{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:MSAKH5MNOOFWOQU54AF563HXTH","short_pith_number":"pith:MSAKH5MN","canonical_record":{"source":{"id":"1202.4353","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-02-20T15:21:47Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"fc805a1b61eb26290563e5cb30325cc2c25a28ec9d53544d9a2afa2196a8d4ad","abstract_canon_sha256":"15e997a28e0d0106281715743e5e0a360706639899b1ffe220b463bb2520b75a"},"schema_version":"1.0"},"canonical_sha256":"6480a3f58d738b67429de00bdf6cf799e9967c870205610fc51041936add2b3b","source":{"kind":"arxiv","id":"1202.4353","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.4353","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"arxiv_version","alias_value":"1202.4353v1","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.4353","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"pith_short_12","alias_value":"MSAKH5MNOOFW","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_16","alias_value":"MSAKH5MNOOFWOQU5","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_8","alias_value":"MSAKH5MN","created_at":"2026-05-18T12:27:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:MSAKH5MNOOFWOQU54AF563HXTH","target":"record","payload":{"canonical_record":{"source":{"id":"1202.4353","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-02-20T15:21:47Z","cross_cats_sorted":["hep-ph","nucl-th"],"title_canon_sha256":"fc805a1b61eb26290563e5cb30325cc2c25a28ec9d53544d9a2afa2196a8d4ad","abstract_canon_sha256":"15e997a28e0d0106281715743e5e0a360706639899b1ffe220b463bb2520b75a"},"schema_version":"1.0"},"canonical_sha256":"6480a3f58d738b67429de00bdf6cf799e9967c870205610fc51041936add2b3b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:23.519635Z","signature_b64":"a8kSBjBZ0E34TfEk62Tv+bMBqLfjogDlSPgtFkfQ3li9TnL76dMyH8aC4V/LeXFOj+nCTI8jGLIsUmmlrd04Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6480a3f58d738b67429de00bdf6cf799e9967c870205610fc51041936add2b3b","last_reissued_at":"2026-05-18T01:58:23.519022Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:23.519022Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1202.4353","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":"2026-05-18T01:58:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iwSNB2jjBYdn1PitzlX8J/PnfYFIUKBZ6DmX2jqqEihLkUk78b8f10zLy7dfr9hGkQve7uOGiCG88EiB2YPjAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T19:42:19.932986Z"},"content_sha256":"9aadbfea8b8d8a180adaebacb8ad8ef1d50992568a25cd7c25fce7ede435fbc0","schema_version":"1.0","event_id":"sha256:9aadbfea8b8d8a180adaebacb8ad8ef1d50992568a25cd7c25fce7ede435fbc0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:MSAKH5MNOOFWOQU54AF563HXTH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-relativistic spectrum of two-color QCD at non-zero baryon density","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-th"],"primary_cat":"hep-lat","authors_text":"Jon-Ivar Skullerud, Seyong Kim, Simon Hands","submitted_at":"2012-02-20T15:21:47Z","abstract_excerpt":"The heavy quarkonium spectrum of Two Color QCD (QC$_2$D) at non-zero quark chemical potential $\\mu$ and temperature $T$ with $\\mu/T\\gg1$ has been calculated in both $S$- and $P$-wave channels using a lattice non-relativistic formulation of QC$_2$D. As $\\mu$ is varied, the quarkonium spectra reveal three separate regions, corroborating previous findings that there are three distinct physical regimes of QC$_2$D at low temperature and high baryon density: hadronic matter, quark/quarkyonic matter, and deconfined matter. The results are interpreted in terms of the formation of heavy-light $Qq$ stat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.4353","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":"2026-05-18T01:58:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"FGHwEFbY3sTqtV2qp6X1SzbcY/i/HZGR/sz+A/WsHEuw5hdPgajabVodQ3kf172gh7j+jfBQstbKAvFFh03BAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T19:42:19.933773Z"},"content_sha256":"f83ef46e5323491faf9f4d0b7c76748a16a4768fe284b54c50b1db5fef252ff0","schema_version":"1.0","event_id":"sha256:f83ef46e5323491faf9f4d0b7c76748a16a4768fe284b54c50b1db5fef252ff0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MSAKH5MNOOFWOQU54AF563HXTH/bundle.json","state_url":"https://pith.science/pith/MSAKH5MNOOFWOQU54AF563HXTH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MSAKH5MNOOFWOQU54AF563HXTH/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":"2026-06-11T19:42:19Z","links":{"resolver":"https://pith.science/pith/MSAKH5MNOOFWOQU54AF563HXTH","bundle":"https://pith.science/pith/MSAKH5MNOOFWOQU54AF563HXTH/bundle.json","state":"https://pith.science/pith/MSAKH5MNOOFWOQU54AF563HXTH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MSAKH5MNOOFWOQU54AF563HXTH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:MSAKH5MNOOFWOQU54AF563HXTH","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":"15e997a28e0d0106281715743e5e0a360706639899b1ffe220b463bb2520b75a","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-02-20T15:21:47Z","title_canon_sha256":"fc805a1b61eb26290563e5cb30325cc2c25a28ec9d53544d9a2afa2196a8d4ad"},"schema_version":"1.0","source":{"id":"1202.4353","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1202.4353","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"arxiv_version","alias_value":"1202.4353v1","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.4353","created_at":"2026-05-18T01:58:23Z"},{"alias_kind":"pith_short_12","alias_value":"MSAKH5MNOOFW","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_16","alias_value":"MSAKH5MNOOFWOQU5","created_at":"2026-05-18T12:27:14Z"},{"alias_kind":"pith_short_8","alias_value":"MSAKH5MN","created_at":"2026-05-18T12:27:14Z"}],"graph_snapshots":[{"event_id":"sha256:f83ef46e5323491faf9f4d0b7c76748a16a4768fe284b54c50b1db5fef252ff0","target":"graph","created_at":"2026-05-18T01:58:23Z","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 heavy quarkonium spectrum of Two Color QCD (QC$_2$D) at non-zero quark chemical potential $\\mu$ and temperature $T$ with $\\mu/T\\gg1$ has been calculated in both $S$- and $P$-wave channels using a lattice non-relativistic formulation of QC$_2$D. As $\\mu$ is varied, the quarkonium spectra reveal three separate regions, corroborating previous findings that there are three distinct physical regimes of QC$_2$D at low temperature and high baryon density: hadronic matter, quark/quarkyonic matter, and deconfined matter. The results are interpreted in terms of the formation of heavy-light $Qq$ stat","authors_text":"Jon-Ivar Skullerud, Seyong Kim, Simon Hands","cross_cats":["hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-02-20T15:21:47Z","title":"Non-relativistic spectrum of two-color QCD at non-zero baryon density"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.4353","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":"sha256:9aadbfea8b8d8a180adaebacb8ad8ef1d50992568a25cd7c25fce7ede435fbc0","target":"record","created_at":"2026-05-18T01:58:23Z","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":"15e997a28e0d0106281715743e5e0a360706639899b1ffe220b463bb2520b75a","cross_cats_sorted":["hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2012-02-20T15:21:47Z","title_canon_sha256":"fc805a1b61eb26290563e5cb30325cc2c25a28ec9d53544d9a2afa2196a8d4ad"},"schema_version":"1.0","source":{"id":"1202.4353","kind":"arxiv","version":1}},"canonical_sha256":"6480a3f58d738b67429de00bdf6cf799e9967c870205610fc51041936add2b3b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6480a3f58d738b67429de00bdf6cf799e9967c870205610fc51041936add2b3b","first_computed_at":"2026-05-18T01:58:23.519022Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:23.519022Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"a8kSBjBZ0E34TfEk62Tv+bMBqLfjogDlSPgtFkfQ3li9TnL76dMyH8aC4V/LeXFOj+nCTI8jGLIsUmmlrd04Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:23.519635Z","signed_message":"canonical_sha256_bytes"},"source_id":"1202.4353","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9aadbfea8b8d8a180adaebacb8ad8ef1d50992568a25cd7c25fce7ede435fbc0","sha256:f83ef46e5323491faf9f4d0b7c76748a16a4768fe284b54c50b1db5fef252ff0"],"state_sha256":"1d39d4b8435559cd21c95e1b00c5d52595f686a16b6540d202beb93488d684d4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s+t/hXKqphmZqX4G9aQ09ARshV+VjE4x/KsGtLG8c93AoMEX0jQklCpIvbC5Qf2kuAqYaKE4OyVmekjwqAtiCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T19:42:19.937951Z","bundle_sha256":"c0f9bf697af19fed3ebcd891e8e3910c3196ad61f065b007741267b88d6cafbc"}}