{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:UP6RQTHOPYJCA5V6MUFZ6ZLTBS","short_pith_number":"pith:UP6RQTHO","canonical_record":{"source":{"id":"2411.17368","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-11-26T12:24:52Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"795dbf4b1b1593e428ec7644a7d616965e9629e2a11a3a8cd9e216009b228639","abstract_canon_sha256":"33a6fabbe46e3fa015bed27e8f737a751afc166153533925ace314238cf26399"},"schema_version":"1.0"},"canonical_sha256":"a3fd184cee7e122076be650b9f65730caeff21093ebd454b49f046c781220db0","source":{"kind":"arxiv","id":"2411.17368","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.17368","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"arxiv_version","alias_value":"2411.17368v2","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.17368","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"pith_short_12","alias_value":"UP6RQTHOPYJC","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"pith_short_16","alias_value":"UP6RQTHOPYJCA5V6","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"pith_short_8","alias_value":"UP6RQTHO","created_at":"2026-07-05T10:44:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:UP6RQTHOPYJCA5V6MUFZ6ZLTBS","target":"record","payload":{"canonical_record":{"source":{"id":"2411.17368","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-11-26T12:24:52Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"795dbf4b1b1593e428ec7644a7d616965e9629e2a11a3a8cd9e216009b228639","abstract_canon_sha256":"33a6fabbe46e3fa015bed27e8f737a751afc166153533925ace314238cf26399"},"schema_version":"1.0"},"canonical_sha256":"a3fd184cee7e122076be650b9f65730caeff21093ebd454b49f046c781220db0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:44:20.169209Z","signature_b64":"F7EMZaPHWzgW2D8z9chSRRFi1y+GM0zfftZfAiVztNZLu2PAuqzoqtFH2MjPl8BczZaI/i03o5ObxyKlIlDIDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a3fd184cee7e122076be650b9f65730caeff21093ebd454b49f046c781220db0","last_reissued_at":"2026-07-05T10:44:20.168667Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:44:20.168667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.17368","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T10:44:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZlLuep4/AagnG8fgUC9FtZgEocvSrU4XrHmCTkwdmvWVTmC9OuM5IxVN1fDXzcAwU6+z2gmkG4HVeYLL1PLmDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T08:38:02.594123Z"},"content_sha256":"15581dc50e4a73c038954736425bb7a3ee119228839c2143cc2436ba403e0a5e","schema_version":"1.0","event_id":"sha256:15581dc50e4a73c038954736425bb7a3ee119228839c2143cc2436ba403e0a5e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:UP6RQTHOPYJCA5V6MUFZ6ZLTBS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the distributed resistor-constant phase element transmission line in a reflective bounded domain","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Anis Allagui, Chunlei Wang, Enrique H. Balaguera","submitted_at":"2024-11-26T12:24:52Z","abstract_excerpt":"In this work we derive and study the analytical solution of the voltage and current diffusion equation for the case of a finite-length resistor-constant phase element (CPE) transmission line (TL) network that can represent a model for porous electrodes in the absence of any Faradic processes. The energy storage component is considered to be an elemental CPE per unit length of impedance $z_c(s)={1}/{(c_{\\alpha} s^{\\alpha})}$ with constant parameters $(c_{\\alpha},\\alpha)$ instead of the ideal capacitor of impedance $z(s)={1}/{(c\\, s)}$ usually assumed in TL modeling. The problem becomes a time-f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.17368","kind":"arxiv","version":2},"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/2411.17368/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":"2026-07-05T10:44:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KYRsTtswJQm9a36Fz20LqFcQpgAZwI4kP1zjNwJtmjEEcQl2XrSDl4DxDEHcTrxKlXTY9Gd/TSmo2En2cc9rDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T08:38:02.594959Z"},"content_sha256":"f4841cc4af9ef6805cff6072adea3f320874c96f064d141bc8a495d9af994fa3","schema_version":"1.0","event_id":"sha256:f4841cc4af9ef6805cff6072adea3f320874c96f064d141bc8a495d9af994fa3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS/bundle.json","state_url":"https://pith.science/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS/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":"2026-08-14T08:38:02Z","links":{"resolver":"https://pith.science/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS","bundle":"https://pith.science/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS/bundle.json","state":"https://pith.science/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UP6RQTHOPYJCA5V6MUFZ6ZLTBS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:UP6RQTHOPYJCA5V6MUFZ6ZLTBS","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":"33a6fabbe46e3fa015bed27e8f737a751afc166153533925ace314238cf26399","cross_cats_sorted":["physics.app-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-11-26T12:24:52Z","title_canon_sha256":"795dbf4b1b1593e428ec7644a7d616965e9629e2a11a3a8cd9e216009b228639"},"schema_version":"1.0","source":{"id":"2411.17368","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.17368","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"arxiv_version","alias_value":"2411.17368v2","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.17368","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"pith_short_12","alias_value":"UP6RQTHOPYJC","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"pith_short_16","alias_value":"UP6RQTHOPYJCA5V6","created_at":"2026-07-05T10:44:20Z"},{"alias_kind":"pith_short_8","alias_value":"UP6RQTHO","created_at":"2026-07-05T10:44:20Z"}],"graph_snapshots":[{"event_id":"sha256:f4841cc4af9ef6805cff6072adea3f320874c96f064d141bc8a495d9af994fa3","target":"graph","created_at":"2026-07-05T10:44:20Z","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/2411.17368/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work we derive and study the analytical solution of the voltage and current diffusion equation for the case of a finite-length resistor-constant phase element (CPE) transmission line (TL) network that can represent a model for porous electrodes in the absence of any Faradic processes. The energy storage component is considered to be an elemental CPE per unit length of impedance $z_c(s)={1}/{(c_{\\alpha} s^{\\alpha})}$ with constant parameters $(c_{\\alpha},\\alpha)$ instead of the ideal capacitor of impedance $z(s)={1}/{(c\\, s)}$ usually assumed in TL modeling. The problem becomes a time-f","authors_text":"Anis Allagui, Chunlei Wang, Enrique H. Balaguera","cross_cats":["physics.app-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-11-26T12:24:52Z","title":"On the distributed resistor-constant phase element transmission line in a reflective bounded domain"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.17368","kind":"arxiv","version":2},"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":"sha256:15581dc50e4a73c038954736425bb7a3ee119228839c2143cc2436ba403e0a5e","target":"record","created_at":"2026-07-05T10:44:20Z","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":"33a6fabbe46e3fa015bed27e8f737a751afc166153533925ace314238cf26399","cross_cats_sorted":["physics.app-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-11-26T12:24:52Z","title_canon_sha256":"795dbf4b1b1593e428ec7644a7d616965e9629e2a11a3a8cd9e216009b228639"},"schema_version":"1.0","source":{"id":"2411.17368","kind":"arxiv","version":2}},"canonical_sha256":"a3fd184cee7e122076be650b9f65730caeff21093ebd454b49f046c781220db0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a3fd184cee7e122076be650b9f65730caeff21093ebd454b49f046c781220db0","first_computed_at":"2026-07-05T10:44:20.168667Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:44:20.168667Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"F7EMZaPHWzgW2D8z9chSRRFi1y+GM0zfftZfAiVztNZLu2PAuqzoqtFH2MjPl8BczZaI/i03o5ObxyKlIlDIDA==","signature_status":"signed_v1","signed_at":"2026-07-05T10:44:20.169209Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.17368","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:15581dc50e4a73c038954736425bb7a3ee119228839c2143cc2436ba403e0a5e","sha256:f4841cc4af9ef6805cff6072adea3f320874c96f064d141bc8a495d9af994fa3"],"state_sha256":"91ac1ba3f5472117f6b894a34cfd104550b1fcff8256e45f32bc71c22eb783ca"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HjxgwyJrNIOGp56oxVVx5Xqwjz5/6KXQ8s05gSkGHrmjkGQTtccY23dfaSXx6/yY6ZTT3rh4YKBrDq8iGaU+DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T08:38:02.599859Z","bundle_sha256":"89c424e9cb9a8539af217b139c10c2afa46294f0a7651ff1d194419f42471d2f"}}