{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:SAUQ7KKPYKWD5IVKNTJ4LNYUO5","short_pith_number":"pith:SAUQ7KKP","canonical_record":{"source":{"id":"nucl-th/9703046","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1997-03-20T22:58:25Z","cross_cats_sorted":[],"title_canon_sha256":"9fc292a658c702fb31413e96481adb6bf6eec7c0a1150759299ec3f20767b2d8","abstract_canon_sha256":"de2e0387e23a1c9d92469b2ec86843effe8249c80cc18308d93bf05431c41073"},"schema_version":"1.0"},"canonical_sha256":"90290fa94fc2ac3ea2aa6cd3c5b714774d6e1919591ee2f8b2840d4de602aee1","source":{"kind":"arxiv","id":"nucl-th/9703046","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9703046","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9703046v3","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9703046","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"pith_short_12","alias_value":"SAUQ7KKPYKWD","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"pith_short_16","alias_value":"SAUQ7KKPYKWD5IVK","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"pith_short_8","alias_value":"SAUQ7KKP","created_at":"2026-07-04T15:23:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:SAUQ7KKPYKWD5IVKNTJ4LNYUO5","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/9703046","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1997-03-20T22:58:25Z","cross_cats_sorted":[],"title_canon_sha256":"9fc292a658c702fb31413e96481adb6bf6eec7c0a1150759299ec3f20767b2d8","abstract_canon_sha256":"de2e0387e23a1c9d92469b2ec86843effe8249c80cc18308d93bf05431c41073"},"schema_version":"1.0"},"canonical_sha256":"90290fa94fc2ac3ea2aa6cd3c5b714774d6e1919591ee2f8b2840d4de602aee1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:23.428323Z","signature_b64":"9BSJGRmWSVbRyuFO++cBuzv18Do1JHr3iNiIBKEuxvwDuHvAlaJbppUeQGtNms/oleUt3Zf0/kWhccqlWu9yAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"90290fa94fc2ac3ea2aa6cd3c5b714774d6e1919591ee2f8b2840d4de602aee1","last_reissued_at":"2026-07-04T15:23:23.427914Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:23.427914Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/9703046","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":"2026-07-04T15:23:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qQBo4zr5yjmmNoy5DRsKO+aVOYJIgR1qX5G5uech1LU46AxQ6tQfyKpYMt8FjKSwzEX5mXaVXK9NT7dqVMNdCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T22:30:02.750304Z"},"content_sha256":"b391957caf6fc4e42e39dbef401f99c9ded005ac907226313b6b6b5746129e8d","schema_version":"1.0","event_id":"sha256:b391957caf6fc4e42e39dbef401f99c9ded005ac907226313b6b6b5746129e8d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:SAUQ7KKPYKWD5IVKNTJ4LNYUO5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Mechanical Localization Effects for Bose-Einstein Correlations","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"C. Slotta, H. Kalechofsky, M. Martin, P. Foka, Q.H. Zhang, U.A. Wiedemann","submitted_at":"1997-03-20T22:58:25Z","abstract_excerpt":"For a set of N identical massive boson wavepackets with optimal initial quantum mechanical localization, we calculate the Hanbury-Brown/Twiss (HBT) two-particle correlation function. Our result provides an algorithm for calculating one-particle spectra and two-particle correlations from an arbitrary phase space occupation (q_i,p_i,t_i)_{i=1,N} as e.g. returned by event generators. It is a microscopic derivation of the result of the coherent state formalism, providing explicit finite multiplicity corrections. Both the one- and two-particle spectra depend explicitly on the initial spatial wavepa"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9703046","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/nucl-th/9703046/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":"2026-07-04T15:23:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QINRE2MRMHUSNy7CQpxObWluPSpXMBMq1RnYp+hNejqUn35XDU8bb6EtBCbzLtXwhQ+Y/7L5AnkFsJkpeAPGAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T22:30:02.750890Z"},"content_sha256":"15aea59f3bddf72083aa07fcc62f24d8beaac41cccecdf828f7aaceb197f9a5b","schema_version":"1.0","event_id":"sha256:15aea59f3bddf72083aa07fcc62f24d8beaac41cccecdf828f7aaceb197f9a5b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5/bundle.json","state_url":"https://pith.science/