{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:PWOZ5I66AOYXONIKCAV4ENRNJ5","short_pith_number":"pith:PWOZ5I66","schema_version":"1.0","canonical_sha256":"7d9d9ea3de03b177350a102bc2362d4f6a818328059b84f379edd08c31d4af9d","source":{"kind":"arxiv","id":"1412.7463","version":2},"attestation_state":"computed","paper":{"title":"Comments on the Casimir energy in supersymmetric field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dario Martelli, Jakob Lorenzen","submitted_at":"2014-12-23T18:30:13Z","abstract_excerpt":"We study the Casimir energy of four-dimensional supersymmetric gauge theories in the context of the rigid limit of new minimal supergravity. Firstly, revisiting the computation of the localized partition function on $S^1\\times S^3$, we recover the supersymmetric Casimir energy. Secondly, we consider the same theories in the Hamiltonian formalism on $\\mathbb{R}\\times S^3$, focussing on the free limit and including a one-parameter family of background gauge fields along $\\mathbb{R}$. We compute the vacuum expectation value of the canonical Hamiltonian using zeta function regularization, and show"},"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":"1412.7463","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-12-23T18:30:13Z","cross_cats_sorted":[],"title_canon_sha256":"a507f8834a7f3f31be4ad0ce8ed5d090f141c3ca0d3cf1a9ad2f8b7b74d13e0c","abstract_canon_sha256":"60fc7764ef0567966dba574dc70dccc877bd46d66146884ed45abbe60b11430e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:37:11.159690Z","signature_b64":"BAX2AFIg0T3mAe/EEYWdPuRzr/ohFs5unHbKYj6WySFOIWJQpg7PIAH481XB9eRurgx5iWGUBho0vwJ2r+LbAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7d9d9ea3de03b177350a102bc2362d4f6a818328059b84f379edd08c31d4af9d","last_reissued_at":"2026-05-18T01:37:11.158898Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:37:11.158898Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Comments on the Casimir energy in supersymmetric field theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dario Martelli, Jakob Lorenzen","submitted_at":"2014-12-23T18:30:13Z","abstract_excerpt":"We study the Casimir energy of four-dimensional supersymmetric gauge theories in the context of the rigid limit of new minimal supergravity. Firstly, revisiting the computation of the localized partition function on $S^1\\times S^3$, we recover the supersymmetric Casimir energy. Secondly, we consider the same theories in the Hamiltonian formalism on $\\mathbb{R}\\times S^3$, focussing on the free limit and including a one-parameter family of background gauge fields along $\\mathbb{R}$. We compute the vacuum expectation value of the canonical Hamiltonian using zeta function regularization, and show"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.7463","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":"1412.7463","created_at":"2026-05-18T01:37:11.159035+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.7463v2","created_at":"2026-05-18T01:37:11.159035+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.7463","created_at":"2026-05-18T01:37:11.159035+00:00"},{"alias_kind":"pith_short_12","alias_value":"PWOZ5I66AOYX","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PWOZ5I66AOYXONIK","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PWOZ5I66","created_at":"2026-05-18T12:28:43.426989+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/PWOZ5I66AOYXONIKCAV4ENRNJ5","json":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5.json","graph_json":"https://pith.science/api/pith-number/PWOZ5I66AOYXONIKCAV4ENRNJ5/graph.json","events_json":"https://pith.science/api/pith-number/PWOZ5I66AOYXONIKCAV4ENRNJ5/events.json","paper":"https://pith.science/paper/PWOZ5I66"},"agent_actions":{"view_html":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5","download_json":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5.json","view_paper":"https://pith.science/paper/PWOZ5I66","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.7463&json=true","fetch_graph":"https://pith.science/api/pith-number/PWOZ5I66AOYXONIKCAV4ENRNJ5/graph.json","fetch_events":"https://pith.science/api/pith-number/PWOZ5I66AOYXONIKCAV4ENRNJ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5/action/storage_attestation","attest_author":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5/action/author_attestation","sign_citation":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5/action/citation_signature","submit_replication":"https://pith.science/pith/PWOZ5I66AOYXONIKCAV4ENRNJ5/action/replication_record"}},"created_at":"2026-05-18T01:37:11.159035+00:00","updated_at":"2026-05-18T01:37:11.159035+00:00"}