{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2006:WN3C5LU5YBMN4QDR2BBRUJZWPF","short_pith_number":"pith:WN3C5LU5","canonical_record":{"source":{"id":"hep-ph/0603266","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-31T13:44:23Z","cross_cats_sorted":[],"title_canon_sha256":"ea2bcc61c309ba35137d8ada5de3caf6a96d5bb86530427067c3fed344f0f26a","abstract_canon_sha256":"fbd6d8e3bab180e7f19c60153a957e42e5be608ba399d8ea3f4bc74aff9e9b30"},"schema_version":"1.0"},"canonical_sha256":"b3762eae9dc058de4071d0431a2736795bd835d5e59810d9cbcbad9f5eab063b","source":{"kind":"arxiv","id":"hep-ph/0603266","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0603266","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0603266v1","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0603266","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"pith_short_12","alias_value":"WN3C5LU5YBMN","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"pith_short_16","alias_value":"WN3C5LU5YBMN4QDR","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"pith_short_8","alias_value":"WN3C5LU5","created_at":"2026-07-04T14:53:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2006:WN3C5LU5YBMN4QDR2BBRUJZWPF","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0603266","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-31T13:44:23Z","cross_cats_sorted":[],"title_canon_sha256":"ea2bcc61c309ba35137d8ada5de3caf6a96d5bb86530427067c3fed344f0f26a","abstract_canon_sha256":"fbd6d8e3bab180e7f19c60153a957e42e5be608ba399d8ea3f4bc74aff9e9b30"},"schema_version":"1.0"},"canonical_sha256":"b3762eae9dc058de4071d0431a2736795bd835d5e59810d9cbcbad9f5eab063b","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:53:55.204709Z","signature_b64":"iw/XNVpze3FS7ku8suoDlwwiBFx00mDYsOyWdc3x9lcIyvVyiRH9rFL/suOTGiXgvUQWCxOBGYMWjVvq78pYAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3762eae9dc058de4071d0431a2736795bd835d5e59810d9cbcbad9f5eab063b","last_reissued_at":"2026-07-04T14:53:55.204337Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:53:55.204337Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0603266","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":"2026-07-04T14:53:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Opi1fTYAPNQEmHjL/nBHM0hP0heoiSAIAABZzkEvNmGqIQ0tYkLstQl7e6TPJzG96q4xPHTnmd+LMTj5gzZwAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T23:07:01.894923Z"},"content_sha256":"8f408ae8a53345a18a39853541d0de3e098516a5539650153eb44822dad15232","schema_version":"1.0","event_id":"sha256:8f408ae8a53345a18a39853541d0de3e098516a5539650153eb44822dad15232"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2006:WN3C5LU5YBMN4QDR2BBRUJZWPF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dissipation coefficients for supersymmetric inflatonary models","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Chun Xiong, Ian G Moss","submitted_at":"2006-03-31T13:44:23Z","abstract_excerpt":"Dissipative effects can lead to a friction term in the equation of motion for an inflaton field during the inflationary era. The friction term may be linear and localised, in which case it is described by a dissipation coefficient. The dissipation coefficient is calculated here in a supersymmetric model with a two stage decay process in which the inflaton decays into a thermal gas of light particles through a heavy intermediate. At low temperatures, the dissipation coefficient $\\propto T^3$ in a thermal approximation. Results are also given for a non-equilibrium anzatz. The dissipation coeffic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0603266","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/hep-ph/0603266/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":"2026-07-04T14:53:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vr1xkvp+DbKPtvKe3Vm8xCV+vtBgYJnQQHkJgAPGujRF8TBMJQPdDoKGPjcol9DvXWveDuuUym+7iNzWthcJAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T23:07:01.895500Z"},"content_sha256":"dddb6cd8a35f72ce4c789a997df6ed77b97ae6b4b0339e40d5c898f95c5cdb31","schema_version":"1.0","event_id":"sha256:dddb6cd8a35f72ce4c789a997df6ed77b97ae6b4b0339e40d5c898f95c5cdb31"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF/bundle.json","state_url":"https://pith.science/