{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:4FVAOUXDF3DTMC2C2RB26C7CCM","short_pith_number":"pith:4FVAOUXD","schema_version":"1.0","canonical_sha256":"e16a0752e32ec7360b42d443af0be2130be2222688485479871519476bee62a5","source":{"kind":"arxiv","id":"1509.02396","version":2},"attestation_state":"computed","paper":{"title":"Masses of $D$ mesons, $D_s$ mesons and charmonium states from twisted mass lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"hep-lat","authors_text":"Marc Wagner, Martin Kalinowski","submitted_at":"2015-09-08T14:51:25Z","abstract_excerpt":"We compute masses of $D$ mesons, $D_s$ mesons and charmonium states using Wilson twisted mass lattice QCD. We present results for spin $J = 0,1,2,3$, parity $\\mathcal{P} = -,+$ and in case of charmonium also charge conjugation $\\mathcal{C} = -,+$. Computations are based on quark-antiquark creation operators and performed at three different unphysically heavy $u/d$ quark masses allowing an extrapolation to the physical $u/d$ quark mass. Within combined statistical and systematic errors, which are around $2 \\% \\ldots 3 \\%$, our results agree with available experimental results. Particular focus "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1509.02396","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-09-08T14:51:25Z","cross_cats_sorted":["hep-ex","hep-ph"],"title_canon_sha256":"3dedf838f4a77f1d04df668f0f1e460ce9dda441df13e6ea271840cf54856373","abstract_canon_sha256":"47b2ad8e10e55a3920d16b9a2728f76326a03bff79b7babf7a69fa1a13c083e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:41.694891Z","signature_b64":"wIFg/fwTJEcmy8mELm58Eq60ARSFg+KKlhXTsT1QDum2Ssj7zTrhMYibcNqWKcEsYH17+/NGIZ668MwHh5UEDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e16a0752e32ec7360b42d443af0be2130be2222688485479871519476bee62a5","last_reissued_at":"2026-05-18T01:26:41.693998Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:41.693998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Masses of $D$ mesons, $D_s$ mesons and charmonium states from twisted mass lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-ph"],"primary_cat":"hep-lat","authors_text":"Marc Wagner, Martin Kalinowski","submitted_at":"2015-09-08T14:51:25Z","abstract_excerpt":"We compute masses of $D$ mesons, $D_s$ mesons and charmonium states using Wilson twisted mass lattice QCD. We present results for spin $J = 0,1,2,3$, parity $\\mathcal{P} = -,+$ and in case of charmonium also charge conjugation $\\mathcal{C} = -,+$. Computations are based on quark-antiquark creation operators and performed at three different unphysically heavy $u/d$ quark masses allowing an extrapolation to the physical $u/d$ quark mass. Within combined statistical and systematic errors, which are around $2 \\% \\ldots 3 \\%$, our results agree with available experimental results. Particular focus "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.02396","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1509.02396","created_at":"2026-05-18T01:26:41.694142+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.02396v2","created_at":"2026-05-18T01:26:41.694142+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.02396","created_at":"2026-05-18T01:26:41.694142+00:00"},{"alias_kind":"pith_short_12","alias_value":"4FVAOUXDF3DT","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_16","alias_value":"4FVAOUXDF3DTMC2C","created_at":"2026-05-18T12:29:05.191682+00:00"},{"alias_kind":"pith_short_8","alias_value":"4FVAOUXD","created_at":"2026-05-18T12:29:05.191682+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM","json":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM.json","graph_json":"https://pith.science/api/pith-number/4FVAOUXDF3DTMC2C2RB26C7CCM/graph.json","events_json":"https://pith.science/api/pith-number/4FVAOUXDF3DTMC2C2RB26C7CCM/events.json","paper":"https://pith.science/paper/4FVAOUXD"},"agent_actions":{"view_html":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM","download_json":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM.json","view_paper":"https://pith.science/paper/4FVAOUXD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.02396&json=true","fetch_graph":"https://pith.science/api/pith-number/4FVAOUXDF3DTMC2C2RB26C7CCM/graph.json","fetch_events":"https://pith.science/api/pith-number/4FVAOUXDF3DTMC2C2RB26C7CCM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM/action/storage_attestation","attest_author":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM/action/author_attestation","sign_citation":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM/action/citation_signature","submit_replication":"https://pith.science/pith/4FVAOUXDF3DTMC2C2RB26C7CCM/action/replication_record"}},"created_at":"2026-05-18T01:26:41.694142+00:00","updated_at":"2026-05-18T01:26:41.694142+00:00"}