{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:YR3F2YOBDKJZFQY6D6JR7OUGBD","short_pith_number":"pith:YR3F2YOB","schema_version":"1.0","canonical_sha256":"c4765d61c11a9392c31e1f931fba8608f437f6a47cf4f47708a19c873ec2716c","source":{"kind":"arxiv","id":"2203.02747","version":2},"attestation_state":"computed","paper":{"title":"The massless thermal field and the thermal fermion bosonization in two dimensions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emil Akhmedov, Henri Epstein, Ugo Moschella","submitted_at":"2022-03-05T13:58:22Z","abstract_excerpt":"We come back to the issue of bosonization of fermions in two spacetime dimension and give a new costruction in the steady state case where left and right moving particles can coexist at two different temperatures. A crucial role in our construction is played by translation invariant infrared states and the corresponding field operators which are naturally linked to the infrared behaviour of the correlation functions. We present two applications: a simple new derivation in the free relativistic case of a formula by Bernard and Doyon and a full operator solution of the massless Thirring model in"},"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":"2203.02747","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-03-05T13:58:22Z","cross_cats_sorted":[],"title_canon_sha256":"c02668c3036d3444bdc642293ab39fe46b4d7f3643425ff7d52e165a77640602","abstract_canon_sha256":"637b7d805a6f52e10448faf1dcb19fc2f4fa75c6dc23c293d1decc92d4e5c84c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:01:20.312677Z","signature_b64":"Uv7XyumgPn+2bFv/J4Q62/umi+/xmi4E3siJstjwnAsV3FaWjoO/Co6IfYcncf+ELdPWGqwOJXXbnzjsml7WCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c4765d61c11a9392c31e1f931fba8608f437f6a47cf4f47708a19c873ec2716c","last_reissued_at":"2026-07-05T05:01:20.312074Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:01:20.312074Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The massless thermal field and the thermal fermion bosonization in two dimensions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Emil Akhmedov, Henri Epstein, Ugo Moschella","submitted_at":"2022-03-05T13:58:22Z","abstract_excerpt":"We come back to the issue of bosonization of fermions in two spacetime dimension and give a new costruction in the steady state case where left and right moving particles can coexist at two different temperatures. A crucial role in our construction is played by translation invariant infrared states and the corresponding field operators which are naturally linked to the infrared behaviour of the correlation functions. We present two applications: a simple new derivation in the free relativistic case of a formula by Bernard and Doyon and a full operator solution of the massless Thirring model in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.02747","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2203.02747/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2203.02747","created_at":"2026-07-05T05:01:20.312142+00:00"},{"alias_kind":"arxiv_version","alias_value":"2203.02747v2","created_at":"2026-07-05T05:01:20.312142+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.02747","created_at":"2026-07-05T05:01:20.312142+00:00"},{"alias_kind":"pith_short_12","alias_value":"YR3F2YOBDKJZ","created_at":"2026-07-05T05:01:20.312142+00:00"},{"alias_kind":"pith_short_16","alias_value":"YR3F2YOBDKJZFQY6","created_at":"2026-07-05T05:01:20.312142+00:00"},{"alias_kind":"pith_short_8","alias_value":"YR3F2YOB","created_at":"2026-07-05T05:01:20.312142+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2509.02181","citing_title":"On the late time behavior of thermal two point function in curved space-time","ref_index":5,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD","json":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD.json","graph_json":"https://pith.science/api/pith-number/YR3F2YOBDKJZFQY6D6JR7OUGBD/graph.json","events_json":"https://pith.science/api/pith-number/YR3F2YOBDKJZFQY6D6JR7OUGBD/events.json","paper":"https://pith.science/paper/YR3F2YOB"},"agent_actions":{"view_html":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD","download_json":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD.json","view_paper":"https://pith.science/paper/YR3F2YOB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2203.02747&json=true","fetch_graph":"https://pith.science/api/pith-number/YR3F2YOBDKJZFQY6D6JR7OUGBD/graph.json","fetch_events":"https://pith.science/api/pith-number/YR3F2YOBDKJZFQY6D6JR7OUGBD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD/action/storage_attestation","attest_author":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD/action/author_attestation","sign_citation":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD/action/citation_signature","submit_replication":"https://pith.science/pith/YR3F2YOBDKJZFQY6D6JR7OUGBD/action/replication_record"}},"created_at":"2026-07-05T05:01:20.312142+00:00","updated_at":"2026-07-05T05:01:20.312142+00:00"}