{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1996:GHB63ZOT7X7U7B7PWGCMSKM6BW","short_pith_number":"pith:GHB63ZOT","canonical_record":{"source":{"id":"hep-ph/9610477","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-10-24T23:58:32Z","cross_cats_sorted":[],"title_canon_sha256":"aaa838d8cebdc8e554eeb2d1f8f71cb0cd4e6949fca53bd4cc23b7a15e12b172","abstract_canon_sha256":"abf39b4224dc58a436f7e4473bd62500c4ba16a535cdbde25ab21b6bf0a5bb03"},"schema_version":"1.0"},"canonical_sha256":"31c3ede5d3fdff4f87efb184c9299e0d82c4cb7736ce5858c024c8fbe95035dc","source":{"kind":"arxiv","id":"hep-ph/9610477","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9610477","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9610477v3","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9610477","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"pith_short_12","alias_value":"GHB63ZOT7X7U","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"pith_short_16","alias_value":"GHB63ZOT7X7U7B7P","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"pith_short_8","alias_value":"GHB63ZOT","created_at":"2026-07-04T16:01:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1996:GHB63ZOT7X7U7B7PWGCMSKM6BW","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9610477","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1996-10-24T23:58:32Z","cross_cats_sorted":[],"title_canon_sha256":"aaa838d8cebdc8e554eeb2d1f8f71cb0cd4e6949fca53bd4cc23b7a15e12b172","abstract_canon_sha256":"abf39b4224dc58a436f7e4473bd62500c4ba16a535cdbde25ab21b6bf0a5bb03"},"schema_version":"1.0"},"canonical_sha256":"31c3ede5d3fdff4f87efb184c9299e0d82c4cb7736ce5858c024c8fbe95035dc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:01:58.944066Z","signature_b64":"FWvzK3W2uj/A8oAEqoQnIijRFcZfV6iJaSKQQXEiwCtp7eZQHQdS95MgpxdBIe/VQwWeyRaw6AKDe8o/H8fzCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"31c3ede5d3fdff4f87efb184c9299e0d82c4cb7736ce5858c024c8fbe95035dc","last_reissued_at":"2026-07-04T16:01:58.943691Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:01:58.943691Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9610477","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":"2026-07-04T16:01:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gRWeWA6swas1awKpvrqE6xS2SJWQiAZxMdMG+hI5s7gk/BIzBGULdEhJUlrJFFUKp+9vL6LAOpFGkBz31ZI0Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T23:29:52.305337Z"},"content_sha256":"35e94777f11404a56efa3e18a148ef7c5334eaa3d4e4f83c8726cd45f5be1a92","schema_version":"1.0","event_id":"sha256:35e94777f11404a56efa3e18a148ef7c5334eaa3d4e4f83c8726cd45f5be1a92"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1996:GHB63ZOT7X7U7B7PWGCMSKM6BW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Resonant decay of Bose condensates","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"I. I. Tkachev, S. Yu. Khlebnikov","submitted_at":"1996-10-24T23:58:32Z","abstract_excerpt":"We present results of fully non-linear calculations of decay of the inflaton interacting with another scalar field X. Combining numerical results for cosmologically interesting range of resonance parameter, q \\leq 10^6, with analytical estimates, we extrapolate them to larger q. We find that scattering of X fluctuations off the Bose condensate is a very efficient mechanism limiting growth of X fluctuations. For a single-component X, the resulting variance, at large q, is much smaller than that obtained in the Hartree approximation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9610477","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/hep-ph/9610477/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":"2026-07-04T16:01:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b2P6rFot21YJTcysV+XeqMQfZ3lZVHDQGs4GlOKB+xKhij6ZkaZ2ky+jzFhHkTB1zHjx9AE0e1OiFMOBu5pQCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T23:29:52.305886Z"},"content_sha256":"b4ca7024784238e0a4bac2808cd39b946dc25005f9e3e3e4ffc7f8b16093c332","schema_version":"1.0","event_id":"sha256:b4ca7024784238e0a4bac2808cd39b946dc25005f9e3e3e4ffc7f8b16093c332"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW/bundle.json","state_url":"https://pith.science/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW/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":"2026-08-16T23:29:52Z","links":{"resolver":"https://pith.science/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW","bundle":"https://pith.science/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW/bundle.json","state":"https://pith.science/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GHB63ZOT7X7U7B7PWGCMSKM6BW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1996:GHB63ZOT7X7U7B7PWGCMSKM6BW","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":"abf39b4224dc58a436f7e4473bd62500c4ba16a535cdbde25ab21b6bf0a5bb03","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1996-10-24T23:58:32Z","title_canon_sha256":"aaa838d8cebdc8e554eeb2d1f8f71cb0cd4e6949fca53bd4cc23b7a15e12b172"},"schema_version":"1.0","source":{"id":"hep-ph/9610477","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9610477","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9610477v3","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9610477","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"pith_short_12","alias_value":"GHB63ZOT7X7U","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"pith_short_16","alias_value":"GHB63ZOT7X7U7B7P","created_at":"2026-07-04T16:01:58Z"},{"alias_kind":"pith_short_8","alias_value":"GHB63ZOT","created_at":"2026-07-04T16:01:58Z"}],"graph_snapshots":[{"event_id":"sha256:b4ca7024784238e0a4bac2808cd39b946dc25005f9e3e3e4ffc7f8b16093c332","target":"graph","created_at":"2026-07-04T16:01:58Z","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/hep-ph/9610477/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present results of fully non-linear calculations of decay of the inflaton interacting with another scalar field X. Combining numerical results for cosmologically interesting range of resonance parameter, q \\leq 10^6, with analytical estimates, we extrapolate them to larger q. We find that scattering of X fluctuations off the Bose condensate is a very efficient mechanism limiting growth of X fluctuations. For a single-component X, the resulting variance, at large q, is much smaller than that obtained in the Hartree approximation.","authors_text":"I. I. Tkachev, S. Yu. Khlebnikov","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1996-10-24T23:58:32Z","title":"Resonant decay of Bose condensates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9610477","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":"sha256:35e94777f11404a56efa3e18a148ef7c5334eaa3d4e4f83c8726cd45f5be1a92","target":"record","created_at":"2026-07-04T16:01:58Z","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":"abf39b4224dc58a436f7e4473bd62500c4ba16a535cdbde25ab21b6bf0a5bb03","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"1996-10-24T23:58:32Z","title_canon_sha256":"aaa838d8cebdc8e554eeb2d1f8f71cb0cd4e6949fca53bd4cc23b7a15e12b172"},"schema_version":"1.0","source":{"id":"hep-ph/9610477","kind":"arxiv","version":3}},"canonical_sha256":"31c3ede5d3fdff4f87efb184c9299e0d82c4cb7736ce5858c024c8fbe95035dc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"31c3ede5d3fdff4f87efb184c9299e0d82c4cb7736ce5858c024c8fbe95035dc","first_computed_at":"2026-07-04T16:01:58.943691Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:01:58.943691Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FWvzK3W2uj/A8oAEqoQnIijRFcZfV6iJaSKQQXEiwCtp7eZQHQdS95MgpxdBIe/VQwWeyRaw6AKDe8o/H8fzCA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:01:58.944066Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9610477","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:35e94777f11404a56efa3e18a148ef7c5334eaa3d4e4f83c8726cd45f5be1a92","sha256:b4ca7024784238e0a4bac2808cd39b946dc25005f9e3e3e4ffc7f8b16093c332"],"state_sha256":"1692713d158269bedd0ddef297a4be72c97b21a6fbbe89adc37a2bfb790ea4d8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6NN8kc9hfrqKD0gr65K41eTqp6FEJWRiFg8PGOOVt13OZHiugMNELxcmVcx2qNl2nXO3WaAKW/hYOQjSnErqAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T23:29:52.309849Z","bundle_sha256":"4c537c911f57148f75b715e7d21f35f881e8b03879e7c2d99c203a918e1b4181"}}