{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2019:HQAASP3Z45IEFTUU3RMN3OYJBG","short_pith_number":"pith:HQAASP3Z","canonical_record":{"source":{"id":"1902.10047","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2019-02-26T16:44:31Z","cross_cats_sorted":[],"title_canon_sha256":"7a18f2ee8bb7f264cf6b8f666488ccb25a8ecce718acd857448e85bccfc05012","abstract_canon_sha256":"5e9cda368fb2d4c9ac5f75dee7c4770daf85f7e2f8cd895795d6aa89379bd364"},"schema_version":"1.0"},"canonical_sha256":"3c00093f79e75042ce94dc58ddbb0909a3cf079d7f8b4bad689774d2651b8f7f","source":{"kind":"arxiv","id":"1902.10047","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.10047","created_at":"2026-05-17T23:50:35Z"},{"alias_kind":"arxiv_version","alias_value":"1902.10047v2","created_at":"2026-05-17T23:50:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.10047","created_at":"2026-05-17T23:50:35Z"},{"alias_kind":"pith_short_12","alias_value":"HQAASP3Z45IE","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_16","alias_value":"HQAASP3Z45IEFTUU","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_8","alias_value":"HQAASP3Z","created_at":"2026-05-18T12:33:18Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2019:HQAASP3Z45IEFTUU3RMN3OYJBG","target":"record","payload":{"canonical_record":{"source":{"id":"1902.10047","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2019-02-26T16:44:31Z","cross_cats_sorted":[],"title_canon_sha256":"7a18f2ee8bb7f264cf6b8f666488ccb25a8ecce718acd857448e85bccfc05012","abstract_canon_sha256":"5e9cda368fb2d4c9ac5f75dee7c4770daf85f7e2f8cd895795d6aa89379bd364"},"schema_version":"1.0"},"canonical_sha256":"3c00093f79e75042ce94dc58ddbb0909a3cf079d7f8b4bad689774d2651b8f7f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:35.999903Z","signature_b64":"ITUZvw8Zy27gFn9IMMC9huQqSnBFaNjruhpLYPaliffyf4I7OemLgfLBYRTUuGsfsR8tVSmF0cJ1RUyIbuW7Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c00093f79e75042ce94dc58ddbb0909a3cf079d7f8b4bad689774d2651b8f7f","last_reissued_at":"2026-05-17T23:50:35.999405Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:35.999405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1902.10047","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":"2026-05-17T23:50:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3adIWSlrtn9x5Luem5YhXbTNEMGeOUUcYbPNNMNRlc1H1XCfvzp4ekbi0/xGlK32G1o1/rOGEmgPoLEzlbo3AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:16:49.895013Z"},"content_sha256":"a9336fe54bbff7f9f27f2db089c011d0dd8f0e6981e91aae89bb56d49d1e5923","schema_version":"1.0","event_id":"sha256:a9336fe54bbff7f9f27f2db089c011d0dd8f0e6981e91aae89bb56d49d1e5923"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2019:HQAASP3Z45IEFTUU3RMN3OYJBG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Modelling a Transition-Edge Sensor X-ray Microcalorimeter Linear Array for Compton Profile Measurements and Energy Dispersive Diffraction","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"Antonino Miceli, Daikang Yan, Lisa M. Gades, Orlando Quaranta, Tejas Guruswamy, Umeshkumar M. Patel","submitted_at":"2019-02-26T16:44:31Z","abstract_excerpt":"Transition-edge sensors are a type of superconducting detector that offers high energy resolution based on their sharp resistance-temperature feature in the superconducting-to-normal transition. TES X-ray microcalorimeters have typically been designed and used for spectroscopic applications. In this work, we present a design optimization for a TES X-ray microcalorimeter array for high-energy scattering and diffraction measurements. In particular, Compton scattering provides information about the electron momentum distribution, while energy dispersive diffraction provides structural information"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.10047","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":""},"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":"2026-05-17T23:50:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tMYVe7qyc5crR3CkfGOAFuNbQEyiiupSkOri+lnVtUftGIslKRJaQilM6RaySgRrsSxsWweDVhhyEG5nP3MzCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:16:49.895706Z"},"content_sha256":"29ea717a641260dfc587cd5a771067b03cec19518df181237c1443765d74c309","schema_version":"1.0","event_id":"sha256:29ea717a641260dfc587cd5a771067b03cec19518df181237c1443765d74c309"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HQAASP3Z45IEFTUU3RMN3OYJBG/bundle.json","state_url":"https://pith