{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:TQSLSMPQKDTSKJMFV67LBVGHIF","short_pith_number":"pith:TQSLSMPQ","canonical_record":{"source":{"id":"2501.02940","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-01-06T11:26:29Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"8bd42c4a77878b0caa6f7a7d4b1f80d16cf775e57766742b9bb9ad09663fab7e","abstract_canon_sha256":"50b335e8be8bff81c25c91a2dfef0d2f365f22c6216ed192150d38cc0d98aeaa"},"schema_version":"1.0"},"canonical_sha256":"9c24b931f050e7252585afbeb0d4c741765972cd1b34c09d0c376e158b813cab","source":{"kind":"arxiv","id":"2501.02940","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.02940","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"arxiv_version","alias_value":"2501.02940v1","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.02940","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"pith_short_12","alias_value":"TQSLSMPQKDTS","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"pith_short_16","alias_value":"TQSLSMPQKDTSKJMF","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"pith_short_8","alias_value":"TQSLSMPQ","created_at":"2026-07-05T09:57:27Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:TQSLSMPQKDTSKJMFV67LBVGHIF","target":"record","payload":{"canonical_record":{"source":{"id":"2501.02940","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-01-06T11:26:29Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"8bd42c4a77878b0caa6f7a7d4b1f80d16cf775e57766742b9bb9ad09663fab7e","abstract_canon_sha256":"50b335e8be8bff81c25c91a2dfef0d2f365f22c6216ed192150d38cc0d98aeaa"},"schema_version":"1.0"},"canonical_sha256":"9c24b931f050e7252585afbeb0d4c741765972cd1b34c09d0c376e158b813cab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:57:27.832043Z","signature_b64":"daz7kWehcM0B55SIn4b2VIcUYnGF0Cfc0N9oiPgoQgFNmvpPnwyKKwm5M4BZH4L7vr2gRMpcw4yZJj7sqbCUCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9c24b931f050e7252585afbeb0d4c741765972cd1b34c09d0c376e158b813cab","last_reissued_at":"2026-07-05T09:57:27.831569Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:57:27.831569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2501.02940","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":"2026-07-05T09:57:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rFNH9dJnJcw7fHpWb8Cf60ChFE9zl8pjg1nghRNPSEQiQ2V/t3cozLme3nkTWwG7xt0Kuv9+wdS9YV9JAfXCAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T08:12:57.918926Z"},"content_sha256":"cda985780bfbae9e5c8ef509b7739e381d84e3d107713c8d73610d3f28cdb7a7","schema_version":"1.0","event_id":"sha256:cda985780bfbae9e5c8ef509b7739e381d84e3d107713c8d73610d3f28cdb7a7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:TQSLSMPQKDTSKJMFV67LBVGHIF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Femtosecond temperature measurements of laser-shocked copper deduced from the intensity of the x-ray thermal diffuse scattering","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A. B. Belonoshko, A. Descamps, A. Di Cicco, A. Dwivedi, A. E. Lazicki, A. Gleason, A. Higginbotham, A. J. Comley, A. Krygier, A. Laso