{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:SMR2JHQ5J2WFJOVUQAGDEVUZUN","short_pith_number":"pith:SMR2JHQ5","canonical_record":{"source":{"id":"1412.1706","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-12-04T15:39:48Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"fb539c44d2a646adc978c172b199c36ace96d9070db1bdbc34b8c86a556ae170","abstract_canon_sha256":"790e759c59c82c55e661fdc94997857ccb0c53c04da2ecf32c5ac10e9fba4d9b"},"schema_version":"1.0"},"canonical_sha256":"9323a49e1d4eac54bab4800c325699a353572e0fe709ff71bec74175f6570bff","source":{"kind":"arxiv","id":"1412.1706","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.1706","created_at":"2026-05-18T01:58:27Z"},{"alias_kind":"arxiv_version","alias_value":"1412.1706v3","created_at":"2026-05-18T01:58:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.1706","created_at":"2026-05-18T01:58:27Z"},{"alias_kind":"pith_short_12","alias_value":"SMR2JHQ5J2WF","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"SMR2JHQ5J2WFJOVU","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"SMR2JHQ5","created_at":"2026-05-18T12:28:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:SMR2JHQ5J2WFJOVUQAGDEVUZUN","target":"record","payload":{"canonical_record":{"source":{"id":"1412.1706","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-12-04T15:39:48Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"fb539c44d2a646adc978c172b199c36ace96d9070db1bdbc34b8c86a556ae170","abstract_canon_sha256":"790e759c59c82c55e661fdc94997857ccb0c53c04da2ecf32c5ac10e9fba4d9b"},"schema_version":"1.0"},"canonical_sha256":"9323a49e1d4eac54bab4800c325699a353572e0fe709ff71bec74175f6570bff","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:27.079110Z","signature_b64":"gzVpgsQJ2AGl540/OdNFTW5PaKNrcMlve+KZ45AJ3kyqH3K3fGCax1ZgcrozrPO/MKfV+ypCzAqjaxSoYHNeDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9323a49e1d4eac54bab4800c325699a353572e0fe709ff71bec74175f6570bff","last_reissued_at":"2026-05-18T01:58:27.078620Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:27.078620Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.1706","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:58:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mftzAy+IlNRMzIEwt7n89AHZUYZc3HyvEtJWwKZcO7xwvVs2RtnmjO8w+ovf6A2VO4rmio324upyfWj9S+BoDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T15:56:28.452566Z"},"content_sha256":"66be06176ab50428596d0544a1238ef957a04d2a9fc95b75a24b1b0c046fba4d","schema_version":"1.0","event_id":"sha256:66be06176ab50428596d0544a1238ef957a04d2a9fc95b75a24b1b0c046fba4d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:SMR2JHQ5J2WFJOVUQAGDEVUZUN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Reanalysis of lattice QCD spectra leading to the $D_{s0}^*(2317)$ and $D_{s1}^*(2460)$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"A. Mart\\'inez Torres, A. Ramos, E. Oset, S. Prelovsek","submitted_at":"2014-12-04T15:39:48Z","abstract_excerpt":"We perform a reanalysis of the energy levels obtained in a recent lattice QCD simulation, from where the existence of bound states of $KD$ and $KD^*$ are induced and identified with the narrow $D_{s0}^*(2317)$ and $D_{s1}^*(2460)$ resonances. The reanalysis is done in terms of an auxiliary potential, employing a single-channel basis $KD^{(*)}$, and a two-channel basis $KD^{(*)}, \\eta D_s^{(*)}$. By means of an extended L\\\"uscher method we determine poles of the continuum $t$-matrix, bound by about 40 MeV with respect to the $KD$ and $KD^*$ thresholds, which we identify with the $D_{s0}^*(2317)"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.1706","kind":"arxiv","version":3},"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":"2026-05-18T01:58:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zWR4eZL69IgNatybVDF2h3SsTm4NEo7Hx4HsyUK3ukzLb7PztQK/fGCcx+1fkYS3DCFqFJPrvSSgxQmupQTiAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T15:56:28.452937Z"},"content_sha256":"6204e0f7e9daf333e75e373e773afefbfd5f8091d51b37850df15a1949ec17ee","schema_version":"1.0","event_id":"sha256:6204e0f7e9daf333e75e373e773afefbfd5f8091d51b37850df15a1949ec17ee"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN/bundle.json","state_url":"https://pith.science/