{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:MXA3NG3JIGQM6732IISOCB5WSS","short_pith_number":"pith:MXA3NG3J","schema_version":"1.0","canonical_sha256":"65c1b69b6941a0cf7f7a4224e107b6948215cb19e458b3aa69106560854d583b","source":{"kind":"arxiv","id":"0904.4715","version":1},"attestation_state":"computed","paper":{"title":"Resummation of infrared divergences in the free-energy of spin-two fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. G. C. McKeon, F. T. Brandt, J. B. Siqueira, J. Frenkel","submitted_at":"2009-04-29T22:20:52Z","abstract_excerpt":"We derive a closed form expression for the sum of all the infrared divergent contributions to the free-energy of a gas of gravitons. An important ingredient of our calculation is the use of a gauge fixing procedure such that the graviton propagator becomes both traceless and transverse. This has been shown to be possible, in a previous work, using a general gauge fixing procedure, in the context of the lowest order expansion of the Einstein-Hilbert action, describing non-interacting spin two fields. In order to encompass the problems involving thermal loops, such as the resummation of the free"},"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":"0904.4715","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-04-29T22:20:52Z","cross_cats_sorted":[],"title_canon_sha256":"17bbf4094c0a2440561c333b12e23b43b650ee9c6b15a5e6fc78919669024c2a","abstract_canon_sha256":"5547d55f93ca1ba6550b28d354f927a51b612abb049103927dffe869f8ac7d06"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:59.452624Z","signature_b64":"p4kpu+ZVgi/5r7MXizrgZ9kMWtuQuUuUARFtAp/VNhBISNP+0Jb0bU3cttdxSXSouezjqxhpjced0RwXpIkADg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"65c1b69b6941a0cf7f7a4224e107b6948215cb19e458b3aa69106560854d583b","last_reissued_at":"2026-05-18T02:34:59.452170Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:59.452170Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resummation of infrared divergences in the free-energy of spin-two fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. G. C. McKeon, F. T. Brandt, J. B. Siqueira, J. Frenkel","submitted_at":"2009-04-29T22:20:52Z","abstract_excerpt":"We derive a closed form expression for the sum of all the infrared divergent contributions to the free-energy of a gas of gravitons. An important ingredient of our calculation is the use of a gauge fixing procedure such that the graviton propagator becomes both traceless and transverse. This has been shown to be possible, in a previous work, using a general gauge fixing procedure, in the context of the lowest order expansion of the Einstein-Hilbert action, describing non-interacting spin two fields. In order to encompass the problems involving thermal loops, such as the resummation of the free"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.4715","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0904.4715","created_at":"2026-05-18T02:34:59.452235+00:00"},{"alias_kind":"arxiv_version","alias_value":"0904.4715v1","created_at":"2026-05-18T02:34:59.452235+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.4715","created_at":"2026-05-18T02:34:59.452235+00:00"},{"alias_kind":"pith_short_12","alias_value":"MXA3NG3JIGQM","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_16","alias_value":"MXA3NG3JIGQM6732","created_at":"2026-05-18T12:26:00.592388+00:00"},{"alias_kind":"pith_short_8","alias_value":"MXA3NG3J","created_at":"2026-05-18T12:26:00.592388+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/MXA3NG3JIGQM6732IISOCB5WSS","json":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS.json","graph_json":"https://pith.science/api/pith-number/MXA3NG3JIGQM6732IISOCB5WSS/graph.json","events_json":"https://pith.science/api/pith-number/MXA3NG3JIGQM6732IISOCB5WSS/events.json","paper":"https://pith.science/paper/MXA3NG3J"},"agent_actions":{"view_html":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS","download_json":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS.json","view_paper":"https://pith.science/paper/MXA3NG3J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0904.4715&json=true","fetch_graph":"https://pith.science/api/pith-number/MXA3NG3JIGQM6732IISOCB5WSS/graph.json","fetch_events":"https://pith.science/api/pith-number/MXA3NG3JIGQM6732IISOCB5WSS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS/action/storage_attestation","attest_author":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS/action/author_attestation","sign_citation":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS/action/citation_signature","submit_replication":"https://pith.science/pith/MXA3NG3JIGQM6732IISOCB5WSS/action/replication_record"}},"created_at":"2026-05-18T02:34:59.452235+00:00","updated_at":"2026-05-18T02:34:59.452235+00:00"}