{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:DF5AIUTUUCIBZPOYOYIJKUKTGC","short_pith_number":"pith:DF5AIUTU","canonical_record":{"source":{"id":"2411.19656","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2024-11-29T12:23:29Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"7e3ef2b652165feaf2d1ae2675bbdc43198ecd4645e97aa210133c8fcefcb7cc","abstract_canon_sha256":"ed7a29f4e1992286ed48a4f8a395cb25971ad93b6131403e5a037b26f22e1986"},"schema_version":"1.0"},"canonical_sha256":"197a045274a0901cbdd8761095515330b708e71dc59e0379e39d830e4d1f5d7a","source":{"kind":"arxiv","id":"2411.19656","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.19656","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"arxiv_version","alias_value":"2411.19656v1","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.19656","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"pith_short_12","alias_value":"DF5AIUTUUCIB","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"pith_short_16","alias_value":"DF5AIUTUUCIBZPOY","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"pith_short_8","alias_value":"DF5AIUTU","created_at":"2026-07-05T09:42:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:DF5AIUTUUCIBZPOYOYIJKUKTGC","target":"record","payload":{"canonical_record":{"source":{"id":"2411.19656","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2024-11-29T12:23:29Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"7e3ef2b652165feaf2d1ae2675bbdc43198ecd4645e97aa210133c8fcefcb7cc","abstract_canon_sha256":"ed7a29f4e1992286ed48a4f8a395cb25971ad93b6131403e5a037b26f22e1986"},"schema_version":"1.0"},"canonical_sha256":"197a045274a0901cbdd8761095515330b708e71dc59e0379e39d830e4d1f5d7a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:42:05.927357Z","signature_b64":"3qolWg08LjotN4/1KIZG4QQq01AOnZ3LMvSr9OAhd/imGNqaG7lUC78dFpGoFUnjls5FqwOTgHLW3V6nulo2BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"197a045274a0901cbdd8761095515330b708e71dc59e0379e39d830e4d1f5d7a","last_reissued_at":"2026-07-05T09:42:05.926885Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:42:05.926885Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2411.19656","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":"2026-07-05T09:42:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vYCq3nbcLh+u3KpkhxpNtGlrH7gwa/GL0AHwLvT5ckToY7QCKeKHM7QucrGMTDJK1dKZjD2iexOHsB5az45UBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T11:54:51.210795Z"},"content_sha256":"6fa717e003e99f2364cb556a034b547f982e834b99695d05e79ee82bed8a23f4","schema_version":"1.0","event_id":"sha256:6fa717e003e99f2364cb556a034b547f982e834b99695d05e79ee82bed8a23f4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:DF5AIUTUUCIBZPOYOYIJKUKTGC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Design of structured La$_{2-x}$Sr$_{x}$CuO$_{4}$ films as superconducting transition-edge sensors at 4.2K","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"cond-mat.supr-con","authors_text":"A.S. Viz, M.M. Botana, M.V. Ramallo","submitted_at":"2024-11-29T12:23:29Z","abstract_excerpt":"We calculate the effects of carrier-density structuration and patterning on thin films of the cuprate superconductor La$_{2-x}$Sr$_{x}$CuO$_{4}$, in order to optimize its functional characteristics as sensing material for resistive transition-edge bolometers at liquid-He temperature. We perform finite-element computations considering two major contributions to structuration: The intrinsic random nanoscale disorder associated to carrier density nonstoichiometry, plus the imposition of regular arrangements of zones with different nominal carrier densities. Using ad-hoc seek algorithms, we obtain"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.19656","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/2411.19656/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":"2026-07-05T09:42:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YczTs1rMNWgW97cOVqvxsG27GoNvDENCkmF+eXCHR6CuTftHDz4McmVqJlnyZvtQ5aQM6aE0KlQd3eveSadMAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T11:54:51.211346Z"},"content_sha256":"4b217f541b681b56c063259e64737c1db53685d65badf03efff99d254832ca50","schema_version":"1.0","event_id":"sha256:4b217f541b681b56c063259e64737c1db53685d65badf03efff99d254832ca50"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC/bundle.json","