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF/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":"2026-08-14T23:07:01Z","links":{"resolver":"https://pith.science/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF","bundle":"https://pith.science/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF/bundle.json","state":"https://pith.science/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WN3C5LU5YBMN4QDR2BBRUJZWPF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2006:WN3C5LU5YBMN4QDR2BBRUJZWPF","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":"fbd6d8e3bab180e7f19c60153a957e42e5be608ba399d8ea3f4bc74aff9e9b30","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-31T13:44:23Z","title_canon_sha256":"ea2bcc61c309ba35137d8ada5de3caf6a96d5bb86530427067c3fed344f0f26a"},"schema_version":"1.0","source":{"id":"hep-ph/0603266","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0603266","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0603266v1","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0603266","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"pith_short_12","alias_value":"WN3C5LU5YBMN","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"pith_short_16","alias_value":"WN3C5LU5YBMN4QDR","created_at":"2026-07-04T14:53:55Z"},{"alias_kind":"pith_short_8","alias_value":"WN3C5LU5","created_at":"2026-07-04T14:53:55Z"}],"graph_snapshots":[{"event_id":"sha256:dddb6cd8a35f72ce4c789a997df6ed77b97ae6b4b0339e40d5c898f95c5cdb31","target":"graph","created_at":"2026-07-04T14:53:55Z","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/0603266/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Dissipative effects can lead to a friction term in the equation of motion for an inflaton field during the inflationary era. The friction term may be linear and localised, in which case it is described by a dissipation coefficient. The dissipation coefficient is calculated here in a supersymmetric model with a two stage decay process in which the inflaton decays into a thermal gas of light particles through a heavy intermediate. At low temperatures, the dissipation coefficient $\\propto T^3$ in a thermal approximation. Results are also given for a non-equilibrium anzatz. The dissipation coeffic","authors_text":"Chun Xiong, Ian G Moss","cross_cats":[],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2006-03-31T13:44:23Z","title":"Dissipation coefficients for supersymmetric inflatonary models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0603266","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":"sha256:8f408ae8a53345a18a39853541d0de3e098516a5539650153eb44822dad15232","target":"record","created_at":"2026-07-04T14:53:55Z","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":"fbd6d8e3bab180e7f19c60153a957e42e5be608ba399d8ea3f4bc74aff9e9b30","cross_cats_sorted":[],"license":"","primary_cat":"hep-ph","submitted_at":"2006-03-31T13:44:23Z","title_canon_sha256":"ea2bcc61c309ba35137d8ada5de3caf6a96d5bb86530427067c3fed344f0f26a"},"schema_version":"1.0","source":{"id":"hep-ph/0603266","kind":"arxiv","version":1}},"canonical_sha256":"b3762eae9dc058de4071d0431a2736795bd835d5e59810d9cbcbad9f5eab063b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b3762eae9dc058de4071d0431a2736795bd835d5e59810d9cbcbad9f5eab063b","first_computed_at":"2026-07-04T14:53:55.204337Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T14:53:55.204337Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iw/XNVpze3FS7ku8suoDlwwiBFx00mDYsOyWdc3x9lcIyvVyiRH9rFL/suOTGiXgvUQWCxOBGYMWjVvq78pYAA==","signature_status":"signed_v1","signed_at":"2026-07-04T14:53:55.204709Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0603266","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8f408ae8a53345a18a39853541d0de3e098516a5539650153eb44822dad15232","sha256:dddb6cd8a35f72ce4c789a997df6ed77b97ae6b4b0339e40d5c898f95c5cdb31"],"state_sha256":"3b6daa77c6b7729abfd67dca27e996dc9526688283e0e2bdbbbfd5af3fca5059"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O+4c17Ytoi+LaVjd4h0ifyxUtA74EJWjFa/kRLt4+xem2q26T8GcEPLxTmPRVH/dav8l7p9dvietDV1ypc8SAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T23:07:01.898739Z","bundle_sha256":"b0c32c434610077cb62b1d7282dda8d3a99cd78d4316219140a85c4993b7a29f"}}