{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:JOWN7RZPSZ37YNXXDRJ5JFU4SP","short_pith_number":"pith:JOWN7RZP","canonical_record":{"source":{"id":"1106.2017","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-06-10T11:17:07Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"93c4cec7d8ad2593b914903dd9c512c2f3abce190999d61f2f6eb44e2c27ebd4","abstract_canon_sha256":"a5047e874f111628cab4b01b38cfee4e501cd55323f3f3894e35c9272ad08649"},"schema_version":"1.0"},"canonical_sha256":"4bacdfc72f9677fc36f71c53d4969c93dd1c8b8833e3a6646ea83ca630320b6d","source":{"kind":"arxiv","id":"1106.2017","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.2017","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"arxiv_version","alias_value":"1106.2017v3","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.2017","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"pith_short_12","alias_value":"JOWN7RZPSZ37","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"JOWN7RZPSZ37YNXX","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"JOWN7RZP","created_at":"2026-05-18T12:26:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:JOWN7RZPSZ37YNXXDRJ5JFU4SP","target":"record","payload":{"canonical_record":{"source":{"id":"1106.2017","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-06-10T11:17:07Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"93c4cec7d8ad2593b914903dd9c512c2f3abce190999d61f2f6eb44e2c27ebd4","abstract_canon_sha256":"a5047e874f111628cab4b01b38cfee4e501cd55323f3f3894e35c9272ad08649"},"schema_version":"1.0"},"canonical_sha256":"4bacdfc72f9677fc36f71c53d4969c93dd1c8b8833e3a6646ea83ca630320b6d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:40.080682Z","signature_b64":"UxLuFJevDTkzBP9IAAZhPjMGpcGwCFtg1nNtL0/cIoo5QhTlw1V5/uwvSOfWm3Sgj2X/+C6Uzugtz7exxSMeCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4bacdfc72f9677fc36f71c53d4969c93dd1c8b8833e3a6646ea83ca630320b6d","last_reissued_at":"2026-05-18T02:01:40.080246Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:40.080246Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1106.2017","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:01:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z8i8muW+Swuyb6WTsA4xWY51U20xrZ/jKoMDonBGd/YJuwXVY/v/5PeWvFSTkFpdyn5NAkoGEWpNdju4OIV1AA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T13:16:49.450622Z"},"content_sha256":"4815f98c46b7360425de1eb7b283bdf3786da0195c2a3a4570e9c60109926bb5","schema_version":"1.0","event_id":"sha256:4815f98c46b7360425de1eb7b283bdf3786da0195c2a3a4570e9c60109926bb5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:JOWN7RZPSZ37YNXXDRJ5JFU4SP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Klein-Gordon-Wheeler-DeWitt-Schroedinger Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Matej Pavsic","submitted_at":"2011-06-10T11:17:07Z","abstract_excerpt":"We start from the Einstein-Hilbert action for the gravitational field in the presence of a \"point particle\" source, and cast the action into the corresponding phase space form. The dynamical variables of such a system satisfy the point particle mass shell constraint, the Hamilton and the momentum constraints of the canonical gravity. In the quantized theory, those constraints become operators that annihilate a state. A state can be represented by a wave functional $\\Psi$ that simultaneously satisfies the Klein-Gordon and the Wheeler-DeWitt-Schr\\\"odinger equation. The latter equation, besides t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.2017","kind":"arxiv","version":3},"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":"2026-05-18T02:01:40Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EnxDfRrgfSe4kcQIUpyzqqiwJcPNnQSUxZjPT5v4gk+l3q9goa8XXw2v3C5d5igFrrTMv0LMN7jfFM4Q6ZvNBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T13:16:49.451409Z"},"content_sha256":"8c960433238269ffbd8e61f261238eb85929c3bdfab49847194bfb5e07c224c1","schema_version":"1.0","event_id":"sha256:8c960433238269ffbd8e61f261238eb85929c3bdfab49847194bfb5e07c224c1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP/bundle.json","state_url":"https://pith.science/