{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:XLUSE6ESWDXEJHNTUAICBLRVQV","short_pith_number":"pith:XLUSE6ES","canonical_record":{"source":{"id":"2501.01624","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-01-03T03:45:13Z","cross_cats_sorted":[],"title_canon_sha256":"e6b8cb630ec533ebcb327f9afe3dd57f9a6a4c571f4107ab4e07646687e56605","abstract_canon_sha256":"4c73bf2e2e8cb62dcf941d61aa3e024798d67a8eae4415c4e07e8492d640bc9f"},"schema_version":"1.0"},"canonical_sha256":"bae9227892b0ee449db3a01020ae35856b4022939c5013a8a0f44d5ecaac0bc7","source":{"kind":"arxiv","id":"2501.01624","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.01624","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"arxiv_version","alias_value":"2501.01624v1","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.01624","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"pith_short_12","alias_value":"XLUSE6ESWDXE","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"pith_short_16","alias_value":"XLUSE6ESWDXEJHNT","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"pith_short_8","alias_value":"XLUSE6ES","created_at":"2026-07-05T11:20:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:XLUSE6ESWDXEJHNTUAICBLRVQV","target":"record","payload":{"canonical_record":{"source":{"id":"2501.01624","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-01-03T03:45:13Z","cross_cats_sorted":[],"title_canon_sha256":"e6b8cb630ec533ebcb327f9afe3dd57f9a6a4c571f4107ab4e07646687e56605","abstract_canon_sha256":"4c73bf2e2e8cb62dcf941d61aa3e024798d67a8eae4415c4e07e8492d640bc9f"},"schema_version":"1.0"},"canonical_sha256":"bae9227892b0ee449db3a01020ae35856b4022939c5013a8a0f44d5ecaac0bc7","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:20:07.709670Z","signature_b64":"QJE/WVidzLLxfXK7tg4ZmonEdbx78YWNqCUIL2FZNShtvDgoehIXAvfCBzt1LBF/hTCrw1WGdiT97ISVn5tKDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bae9227892b0ee449db3a01020ae35856b4022939c5013a8a0f44d5ecaac0bc7","last_reissued_at":"2026-07-05T11:20:07.709185Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:20:07.709185Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2501.01624","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":"2026-07-05T11:20:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"geDfoGRwGcbAUO58MIr8V1/5bVssqcFJrIwSkpePDot6NTd8hAplj+IwRlllfcfIQXcF0nB9JJRfTsk8E4P2CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-23T22:58:34.376433Z"},"content_sha256":"ee1d3a35f7b453b48f858e48d01b4b588b09ca549bfe81015a95306a557fd908","schema_version":"1.0","event_id":"sha256:ee1d3a35f7b453b48f858e48d01b4b588b09ca549bfe81015a95306a557fd908"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:XLUSE6ESWDXEJHNTUAICBLRVQV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fermionic Casimir effect at finite temperature in Horava-Lifshitz theories","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Andrea Erdas","submitted_at":"2025-01-03T03:45:13Z","abstract_excerpt":"In this work, I study the finite temperature Casimir effect due to a massless fermion field that violates Lorentz invariance according to the Horava-Lifshitz theory. I investigate a fermion field that obeys MIT bag boundary conditions on a pair of parallel plates. I carry out this study using the generalized zeta function technique that enables me to obtain the Helmholtz free energy and the Casimir pressure when the Casimir plates are in thermal equilibrium with a heat reservoir at finite temperature. I investigate the cases when the parameter associated with the violation of Lorentz invarianc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.01624","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.01624/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:20:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fpe3MbB7ijxZ+8zfBTRraYRNqghDWce06W3VdhuPZX3Jo5jaBeDoKUiojiToEzbUpW7cFomjzvn7AOlAawqTBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-23T22:58:34.376927Z"},"content_sha256":"fb7d97a05534d8b551441d7ce7255f2aed7736f8e0caebaf4ca919adb54a1436","schema_version":"1.0","event_id":"sha256:fb7d97a05534d8b551441d7ce7255f2aed7736f8e0caebaf4ca919adb54a1436"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XLUSE6ESWDXEJHNTUAICBLRVQV/bundle.json","state_url":"https://