{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2008:6BTCXLAM3UBXOCM5GKBVCCAICH","short_pith_number":"pith:6BTCXLAM","canonical_record":{"source":{"id":"0805.4038","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-05-27T02:39:45Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","quant-ph"],"title_canon_sha256":"34c424e9bdc7cea00f7cf0e2e295db1ad10fd3c2ce9641e6821c5f1b4c7eb6cb","abstract_canon_sha256":"07f72c626fa098b409b6a3c54e280ddd177d68db5a414f32950be7d426a64c16"},"schema_version":"1.0"},"canonical_sha256":"f0662bac0cdd0377099d328351080811ece95860940bdd7eb3697884dfdf450d","source":{"kind":"arxiv","id":"0805.4038","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0805.4038","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"arxiv_version","alias_value":"0805.4038v1","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0805.4038","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"pith_short_12","alias_value":"6BTCXLAM3UBX","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"pith_short_16","alias_value":"6BTCXLAM3UBXOCM5","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"pith_short_8","alias_value":"6BTCXLAM","created_at":"2026-07-04T15:30:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2008:6BTCXLAM3UBXOCM5GKBVCCAICH","target":"record","payload":{"canonical_record":{"source":{"id":"0805.4038","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-05-27T02:39:45Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","quant-ph"],"title_canon_sha256":"34c424e9bdc7cea00f7cf0e2e295db1ad10fd3c2ce9641e6821c5f1b4c7eb6cb","abstract_canon_sha256":"07f72c626fa098b409b6a3c54e280ddd177d68db5a414f32950be7d426a64c16"},"schema_version":"1.0"},"canonical_sha256":"f0662bac0cdd0377099d328351080811ece95860940bdd7eb3697884dfdf450d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:30:11.396841Z","signature_b64":"fdBshh9/EKCAqX/OL2khvUGHvx9xFTvAOJ0n08CKpxzdNbzn/tjK60DGuGMhhbRIpWGOEa8wNd+dVE7MDBUYCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f0662bac0cdd0377099d328351080811ece95860940bdd7eb3697884dfdf450d","last_reissued_at":"2026-07-04T15:30:11.396453Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:30:11.396453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0805.4038","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":"2026-07-04T15:30:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l69YmWpG7nfP8zgyomP7KoUfHoIW5DQN71um5WRgkntdv1ieHRrkaXdSkvpQ0bmShZKQ4hASiHQpQ+6xnBhcBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T15:07:46.260308Z"},"content_sha256":"b15c89e486471b72aa9fda0e86ce5076d1034492ac7cfc79dd113d2036963b24","schema_version":"1.0","event_id":"sha256:b15c89e486471b72aa9fda0e86ce5076d1034492ac7cfc79dd113d2036963b24"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2008:6BTCXLAM3UBXOCM5GKBVCCAICH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The perfect magnetic conductor (PMC) Casimir piston in d+1 dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","quant-ph"],"primary_cat":"hep-th","authors_text":"A. Edery, V. Marachevsky","submitted_at":"2008-05-27T02:39:45Z","abstract_excerpt":"Perfect magnetic conductor (PMC) boundary conditions are dual to the more familiar perfect electric conductor (PEC) conditions and can be viewed as the electromagnetic analog of the boundary conditions in the bag model for hadrons in QCD. Recent advances and requirements in communication technologies have attracted great interest in PMC's and Casimir experiments involving structures that approximate PMC's may be carried out in the not too distant future. In this paper, we make a study of the zero-temperature PMC Casimir piston in $d+1$ dimensions. The PMC Casimir energy is explicitly evaluated"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0805.4038","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/0805.4038/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":"2026-07-04T15:30:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wrsM1TIgdabifF43lFF3AZkjpFYMsnuGWSKpjs+CL7zAdA0NWQfQVwVrw0IC4RJZCVqnl7LVpOO9luX2bePvCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-12T15:07:46.261061Z"},"content_sha256":"2b04fc4bacd90c26fdea25cd62d4ed1434d7696f8a3cbea737f2f709c2e5d59e","schema_version":"1.0","event_id":"sha256:2b04fc4bacd90c26fdea25cd62d4ed1434d7696f8a3cbea737f2f709c2e5d59e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