{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1993:DXA4DTABSOF5D5HIPWBYY2RRAJ","short_pith_number":"pith:DXA4DTAB","canonical_record":{"source":{"id":"hep-th/9306007","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-06-01T19:41:04Z","cross_cats_sorted":["cond-mat","nucl-th"],"title_canon_sha256":"a9d06d71d8e2858d40b8b3c7c4ac4ff654ee6ab0fb89e753ca87fda075cb277a","abstract_canon_sha256":"056f3c4fb0f34ed4fa9dd40c148d239c220d7ab668226dcafe0b5805df1a123f"},"schema_version":"1.0"},"canonical_sha256":"1dc1c1cc01938bd1f4e87d838c6a31026f8866c2391a27436ab3cdd97cd09b06","source":{"kind":"arxiv","id":"hep-th/9306007","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9306007","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9306007v1","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9306007","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"pith_short_12","alias_value":"DXA4DTABSOF5","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"pith_short_16","alias_value":"DXA4DTABSOF5D5HI","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"pith_short_8","alias_value":"DXA4DTAB","created_at":"2026-07-04T15:56:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1993:DXA4DTABSOF5D5HIPWBYY2RRAJ","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9306007","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1993-06-01T19:41:04Z","cross_cats_sorted":["cond-mat","nucl-th"],"title_canon_sha256":"a9d06d71d8e2858d40b8b3c7c4ac4ff654ee6ab0fb89e753ca87fda075cb277a","abstract_canon_sha256":"056f3c4fb0f34ed4fa9dd40c148d239c220d7ab668226dcafe0b5805df1a123f"},"schema_version":"1.0"},"canonical_sha256":"1dc1c1cc01938bd1f4e87d838c6a31026f8866c2391a27436ab3cdd97cd09b06","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:56:14.521759Z","signature_b64":"bS1CD1zOv1E/dJc8lpm0YdLlCWmcuO3fp4RQR2MPBtcHx4JHaucb2eq7hfsd6ARSK58JXwhzpF96cXKK0571Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1dc1c1cc01938bd1f4e87d838c6a31026f8866c2391a27436ab3cdd97cd09b06","last_reissued_at":"2026-07-04T15:56:14.521380Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:56:14.521380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9306007","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":"2026-07-04T15:56:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0rMcbU921TLeZM8pnf9mVjymeGTA6e60UnqDIA5wt/+NuXiGvwsVS8b540S80g5tGOZBX+NkFVCQmNxBnSkIBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T06:55:32.610767Z"},"content_sha256":"3de4f9241bd3b6b528d22083e527e3f012daad203b9ef62b683db44bd4cef057","schema_version":"1.0","event_id":"sha256:3de4f9241bd3b6b528d22083e527e3f012daad203b9ef62b683db44bd4cef057"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1993:DXA4DTABSOF5D5HIPWBYY2RRAJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Transport Properties of Solitons","license":"","headline":"","cross_cats":["cond-mat","nucl-th"],"primary_cat":"hep-th","authors_text":"A.H.Castro Neto, A.O.Caldeira","submitted_at":"1993-06-01T19:41:04Z","abstract_excerpt":"We calculate in this article the transport coefficients which characterize the dynamics of solitons in quantum field theory using the methods of dissipative quantum systems. We show how the damping and diffusion coefficients of soliton-like excitations can be calculated using the integral functional formalism. The model obtained in this article has new features which cannot be obtained in the standard models of dissipation in quantum mechanics."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9306007","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-th/9306007/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":"2026-07-04T15:56:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/ZE/2T/TA5HSIOk1SuhnVN9CWoFOheNYqWJINOrwecm9wgpIhe35gaV262L5idzDtot/BtcQgFQNqm/QbQc+Aw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T06:55:32.611131Z"},"content_sha256":"870b611ec3275e3a4bfa45848cb8bd43a7cab405fc4fb1552968749a0545e738","schema_version":"1.0","event_id":"sha256:870b611ec3275e3a4bfa45848cb8bd43a7cab405fc4fb1552968749a0545e738"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ/bundle.json","state_url":"https://pith.science