{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:SZWTOKKMXSESHEMK7QCWKOURRW","short_pith_number":"pith:SZWTOKKM","canonical_record":{"source":{"id":"1204.5954","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-04-26T15:01:19Z","cross_cats_sorted":[],"title_canon_sha256":"de73ccc6cdac775e2c6ef816ecb07bcea699338621b236df023fbeda21ca141d","abstract_canon_sha256":"87c44a643e62fd5e7a0466fbffc1d067506a0103941882602b3fbd2aec8ebd35"},"schema_version":"1.0"},"canonical_sha256":"966d37294cbc8923918afc05653a918d8a06e0cd137a5b3c0b7f92b2330d3098","source":{"kind":"arxiv","id":"1204.5954","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1204.5954","created_at":"2026-05-18T01:57:43Z"},{"alias_kind":"arxiv_version","alias_value":"1204.5954v2","created_at":"2026-05-18T01:57:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.5954","created_at":"2026-05-18T01:57:43Z"},{"alias_kind":"pith_short_12","alias_value":"SZWTOKKMXSES","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"SZWTOKKMXSESHEMK","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"SZWTOKKM","created_at":"2026-05-18T12:27:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:SZWTOKKMXSESHEMK7QCWKOURRW","target":"record","payload":{"canonical_record":{"source":{"id":"1204.5954","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-04-26T15:01:19Z","cross_cats_sorted":[],"title_canon_sha256":"de73ccc6cdac775e2c6ef816ecb07bcea699338621b236df023fbeda21ca141d","abstract_canon_sha256":"87c44a643e62fd5e7a0466fbffc1d067506a0103941882602b3fbd2aec8ebd35"},"schema_version":"1.0"},"canonical_sha256":"966d37294cbc8923918afc05653a918d8a06e0cd137a5b3c0b7f92b2330d3098","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:57:43.793097Z","signature_b64":"Df49KLKvt++BTKlOtBSDhV2HdPguRF2CBVTJZYBV9t/eZsUxDTvWw87X3296Ftfr/9oBol1lTKqvr1koxSDgDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"966d37294cbc8923918afc05653a918d8a06e0cd137a5b3c0b7f92b2330d3098","last_reissued_at":"2026-05-18T01:57:43.792456Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:57:43.792456Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1204.5954","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:57:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"540p0M8Q+qTnDmir+Eqg7UqKLbR1iKidJrUn9uaACHMLtQGYv30BLlyui/TJgJkZ+2ajytW7sgFHRqdHKLhEDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T06:45:34.202470Z"},"content_sha256":"8c87c57b3aaaf81521ae1097449eb0ab304e4813fd9299dcb62937a2768b0991","schema_version":"1.0","event_id":"sha256:8c87c57b3aaaf81521ae1097449eb0ab304e4813fd9299dcb62937a2768b0991"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:SZWTOKKMXSESHEMK7QCWKOURRW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum theories of (p,q)-forms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Carlo Iazeolla, Fiorenzo Bastianelli, Roberto Bonezzi","submitted_at":"2012-04-26T15:01:19Z","abstract_excerpt":"We describe quantum theories for massless (p,q)-forms living on Kaehler spaces. In particular we consider four different types of quantum theories: two types involve gauge symmetries and two types are simpler theories without gauge invariances. The latter can be seen as building blocks of the former. Their equations of motion can be obtained in a natural way by first-quantizing a spinning particle with a U(2)-extended supersymmetry on the worldline. The particle system contains four supersymmetric charges, represented quantum mechanically by the Dolbeault operators and their hermitian conjugat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.5954","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:57:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+dsMoFB6AWjaNET0ILbBSRs6Pb/M9DIffaNdhLXvf9GG71k3OmzBY50AjI/8x7zxjGIjKuQZ2izRsdnvX4mTCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-21T06:45:34.202829Z"},"content_sha256":"0843bad86a5c353e951f99d8e78df084184317818de74b7fdb79e05daf491377","schema_version":"1.0","event_id":"sha256:0843bad86a5c353e951f99d8e78df084184317818de74b7fdb79e05daf491377"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SZWTOKKMXSESHEMK7QCWKOURRW/bundle.json","state_url":"https://pith.science/pith/SZWTOKKMXSESHEMK7QCWKOURRW