6BTCXLAM3UBXOCM5GKBVCCAICH/bundle.json","state_url":"https://pith.science/pith/6BTCXLAM3UBXOCM5GKBVCCAICH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6BTCXLAM3UBXOCM5GKBVCCAICH/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":"2026-08-12T15:07:46Z","links":{"resolver":"https://pith.science/pith/6BTCXLAM3UBXOCM5GKBVCCAICH","bundle":"https://pith.science/pith/6BTCXLAM3UBXOCM5GKBVCCAICH/bundle.json","state":"https://pith.science/pith/6BTCXLAM3UBXOCM5GKBVCCAICH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6BTCXLAM3UBXOCM5GKBVCCAICH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2008:6BTCXLAM3UBXOCM5GKBVCCAICH","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":"07f72c626fa098b409b6a3c54e280ddd177d68db5a414f32950be7d426a64c16","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-05-27T02:39:45Z","title_canon_sha256":"34c424e9bdc7cea00f7cf0e2e295db1ad10fd3c2ce9641e6821c5f1b4c7eb6cb"},"schema_version":"1.0","source":{"id":"0805.4038","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0805.4038","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"arxiv_version","alias_value":"0805.4038v1","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0805.4038","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"pith_short_12","alias_value":"6BTCXLAM3UBX","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"pith_short_16","alias_value":"6BTCXLAM3UBXOCM5","created_at":"2026-07-04T15:30:11Z"},{"alias_kind":"pith_short_8","alias_value":"6BTCXLAM","created_at":"2026-07-04T15:30:11Z"}],"graph_snapshots":[{"event_id":"sha256:2b04fc4bacd90c26fdea25cd62d4ed1434d7696f8a3cbea737f2f709c2e5d59e","target":"graph","created_at":"2026-07-04T15:30:11Z","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/0805.4038/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Perfect magnetic conductor (PMC) boundary conditions are dual to the more familiar perfect electric conductor (PEC) conditions and can be viewed as the electromagnetic analog of the boundary conditions in the bag model for hadrons in QCD. Recent advances and requirements in communication technologies have attracted great interest in PMC's and Casimir experiments involving structures that approximate PMC's may be carried out in the not too distant future. In this paper, we make a study of the zero-temperature PMC Casimir piston in $d+1$ dimensions. The PMC Casimir energy is explicitly evaluated","authors_text":"A. Edery, V. Marachevsky","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-05-27T02:39:45Z","title":"The perfect magnetic conductor (PMC) Casimir piston in d+1 dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0805.4038","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:b15c89e486471b72aa9fda0e86ce5076d1034492ac7cfc79dd113d2036963b24","target":"record","created_at":"2026-07-04T15:30:11Z","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":"07f72c626fa098b409b6a3c54e280ddd177d68db5a414f32950be7d426a64c16","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2008-05-27T02:39:45Z","title_canon_sha256":"34c424e9bdc7cea00f7cf0e2e295db1ad10fd3c2ce9641e6821c5f1b4c7eb6cb"},"schema_version":"1.0","source":{"id":"0805.4038","kind":"arxiv","version":1}},"canonical_sha256":"f0662bac0cdd0377099d328351080811ece95860940bdd7eb3697884dfdf450d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f0662bac0cdd0377099d328351080811ece95860940bdd7eb3697884dfdf450d","first_computed_at":"2026-07-04T15:30:11.396453Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:30:11.396453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fdBshh9/EKCAqX/OL2khvUGHvx9xFTvAOJ0n08CKpxzdNbzn/tjK60DGuGMhhbRIpWGOEa8wNd+dVE7MDBUYCA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:30:11.396841Z","signed_message":"canonical_sha256_bytes"},"source_id":"0805.4038","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b15c89e486471b72aa9fda0e86ce5076d1034492ac7cfc79dd113d2036963b24","sha256:2b04fc4bacd90c26fdea25cd62d4ed1434d7696f8a3cbea737f2f709c2e5d59e"],"state_sha256":"72faaca92774f2adf0307cd9355e52e55a464dd12cce674ed4c407aa05b57b9e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZveBp/cXb4CpO9vCwevHM9Sw6tra5qUVF7s4dfPdnwPhPkiOejT2/9v6ptEiEf2qNYyOBODmOnCTaF3TCJczDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-12T15:07:46.268112Z","bundle_sha256":"279755180797f33ca47ef56567234aab74bac728f26eaa3fc2bf584147525a22"}}