state_url":"https://pith.science/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC/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":"2026-08-14T11:54:51Z","links":{"resolver":"https://pith.science/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC","bundle":"https://pith.science/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC/bundle.json","state":"https://pith.science/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DF5AIUTUUCIBZPOYOYIJKUKTGC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:DF5AIUTUUCIBZPOYOYIJKUKTGC","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":"ed7a29f4e1992286ed48a4f8a395cb25971ad93b6131403e5a037b26f22e1986","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2024-11-29T12:23:29Z","title_canon_sha256":"7e3ef2b652165feaf2d1ae2675bbdc43198ecd4645e97aa210133c8fcefcb7cc"},"schema_version":"1.0","source":{"id":"2411.19656","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.19656","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"arxiv_version","alias_value":"2411.19656v1","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.19656","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"pith_short_12","alias_value":"DF5AIUTUUCIB","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"pith_short_16","alias_value":"DF5AIUTUUCIBZPOY","created_at":"2026-07-05T09:42:05Z"},{"alias_kind":"pith_short_8","alias_value":"DF5AIUTU","created_at":"2026-07-05T09:42:05Z"}],"graph_snapshots":[{"event_id":"sha256:4b217f541b681b56c063259e64737c1db53685d65badf03efff99d254832ca50","target":"graph","created_at":"2026-07-05T09:42:05Z","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/2411.19656/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We calculate the effects of carrier-density structuration and patterning on thin films of the cuprate superconductor La$_{2-x}$Sr$_{x}$CuO$_{4}$, in order to optimize its functional characteristics as sensing material for resistive transition-edge bolometers at liquid-He temperature. We perform finite-element computations considering two major contributions to structuration: The intrinsic random nanoscale disorder associated to carrier density nonstoichiometry, plus the imposition of regular arrangements of zones with different nominal carrier densities. Using ad-hoc seek algorithms, we obtain","authors_text":"A.S. Viz, M.M. Botana, M.V. Ramallo","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2024-11-29T12:23:29Z","title":"Design of structured La$_{2-x}$Sr$_{x}$CuO$_{4}$ films as superconducting transition-edge sensors at 4.2K"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.19656","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":"sha256:6fa717e003e99f2364cb556a034b547f982e834b99695d05e79ee82bed8a23f4","target":"record","created_at":"2026-07-05T09:42:05Z","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":"ed7a29f4e1992286ed48a4f8a395cb25971ad93b6131403e5a037b26f22e1986","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2024-11-29T12:23:29Z","title_canon_sha256":"7e3ef2b652165feaf2d1ae2675bbdc43198ecd4645e97aa210133c8fcefcb7cc"},"schema_version":"1.0","source":{"id":"2411.19656","kind":"arxiv","version":1}},"canonical_sha256":"197a045274a0901cbdd8761095515330b708e71dc59e0379e39d830e4d1f5d7a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"197a045274a0901cbdd8761095515330b708e71dc59e0379e39d830e4d1f5d7a","first_computed_at":"2026-07-05T09:42:05.926885Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:42:05.926885Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"3qolWg08LjotN4/1KIZG4QQq01AOnZ3LMvSr9OAhd/imGNqaG7lUC78dFpGoFUnjls5FqwOTgHLW3V6nulo2BQ==","signature_status":"signed_v1","signed_at":"2026-07-05T09:42:05.927357Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.19656","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6fa717e003e99f2364cb556a034b547f982e834b99695d05e79ee82bed8a23f4","sha256:4b217f541b681b56c063259e64737c1db53685d65badf03efff99d254832ca50"],"state_sha256":"20f4b5314be34959fe9008b304c5ef7fd4c942add64b4a3de7ee2440fdcc535d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u4xdu6ClGRPyxsuWuj/pYefWWVMdHbmWfMOBDl6Mb88f/xjZNtOrffA+WjVVjfG4tBjfUJZO1jOt3Xp6PNxrAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T11:54:51.217532Z","bundle_sha256":"0803ba9aadcff1b44e57d3f2882e462f09b17553a1eaf3dfa169b3906ba39249"}}