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5/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":"2026-08-04T22:30:02Z","links":{"resolver":"https://pith.science/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5","bundle":"https://pith.science/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5/bundle.json","state":"https://pith.science/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SAUQ7KKPYKWD5IVKNTJ4LNYUO5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:SAUQ7KKPYKWD5IVKNTJ4LNYUO5","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":"de2e0387e23a1c9d92469b2ec86843effe8249c80cc18308d93bf05431c41073","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"1997-03-20T22:58:25Z","title_canon_sha256":"9fc292a658c702fb31413e96481adb6bf6eec7c0a1150759299ec3f20767b2d8"},"schema_version":"1.0","source":{"id":"nucl-th/9703046","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/9703046","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9703046v3","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9703046","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"pith_short_12","alias_value":"SAUQ7KKPYKWD","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"pith_short_16","alias_value":"SAUQ7KKPYKWD5IVK","created_at":"2026-07-04T15:23:23Z"},{"alias_kind":"pith_short_8","alias_value":"SAUQ7KKP","created_at":"2026-07-04T15:23:23Z"}],"graph_snapshots":[{"event_id":"sha256:15aea59f3bddf72083aa07fcc62f24d8beaac41cccecdf828f7aaceb197f9a5b","target":"graph","created_at":"2026-07-04T15:23:23Z","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/nucl-th/9703046/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"For a set of N identical massive boson wavepackets with optimal initial quantum mechanical localization, we calculate the Hanbury-Brown/Twiss (HBT) two-particle correlation function. Our result provides an algorithm for calculating one-particle spectra and two-particle correlations from an arbitrary phase space occupation (q_i,p_i,t_i)_{i=1,N} as e.g. returned by event generators. It is a microscopic derivation of the result of the coherent state formalism, providing explicit finite multiplicity corrections. Both the one- and two-particle spectra depend explicitly on the initial spatial wavepa","authors_text":"C. Slotta, H. Kalechofsky, M. Martin, P. Foka, Q.H. Zhang, U.A. Wiedemann","cross_cats":[],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"1997-03-20T22:58:25Z","title":"Quantum Mechanical Localization Effects for Bose-Einstein Correlations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9703046","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:b391957caf6fc4e42e39dbef401f99c9ded005ac907226313b6b6b5746129e8d","target":"record","created_at":"2026-07-04T15:23:23Z","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":"de2e0387e23a1c9d92469b2ec86843effe8249c80cc18308d93bf05431c41073","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"1997-03-20T22:58:25Z","title_canon_sha256":"9fc292a658c702fb31413e96481adb6bf6eec7c0a1150759299ec3f20767b2d8"},"schema_version":"1.0","source":{"id":"nucl-th/9703046","kind":"arxiv","version":3}},"canonical_sha256":"90290fa94fc2ac3ea2aa6cd3c5b714774d6e1919591ee2f8b2840d4de602aee1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"90290fa94fc2ac3ea2aa6cd3c5b714774d6e1919591ee2f8b2840d4de602aee1","first_computed_at":"2026-07-04T15:23:23.427914Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:23:23.427914Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9BSJGRmWSVbRyuFO++cBuzv18Do1JHr3iNiIBKEuxvwDuHvAlaJbppUeQGtNms/oleUt3Zf0/kWhccqlWu9yAw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:23:23.428323Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/9703046","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b391957caf6fc4e42e39dbef401f99c9ded005ac907226313b6b6b5746129e8d","sha256:15aea59f3bddf72083aa07fcc62f24d8beaac41cccecdf828f7aaceb197f9a5b"],"state_sha256":"569e700804d0a715df459cf2ea1b7c37609c53ed6e368ccf3103b9aa88c69733"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TItqWu76HxkinQ2D/V0SMPUKptHveM7NT+vT2xWrDX3W2gvdaHxv6fnjcqk1sOzd8y2cdfMPGvbgCQhT8IbRBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T22:30:02.755147Z","bundle_sha256":"0271ff84209bb022757c46ddd16eb4be143880101dd72d8179c1c931ed73c536"}}