.science/pith/HQAASP3Z45IEFTUU3RMN3OYJBG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HQAASP3Z45IEFTUU3RMN3OYJBG/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":"2026-05-27T05:16:49Z","links":{"resolver":"https://pith.science/pith/HQAASP3Z45IEFTUU3RMN3OYJBG","bundle":"https://pith.science/pith/HQAASP3Z45IEFTUU3RMN3OYJBG/bundle.json","state":"https://pith.science/pith/HQAASP3Z45IEFTUU3RMN3OYJBG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HQAASP3Z45IEFTUU3RMN3OYJBG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:HQAASP3Z45IEFTUU3RMN3OYJBG","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":"5e9cda368fb2d4c9ac5f75dee7c4770daf85f7e2f8cd895795d6aa89379bd364","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2019-02-26T16:44:31Z","title_canon_sha256":"7a18f2ee8bb7f264cf6b8f666488ccb25a8ecce718acd857448e85bccfc05012"},"schema_version":"1.0","source":{"id":"1902.10047","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1902.10047","created_at":"2026-05-17T23:50:35Z"},{"alias_kind":"arxiv_version","alias_value":"1902.10047v2","created_at":"2026-05-17T23:50:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.10047","created_at":"2026-05-17T23:50:35Z"},{"alias_kind":"pith_short_12","alias_value":"HQAASP3Z45IE","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_16","alias_value":"HQAASP3Z45IEFTUU","created_at":"2026-05-18T12:33:18Z"},{"alias_kind":"pith_short_8","alias_value":"HQAASP3Z","created_at":"2026-05-18T12:33:18Z"}],"graph_snapshots":[{"event_id":"sha256:29ea717a641260dfc587cd5a771067b03cec19518df181237c1443765d74c309","target":"graph","created_at":"2026-05-17T23:50:35Z","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"},"paper":{"abstract_excerpt":"Transition-edge sensors are a type of superconducting detector that offers high energy resolution based on their sharp resistance-temperature feature in the superconducting-to-normal transition. TES X-ray microcalorimeters have typically been designed and used for spectroscopic applications. In this work, we present a design optimization for a TES X-ray microcalorimeter array for high-energy scattering and diffraction measurements. In particular, Compton scattering provides information about the electron momentum distribution, while energy dispersive diffraction provides structural information","authors_text":"Antonino Miceli, Daikang Yan, Lisa M. Gades, Orlando Quaranta, Tejas Guruswamy, Umeshkumar M. Patel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2019-02-26T16:44:31Z","title":"Modelling a Transition-Edge Sensor X-ray Microcalorimeter Linear Array for Compton Profile Measurements and Energy Dispersive Diffraction"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.10047","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:a9336fe54bbff7f9f27f2db089c011d0dd8f0e6981e91aae89bb56d49d1e5923","target":"record","created_at":"2026-05-17T23:50:35Z","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":"5e9cda368fb2d4c9ac5f75dee7c4770daf85f7e2f8cd895795d6aa89379bd364","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2019-02-26T16:44:31Z","title_canon_sha256":"7a18f2ee8bb7f264cf6b8f666488ccb25a8ecce718acd857448e85bccfc05012"},"schema_version":"1.0","source":{"id":"1902.10047","kind":"arxiv","version":2}},"canonical_sha256":"3c00093f79e75042ce94dc58ddbb0909a3cf079d7f8b4bad689774d2651b8f7f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3c00093f79e75042ce94dc58ddbb0909a3cf079d7f8b4bad689774d2651b8f7f","first_computed_at":"2026-05-17T23:50:35.999405Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:50:35.999405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ITUZvw8Zy27gFn9IMMC9huQqSnBFaNjruhpLYPaliffyf4I7OemLgfLBYRTUuGsfsR8tVSmF0cJ1RUyIbuW7Dw==","signature_status":"signed_v1","signed_at":"2026-05-17T23:50:35.999903Z","signed_message":"canonical_sha256_bytes"},"source_id":"1902.10047","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a9336fe54bbff7f9f27f2db089c011d0dd8f0e6981e91aae89bb56d49d1e5923","sha256:29ea717a641260dfc587cd5a771067b03cec19518df181237c1443765d74c309"],"state_sha256":"3731220d3ee240019bd9e0e3659e040109c4c7c80db23e8568c43ca4162fdc4b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u6xQv+ikBmXZS2MekuzsSw8U2X5Tdp6LQJw7OSvPISwWxEAB2TacavacbHoRV6KW2L3gcQzHCHTAtYC3yRSQBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T05:16:49.900111Z","bundle_sha256":"125361f54b00c74774c8b5ebc51c5bda4e69ee5c44008b417ff40d45232c0ce2"}}