869d1f50664ccb4e7a0eb537a97bcf49baa4a4152d4464","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2015-07-30T06:40:15Z","title_canon_sha256":"2d43b39856842933abf271484f6e5ef08b8975e29a07c002b80ecddde000004d"},"schema_version":"1.0","source":{"id":"1507.08395","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1507.08395","created_at":"2026-05-18T01:35:59Z"},{"alias_kind":"arxiv_version","alias_value":"1507.08395v2","created_at":"2026-05-18T01:35:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.08395","created_at":"2026-05-18T01:35:59Z"},{"alias_kind":"pith_short_12","alias_value":"GBOAVTH7KI7S","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_16","alias_value":"GBOAVTH7KI7SS3SS","created_at":"2026-05-18T12:29:22Z"},{"alias_kind":"pith_short_8","alias_value":"GBOAVTH7","created_at":"2026-05-18T12:29:22Z"}],"graph_snapshots":[{"event_id":"sha256:a040be31b8a0ce0f7af63ad0b59c6d82ac51f2ff61b783cb1b2a693b13409c86","target":"graph","created_at":"2026-05-18T01:35:59Z","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":"Quark masses are of great prominence in high-energy physics. In this paper, we have studied the heavy meson systems via solving the Lippmann-Schwinger equation by using the Martin potential for heavy quark masses. We have also attempted to use Martin potential to find an acceptable mass spectrum for heavy quarkonia. We obtained this spectrum via minimal phenomenological model (M. Melles, Phys. Rev. D \\textbf{62}: 074019 2000). The mass spectra for $b\\bar{b}$ and $c\\bar{c}$ are calculated without taking into account the relativistic corrections and spin-dependent effects. The obtained mass spec","authors_text":"M. Monemzadeh, M. R. Hadizadeh, N. Tazimi","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2015-07-30T06:40:15Z","title":"Description of Heavy Quark $\\overline{MS}$ Mass by Lippmann Schwinger Equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.08395","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":"sha256:51d303ca118bcbdbf4f04b244bdb215dcb634474716d954cef60cb922fa42e65","target":"record","created_at":"2026-05-18T01:35:59Z","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":"93de3cad501c25e50f869d1f50664ccb4e7a0eb537a97bcf49baa4a4152d4464","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2015-07-30T06:40:15Z","title_canon_sha256":"2d43b39856842933abf271484f6e5ef08b8975e29a07c002b80ecddde000004d"},"schema_version":"1.0","source":{"id":"1507.08395","kind":"arxiv","version":2}},"canonical_sha256":"305c0accff523f296e52f306b534d9764a26b8e0a2aaf598e3f476b89a7f1287","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"305c0accff523f296e52f306b534d9764a26b8e0a2aaf598e3f476b89a7f1287","first_computed_at":"2026-05-18T01:35:59.346086Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:35:59.346086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0jqvyyFJLUcj40meNGYyN9Bydjk8gHLBmYNuqWyQjVu6uideFBuSGH3Z5/4YyJYF4c6AdCDn544KCrEM+MUpBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:35:59.346578Z","signed_message":"canonical_sha256_bytes"},"source_id":"1507.08395","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:51d303ca118bcbdbf4f04b244bdb215dcb634474716d954cef60cb922fa42e65","sha256:a040be31b8a0ce0f7af63ad0b59c6d82ac51f2ff61b783cb1b2a693b13409c86"],"state_sha256":"d6854c1aec1c9dcc48687f0a84eeaeb17121cfb653d8713dfa7744da56e804ba"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UijKrtpj0FkUDAltpzL4qWxEjy9SsKXr3vyrbXesQ4nnEXAld0fTp3pVEfhQdvllY3mnOd8Xy6tE2kgHsYZgAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T22:46:10.082675Z","bundle_sha256":"fa869402fefa7a6d5fe334d2b9e8ebf1379f808d77ac943c5763f2deafbafc74"}}