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN/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":"2026-05-21T15:56:28Z","links":{"resolver":"https://pith.science/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN","bundle":"https://pith.science/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN/bundle.json","state":"https://pith.science/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SMR2JHQ5J2WFJOVUQAGDEVUZUN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:SMR2JHQ5J2WFJOVUQAGDEVUZUN","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":"790e759c59c82c55e661fdc94997857ccb0c53c04da2ecf32c5ac10e9fba4d9b","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-12-04T15:39:48Z","title_canon_sha256":"fb539c44d2a646adc978c172b199c36ace96d9070db1bdbc34b8c86a556ae170"},"schema_version":"1.0","source":{"id":"1412.1706","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.1706","created_at":"2026-05-18T01:58:27Z"},{"alias_kind":"arxiv_version","alias_value":"1412.1706v3","created_at":"2026-05-18T01:58:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.1706","created_at":"2026-05-18T01:58:27Z"},{"alias_kind":"pith_short_12","alias_value":"SMR2JHQ5J2WF","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_16","alias_value":"SMR2JHQ5J2WFJOVU","created_at":"2026-05-18T12:28:49Z"},{"alias_kind":"pith_short_8","alias_value":"SMR2JHQ5","created_at":"2026-05-18T12:28:49Z"}],"graph_snapshots":[{"event_id":"sha256:6204e0f7e9daf333e75e373e773afefbfd5f8091d51b37850df15a1949ec17ee","target":"graph","created_at":"2026-05-18T01:58:27Z","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":"We perform a reanalysis of the energy levels obtained in a recent lattice QCD simulation, from where the existence of bound states of $KD$ and $KD^*$ are induced and identified with the narrow $D_{s0}^*(2317)$ and $D_{s1}^*(2460)$ resonances. The reanalysis is done in terms of an auxiliary potential, employing a single-channel basis $KD^{(*)}$, and a two-channel basis $KD^{(*)}, \\eta D_s^{(*)}$. By means of an extended L\\\"uscher method we determine poles of the continuum $t$-matrix, bound by about 40 MeV with respect to the $KD$ and $KD^*$ thresholds, which we identify with the $D_{s0}^*(2317)","authors_text":"A. Mart\\'inez Torres, A. Ramos, E. Oset, S. Prelovsek","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-12-04T15:39:48Z","title":"Reanalysis of lattice QCD spectra leading to the $D_{s0}^*(2317)$ and $D_{s1}^*(2460)$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.1706","kind":"arxiv","version":3},"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":"sha256:66be06176ab50428596d0544a1238ef957a04d2a9fc95b75a24b1b0c046fba4d","target":"record","created_at":"2026-05-18T01:58:27Z","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":"790e759c59c82c55e661fdc94997857ccb0c53c04da2ecf32c5ac10e9fba4d9b","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-12-04T15:39:48Z","title_canon_sha256":"fb539c44d2a646adc978c172b199c36ace96d9070db1bdbc34b8c86a556ae170"},"schema_version":"1.0","source":{"id":"1412.1706","kind":"arxiv","version":3}},"canonical_sha256":"9323a49e1d4eac54bab4800c325699a353572e0fe709ff71bec74175f6570bff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9323a49e1d4eac54bab4800c325699a353572e0fe709ff71bec74175f6570bff","first_computed_at":"2026-05-18T01:58:27.078620Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:27.078620Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"gzVpgsQJ2AGl540/OdNFTW5PaKNrcMlve+KZ45AJ3kyqH3K3fGCax1ZgcrozrPO/MKfV+ypCzAqjaxSoYHNeDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:27.079110Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.1706","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:66be06176ab50428596d0544a1238ef957a04d2a9fc95b75a24b1b0c046fba4d","sha256:6204e0f7e9daf333e75e373e773afefbfd5f8091d51b37850df15a1949ec17ee"],"state_sha256":"bd50f7c469972be58060ddc4de16d9130512fb1f56bf2a82457f4518aaf5dfb7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U09+365w/T+JBtwD9672TWtH8yRIhNDX6yewSOZ0w/6K7vysSN3VUOKCT8l6oHECgetYUNXTRFke8L8VBNLIAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T15:56:28.455607Z","bundle_sha256":"454d90fd1789de794a1d65c6524691f0e3fdf0a52e79b9af73a57e0c47a8714c"}}