/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ/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":"2026-07-05T06:55:32Z","links":{"resolver":"https://pith.science/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ","bundle":"https://pith.science/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ/bundle.json","state":"https://pith.science/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DXA4DTABSOF5D5HIPWBYY2RRAJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1993:DXA4DTABSOF5D5HIPWBYY2RRAJ","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":"056f3c4fb0f34ed4fa9dd40c148d239c220d7ab668226dcafe0b5805df1a123f","cross_cats_sorted":["cond-mat","nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"1993-06-01T19:41:04Z","title_canon_sha256":"a9d06d71d8e2858d40b8b3c7c4ac4ff654ee6ab0fb89e753ca87fda075cb277a"},"schema_version":"1.0","source":{"id":"hep-th/9306007","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9306007","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9306007v1","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9306007","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"pith_short_12","alias_value":"DXA4DTABSOF5","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"pith_short_16","alias_value":"DXA4DTABSOF5D5HI","created_at":"2026-07-04T15:56:14Z"},{"alias_kind":"pith_short_8","alias_value":"DXA4DTAB","created_at":"2026-07-04T15:56:14Z"}],"graph_snapshots":[{"event_id":"sha256:870b611ec3275e3a4bfa45848cb8bd43a7cab405fc4fb1552968749a0545e738","target":"graph","created_at":"2026-07-04T15:56:14Z","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-th/9306007/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate in this article the transport coefficients which characterize the dynamics of solitons in quantum field theory using the methods of dissipative quantum systems. We show how the damping and diffusion coefficients of soliton-like excitations can be calculated using the integral functional formalism. The model obtained in this article has new features which cannot be obtained in the standard models of dissipation in quantum mechanics.","authors_text":"A.H.Castro Neto, A.O.Caldeira","cross_cats":["cond-mat","nucl-th"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1993-06-01T19:41:04Z","title":"Transport Properties of Solitons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9306007","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":"sha256:3de4f9241bd3b6b528d22083e527e3f012daad203b9ef62b683db44bd4cef057","target":"record","created_at":"2026-07-04T15:56:14Z","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":"056f3c4fb0f34ed4fa9dd40c148d239c220d7ab668226dcafe0b5805df1a123f","cross_cats_sorted":["cond-mat","nucl-th"],"license":"","primary_cat":"hep-th","submitted_at":"1993-06-01T19:41:04Z","title_canon_sha256":"a9d06d71d8e2858d40b8b3c7c4ac4ff654ee6ab0fb89e753ca87fda075cb277a"},"schema_version":"1.0","source":{"id":"hep-th/9306007","kind":"arxiv","version":1}},"canonical_sha256":"1dc1c1cc01938bd1f4e87d838c6a31026f8866c2391a27436ab3cdd97cd09b06","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1dc1c1cc01938bd1f4e87d838c6a31026f8866c2391a27436ab3cdd97cd09b06","first_computed_at":"2026-07-04T15:56:14.521380Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:56:14.521380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bS1CD1zOv1E/dJc8lpm0YdLlCWmcuO3fp4RQR2MPBtcHx4JHaucb2eq7hfsd6ARSK58JXwhzpF96cXKK0571Aw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:56:14.521759Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9306007","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3de4f9241bd3b6b528d22083e527e3f012daad203b9ef62b683db44bd4cef057","sha256:870b611ec3275e3a4bfa45848cb8bd43a7cab405fc4fb1552968749a0545e738"],"state_sha256":"4a41eee6055a42c394b84b36f14047ba797ad9a28a008407723f1aaa548807bf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vlhQOtACEkP3gG5zoseQfNl/t0gN6brI25gcEprotFmvCfbg+gC92qSM2iTOIgoh8ZTl6cOA4M/QnBfSexzyDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-05T06:55:32.612981Z","bundle_sha256":"72c5ce8e457701fc650cfc607094364f52172bd1ea56abfdf1061c8ef01d0a7c"}}