{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:YGBSNDXHXE2PDF6JBEXMQVJARL","short_pith_number":"pith:YGBSNDXH","schema_version":"1.0","canonical_sha256":"c183268ee7b934f197c9092ec855208ac1c7ba9e1395bc6627ed47fe3b3043ae","source":{"kind":"arxiv","id":"1105.4807","version":2},"attestation_state":"computed","paper":{"title":"The spin-orbit potential and Poincar\\'e invariance in finite temperature pNRQCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Antonio Vairo, Jacopo Ghiglieri, Miguel Angel Escobedo, Nora Brambilla","submitted_at":"2011-05-24T15:47:24Z","abstract_excerpt":"Heavy quarkonium at finite temperature has been the subject of intense theoretical studies, for it provides a potentially clean probe of the quark-gluon plasma. Recent studies have made use of effective field theories to exploit in a systematic manner the hierarchy of energy scales that characterize the system. In the case of a quarkonium in a medium whose temperature is smaller than the typical momentum transfer in the bound state but larger than its energy, the suitable effective field theory is pNRQCD_HTL, where degrees of freedom with energy or momentum larger than the binding energy have "},"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":"1105.4807","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-05-24T15:47:24Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"9f269d34e6b73fde049e6435741fc97da925bdc7eebf6621e31b3d0523bc8502","abstract_canon_sha256":"b1b7eaa8b95f38b5369df638a64df033d71e56b9518717d61a078895bdbb51be"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:02.363970Z","signature_b64":"GXYTATrU9exd5rnX+j+y1U4SPLTUhp2ApWVAPbV4yqTdRyvGZM6B3mWXxJBpI7S9WGGQi8QADy1HjXWZ/2g/AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c183268ee7b934f197c9092ec855208ac1c7ba9e1395bc6627ed47fe3b3043ae","last_reissued_at":"2026-05-18T04:17:02.363242Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:02.363242Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The spin-orbit potential and Poincar\\'e invariance in finite temperature pNRQCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Antonio Vairo, Jacopo Ghiglieri, Miguel Angel Escobedo, Nora Brambilla","submitted_at":"2011-05-24T15:47:24Z","abstract_excerpt":"Heavy quarkonium at finite temperature has been the subject of intense theoretical studies, for it provides a potentially clean probe of the quark-gluon plasma. Recent studies have made use of effective field theories to exploit in a systematic manner the hierarchy of energy scales that characterize the system. In the case of a quarkonium in a medium whose temperature is smaller than the typical momentum transfer in the bound state but larger than its energy, the suitable effective field theory is pNRQCD_HTL, where degrees of freedom with energy or momentum larger than the binding energy have "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.4807","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":"1105.4807","created_at":"2026-05-18T04:17:02.363353+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.4807v2","created_at":"2026-05-18T04:17:02.363353+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.4807","created_at":"2026-05-18T04:17:02.363353+00:00"},{"alias_kind":"pith_short_12","alias_value":"YGBSNDXHXE2P","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"YGBSNDXHXE2PDF6J","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"YGBSNDXH","created_at":"2026-05-18T12:26:47.523578+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/YGBSNDXHXE2PDF6JBEXMQVJARL","json":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL.json","graph_json":"https://pith.science/api/pith-number/YGBSNDXHXE2PDF6JBEXMQVJARL/graph.json","events_json":"https://pith.science/api/pith-number/YGBSNDXHXE2PDF6JBEXMQVJARL/events.json","paper":"https://pith.science/paper/YGBSNDXH"},"agent_actions":{"view_html":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL","download_json":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL.json","view_paper":"https://pith.science/paper/YGBSNDXH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.4807&json=true","fetch_graph":"https://pith.science/api/pith-number/YGBSNDXHXE2PDF6JBEXMQVJARL/graph.json","fetch_events":"https://pith.science/api/pith-number/YGBSNDXHXE2PDF6JBEXMQVJARL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL/action/storage_attestation","attest_author":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL/action/author_attestation","sign_citation":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL/action/citation_signature","submit_replication":"https://pith.science/pith/YGBSNDXHXE2PDF6JBEXMQVJARL/action/replication_record"}},"created_at":"2026-05-18T04:17:02.363353+00:00","updated_at":"2026-05-18T04:17:02.363353+00:00"}