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP/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":"2026-05-30T13:16:49Z","links":{"resolver":"https://pith.science/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP","bundle":"https://pith.science/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP/bundle.json","state":"https://pith.science/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/JOWN7RZPSZ37YNXXDRJ5JFU4SP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:JOWN7RZPSZ37YNXXDRJ5JFU4SP","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":"a5047e874f111628cab4b01b38cfee4e501cd55323f3f3894e35c9272ad08649","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-06-10T11:17:07Z","title_canon_sha256":"93c4cec7d8ad2593b914903dd9c512c2f3abce190999d61f2f6eb44e2c27ebd4"},"schema_version":"1.0","source":{"id":"1106.2017","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1106.2017","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"arxiv_version","alias_value":"1106.2017v3","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.2017","created_at":"2026-05-18T02:01:40Z"},{"alias_kind":"pith_short_12","alias_value":"JOWN7RZPSZ37","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_16","alias_value":"JOWN7RZPSZ37YNXX","created_at":"2026-05-18T12:26:32Z"},{"alias_kind":"pith_short_8","alias_value":"JOWN7RZP","created_at":"2026-05-18T12:26:32Z"}],"graph_snapshots":[{"event_id":"sha256:8c960433238269ffbd8e61f261238eb85929c3bdfab49847194bfb5e07c224c1","target":"graph","created_at":"2026-05-18T02:01:40Z","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 start from the Einstein-Hilbert action for the gravitational field in the presence of a \"point particle\" source, and cast the action into the corresponding phase space form. The dynamical variables of such a system satisfy the point particle mass shell constraint, the Hamilton and the momentum constraints of the canonical gravity. In the quantized theory, those constraints become operators that annihilate a state. A state can be represented by a wave functional $\\Psi$ that simultaneously satisfies the Klein-Gordon and the Wheeler-DeWitt-Schr\\\"odinger equation. The latter equation, besides t","authors_text":"Matej Pavsic","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-06-10T11:17:07Z","title":"Klein-Gordon-Wheeler-DeWitt-Schroedinger Equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.2017","kind":"arxiv","version":3},"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":"sha256:4815f98c46b7360425de1eb7b283bdf3786da0195c2a3a4570e9c60109926bb5","target":"record","created_at":"2026-05-18T02:01:40Z","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":"a5047e874f111628cab4b01b38cfee4e501cd55323f3f3894e35c9272ad08649","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-06-10T11:17:07Z","title_canon_sha256":"93c4cec7d8ad2593b914903dd9c512c2f3abce190999d61f2f6eb44e2c27ebd4"},"schema_version":"1.0","source":{"id":"1106.2017","kind":"arxiv","version":3}},"canonical_sha256":"4bacdfc72f9677fc36f71c53d4969c93dd1c8b8833e3a6646ea83ca630320b6d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4bacdfc72f9677fc36f71c53d4969c93dd1c8b8833e3a6646ea83ca630320b6d","first_computed_at":"2026-05-18T02:01:40.080246Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:01:40.080246Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UxLuFJevDTkzBP9IAAZhPjMGpcGwCFtg1nNtL0/cIoo5QhTlw1V5/uwvSOfWm3Sgj2X/+C6Uzugtz7exxSMeCw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:01:40.080682Z","signed_message":"canonical_sha256_bytes"},"source_id":"1106.2017","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4815f98c46b7360425de1eb7b283bdf3786da0195c2a3a4570e9c60109926bb5","sha256:8c960433238269ffbd8e61f261238eb85929c3bdfab49847194bfb5e07c224c1"],"state_sha256":"5f825522ef3b7cc1879eb44140bbf0016a536c9558ad661fb5dbe48e65028989"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZsxGqWMqUvbqahZifGFbfw1fx2nMfjtDxZVnE035VT8tIz4iwevuP0B5g7Q0MYfTs8E3Tj3D8a0oEL8hROtqBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T13:16:49.455299Z","bundle_sha256":"0f3c01fe456a14c3eed83d3136ff4233040724c3725322ea5100b1e4694ea5fc"}}