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SZWTOKKMXSESHEMK7QCWKOURRW/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":"2026-05-21T06:45:34Z","links":{"resolver":"https://pith.science/pith/SZWTOKKMXSESHEMK7QCWKOURRW","bundle":"https://pith.science/pith/SZWTOKKMXSESHEMK7QCWKOURRW/bundle.json","state":"https://pith.science/pith/SZWTOKKMXSESHEMK7QCWKOURRW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SZWTOKKMXSESHEMK7QCWKOURRW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:SZWTOKKMXSESHEMK7QCWKOURRW","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":"87c44a643e62fd5e7a0466fbffc1d067506a0103941882602b3fbd2aec8ebd35","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-04-26T15:01:19Z","title_canon_sha256":"de73ccc6cdac775e2c6ef816ecb07bcea699338621b236df023fbeda21ca141d"},"schema_version":"1.0","source":{"id":"1204.5954","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1204.5954","created_at":"2026-05-18T01:57:43Z"},{"alias_kind":"arxiv_version","alias_value":"1204.5954v2","created_at":"2026-05-18T01:57:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.5954","created_at":"2026-05-18T01:57:43Z"},{"alias_kind":"pith_short_12","alias_value":"SZWTOKKMXSES","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"SZWTOKKMXSESHEMK","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"SZWTOKKM","created_at":"2026-05-18T12:27:23Z"}],"graph_snapshots":[{"event_id":"sha256:0843bad86a5c353e951f99d8e78df084184317818de74b7fdb79e05daf491377","target":"graph","created_at":"2026-05-18T01:57:43Z","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"},"paper":{"abstract_excerpt":"We describe quantum theories for massless (p,q)-forms living on Kaehler spaces. In particular we consider four different types of quantum theories: two types involve gauge symmetries and two types are simpler theories without gauge invariances. The latter can be seen as building blocks of the former. Their equations of motion can be obtained in a natural way by first-quantizing a spinning particle with a U(2)-extended supersymmetry on the worldline. The particle system contains four supersymmetric charges, represented quantum mechanically by the Dolbeault operators and their hermitian conjugat","authors_text":"Carlo Iazeolla, Fiorenzo Bastianelli, Roberto Bonezzi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-04-26T15:01:19Z","title":"Quantum theories of (p,q)-forms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.5954","kind":"arxiv","version":2},"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":"sha256:8c87c57b3aaaf81521ae1097449eb0ab304e4813fd9299dcb62937a2768b0991","target":"record","created_at":"2026-05-18T01:57:43Z","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":"87c44a643e62fd5e7a0466fbffc1d067506a0103941882602b3fbd2aec8ebd35","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-04-26T15:01:19Z","title_canon_sha256":"de73ccc6cdac775e2c6ef816ecb07bcea699338621b236df023fbeda21ca141d"},"schema_version":"1.0","source":{"id":"1204.5954","kind":"arxiv","version":2}},"canonical_sha256":"966d37294cbc8923918afc05653a918d8a06e0cd137a5b3c0b7f92b2330d3098","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"966d37294cbc8923918afc05653a918d8a06e0cd137a5b3c0b7f92b2330d3098","first_computed_at":"2026-05-18T01:57:43.792456Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:57:43.792456Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Df49KLKvt++BTKlOtBSDhV2HdPguRF2CBVTJZYBV9t/eZsUxDTvWw87X3296Ftfr/9oBol1lTKqvr1koxSDgDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:57:43.793097Z","signed_message":"canonical_sha256_bytes"},"source_id":"1204.5954","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8c87c57b3aaaf81521ae1097449eb0ab304e4813fd9299dcb62937a2768b0991","sha256:0843bad86a5c353e951f99d8e78df084184317818de74b7fdb79e05daf491377"],"state_sha256":"5916a4248baa30a4947cb98740f8e1fc867c1a37fab7f7c3f3421f32640a1e3a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XDkRw0FCOlN4C5jnqwEXDJpv1h/8LRGc1A1de+qr1RQrMgN0SKDO64NIu2C2JM+349zwGG9sHk71ksAyNqa7BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-21T06:45:34.204823Z","bundle_sha256":"8b758cddebf698f785723da4ecebb4a2daf2ccf568a27e681979ac1b6dab4641"}}