pith.science/pith/XLUSE6ESWDXEJHNTUAICBLRVQV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XLUSE6ESWDXEJHNTUAICBLRVQV/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":"2026-08-23T22:58:34Z","links":{"resolver":"https://pith.science/pith/XLUSE6ESWDXEJHNTUAICBLRVQV","bundle":"https://pith.science/pith/XLUSE6ESWDXEJHNTUAICBLRVQV/bundle.json","state":"https://pith.science/pith/XLUSE6ESWDXEJHNTUAICBLRVQV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XLUSE6ESWDXEJHNTUAICBLRVQV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:XLUSE6ESWDXEJHNTUAICBLRVQV","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":"4c73bf2e2e8cb62dcf941d61aa3e024798d67a8eae4415c4e07e8492d640bc9f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-01-03T03:45:13Z","title_canon_sha256":"e6b8cb630ec533ebcb327f9afe3dd57f9a6a4c571f4107ab4e07646687e56605"},"schema_version":"1.0","source":{"id":"2501.01624","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.01624","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"arxiv_version","alias_value":"2501.01624v1","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.01624","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"pith_short_12","alias_value":"XLUSE6ESWDXE","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"pith_short_16","alias_value":"XLUSE6ESWDXEJHNT","created_at":"2026-07-05T11:20:07Z"},{"alias_kind":"pith_short_8","alias_value":"XLUSE6ES","created_at":"2026-07-05T11:20:07Z"}],"graph_snapshots":[{"event_id":"sha256:fb7d97a05534d8b551441d7ce7255f2aed7736f8e0caebaf4ca919adb54a1436","target":"graph","created_at":"2026-07-05T11:20:07Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2501.01624/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work, I study the finite temperature Casimir effect due to a massless fermion field that violates Lorentz invariance according to the Horava-Lifshitz theory. I investigate a fermion field that obeys MIT bag boundary conditions on a pair of parallel plates. I carry out this study using the generalized zeta function technique that enables me to obtain the Helmholtz free energy and the Casimir pressure when the Casimir plates are in thermal equilibrium with a heat reservoir at finite temperature. I investigate the cases when the parameter associated with the violation of Lorentz invarianc","authors_text":"Andrea Erdas","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-01-03T03:45:13Z","title":"Fermionic Casimir effect at finite temperature in Horava-Lifshitz theories"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.01624","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:ee1d3a35f7b453b48f858e48d01b4b588b09ca549bfe81015a95306a557fd908","target":"record","created_at":"2026-07-05T11:20:07Z","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":"4c73bf2e2e8cb62dcf941d61aa3e024798d67a8eae4415c4e07e8492d640bc9f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2025-01-03T03:45:13Z","title_canon_sha256":"e6b8cb630ec533ebcb327f9afe3dd57f9a6a4c571f4107ab4e07646687e56605"},"schema_version":"1.0","source":{"id":"2501.01624","kind":"arxiv","version":1}},"canonical_sha256":"bae9227892b0ee449db3a01020ae35856b4022939c5013a8a0f44d5ecaac0bc7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bae9227892b0ee449db3a01020ae35856b4022939c5013a8a0f44d5ecaac0bc7","first_computed_at":"2026-07-05T11:20:07.709185Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:20:07.709185Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QJE/WVidzLLxfXK7tg4ZmonEdbx78YWNqCUIL2FZNShtvDgoehIXAvfCBzt1LBF/hTCrw1WGdiT97ISVn5tKDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:20:07.709670Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.01624","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ee1d3a35f7b453b48f858e48d01b4b588b09ca549bfe81015a95306a557fd908","sha256:fb7d97a05534d8b551441d7ce7255f2aed7736f8e0caebaf4ca919adb54a1436"],"state_sha256":"01a56a26a8aed848d95ac25d55b8d9c43f0a9cd1ab0f3aed5c3d5de4ee3900dd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZL3Wq5iHZCp3kNIYSUh9H03sUYVZRDc3oN/tEsZLjwe13X5D0EL9oQtdJQ7hqJ9pgreLnZc/8zMNLK8XI6dnBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-23T22:58:34.381416Z","bundle_sha256":"dc0588d7155cd9f419427732ecdb4ed0070dbc832a040ae10f0c6773714d2f4a"}}