Garcia, A. L. Coleman, A-M. Norton, A. Pelka, A. Ravasio, A. Sollier, A. Trapananti, B. Albertazzi, B. Massani, B. Nagler, C. A. Bolme, C. Baehtz, C. Edwards, C. E. Vennari, C. Hernandez-Gomez, C. McGuire, C. Otzen, C. Prescher, C. Spindloe, C. Strohm, D. A. Keen, D. Errandonea, D. J. Peake, D. J. Savage, D. Kraus, D. McGonegle, D. Ranjan, D. Santamaria-Perez, E. Brambrink, E. E. McBride, E. Galtier, F. Coppari, F. Dorchies, G. Collins, G. Cristoforetti, G. Fiquet, G. Morard, H. Cynn, H. Ginestet, H. H\\\"oppner, H. Hwang, H-P. Liermann, I. I. Oleynik, J. Chantel, J. Collier, J. D. McHardy, J. H. Eggert, J. Kim, J. M. Gonzalez, J. P. Phillips, J-P. Schwinkendorf, J. Rips, J. Smith, J. Spear, J. S. Wark, J. T. Willman, J. Vorberger, K. A. Pereira, K. Appel, K. Buakor, K. Nguyen-Cong, L. Antonelli, L. Gizzi, L. Labate, L. Randolph, L. Wollenweber, M. G. Gorman, M. Harmand, M. I. McMahon, M. J. Duff, M. Masruri, M. Nakatsutsumi, M. R. Armstrong, M. Schoelmerich, M. Stevenson, M. Tang, M. Toncian, M. Tyldesley, N. Hartley, N. Ozaki, O. B. Ball, O. S. Humphries, P. G. Heighway, P. Koester, P. Mason, P. Sterne, R. Briggs, R. F. Smith, R. J. Husband, R. Redmer, R. S. McWilliams, S. Banerjee, S. C. Vogel, S. Di Dio Cafiso, S. Goede, S. J. Ali, S. J. Tracy, S. Merkel, S. Pandolfi, S. Singh, T-A. Suer, T. Butcher, T. E. Cowan, T. J. Volz, T. M. Hutchinson, T. Preston, T. Stevens, T. Toncian, T. Tschentscher, T. Vinci, U. Zastrau, V. Bouffetier, V. Cerantola, Y. Lee, Y. Ping, Z. Konopkova","submitted_at":"2025-01-06T11:26:29Z","abstract_excerpt":"We present 50-fs, single-shot measurements of the x-ray thermal diffuse scattering (TDS) from copper foils that have been shocked via nanosecond laser-ablation up to pressures above 135~GPa. We hence deduce the x-ray Debye-Waller (DW) factor, providing a temperature measurement. The targets were laser-shocked with the DiPOLE 100-X laser at the High Energy Density (HED) endstation of the European X-ray Free-Electron Laser (EuXFEL). Single x-ray pulses, with a photon energy of 18 keV, were scattered from the samples and recorded on Varex detectors. Despite the targets being highly textured (as e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.02940","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/2501.02940/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":"2026-07-05T09:57:27Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qbLn9M/sx32UWmdRVct8opnsD9yZSJX5CXYyEozQ/ZXVF4KqmiIjSSyu9mU82N+h9ZZiVdIn82oSm3YwOIdOCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-11T08:12:57.919468Z"},"content_sha256":"b53c5fc99d79301be140b0f3bdb109c5cc62e1393b978f7a32d53418e144c946","schema_version":"1.0","event_id":"sha256:b53c5fc99d79301be140b0f3bdb109c5cc62e1393b978f7a32d53418e144c946"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TQSLSMPQKDTSKJMFV67LBVGHIF/bundle.json","state_url":"https://pith.science/pith/TQSLSMPQKDTSKJMFV67LBVGHIF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TQSLSMPQKDTSKJMFV67LBVGHIF/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":"2026-08-11T08:12:57Z","links":{"resolver":"https://pith.science/pith/TQSLSMPQKDTSKJMFV67LBVGHIF","bundle":"https://pith.science/pith/TQSLSMPQKDTSKJMFV67LBVGHIF/bundle.json","state":"https://pith.science/pith/TQSLSMPQKDTSKJMFV67LBVGHIF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TQSLSMPQKDTSKJMFV67LBVGHIF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:TQSLSMPQKDTSKJMFV67LBVGHIF","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":"50b335e8be8bff81c25c91a2dfef0d2f365f22c6216ed192150d38cc0d98aeaa","cross_cats_sorted":["physics.app-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-01-06T11:26:29Z","title_canon_sha256":"8bd42c4a77878b0caa6f7a7d4b1f80d16cf775e57766742b9bb9ad09663fab7e"},"schema_version":"1.0","source":{"id":"2501.02940","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2501.02940","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"arxiv_version","alias_value":"2501.02940v1","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.02940","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"pith_short_12","alias_value":"TQSLSMPQKDTS","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"pith_short_16","alias_value":"TQSLSMPQKDTSKJMF","created_at":"2026-07-05T09:57:27Z"},{"alias_kind":"pith_short_8","alias_value":"TQSLSMPQ","created_at":"2026-07-05T09:57:27Z"}],"graph_snapshots":[{"event_id":"sha256:b53c5fc99d79301be140b0f3bdb109c5cc62e1393b978f7a32d53418e144c946","target":"graph","created_at":"2026-07-05T09:57:27Z","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/2501.02940/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present 50-fs, single-shot measurements of the x-ray thermal diffuse scattering (TDS) from copper foils that have been shocked via nanosecond laser-ablation up to pressures above 135~GPa. We hence deduce the x-ray Debye-Waller (DW) factor, providing a temperature measurement. The targets were laser-shocked with the DiPOLE 100-X laser at the High Energy Density (HED) endstation of the European X-ray Free-Electron Laser (EuXFEL). Single x-ray pulses, with a photon energy of 18 keV, were scattered from the samples and recorded on Varex detectors. Despite the targets being highly textured (as e","authors_text":"A. B. Belonoshko, A. Descamps, A. Di Cicco, A. Dwivedi, A. E. Lazicki, A. Gleason, A. Higginbotham, A. J. Comley, A. Krygier, A. Laso Garcia, A. L. Coleman, A-M. Norton, A. Pelka, A. Ravasio, A. Sollier, A. Trapananti, B. Albertazzi, B. Massani, B. Nagler, C. A. Bolme, C. Baehtz, C. Edwards, C. E. Vennari, C. Hernandez-Gomez, C. McGuire, C. Otzen, C. Prescher, C. Spindloe, C. Strohm, D. A. Keen, D. Errandonea, D. J. Peake, D. J. Savage, D. Kraus, D. McGonegle, D. Ranjan, D. Santamaria-Perez, E. Brambrink, E. E. McBride, E. Galtier, F. Coppari, F. Dorchies, G. Collins, G. Cristoforetti, G. Fiquet, G. Morard, H. Cynn, H. Ginestet, H. H\\\"oppner, H. Hwang, H-P. Liermann, I. I. Oleynik, J. Chantel, J. Collier, J. D. McHardy, J. H. Eggert, J. Kim, J. M. Gonzalez, J. P. Phillips, J-P. Schwinkendorf, J. Rips, J. Smith, J. Spear, J. S. Wark, J. T. Willman, J. Vorberger, K. A. Pereira, K. Appel, K. Buakor, K. Nguyen-Cong, L. Antonelli, L. Gizzi, L. Labate, L. Randolph, L. Wollenweber, M. G. Gorman, M. Harmand, M. I. McMahon, M. J. Duff, M. Masruri, M. Nakatsutsumi, M. R. Armstrong, M. Schoelmerich, M. Stevenson, M. Tang, M. Toncian, M. Tyldesley, N. Hartley, N. Ozaki, O. B. Ball, O. S. Humphries, P. G. Heighway, P. Koester, P. Mason, P. Sterne, R. Briggs, R. F. Smith, R. J. Husband, R. Redmer, R. S. McWilliams, S. Banerjee, S. C. Vogel, S. Di Dio Cafiso, S. Goede, S. J. Ali, S. J. Tracy, S. Merkel, S. Pandolfi, S. Singh, T-A. Suer, T. Butcher, T. E. Cowan, T. J. Volz, T. M. Hutchinson, T. Preston, T. Stevens, T. Toncian, T. Tschentscher, T. Vinci, U. Zastrau, V. Bouffetier, V. Cerantola, Y. Lee, Y. Ping, Z. Konopkova","cross_cats":["physics.app-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-01-06T11:26:29Z","title":"Femtosecond temperature measurements of laser-shocked copper deduced from the intensity of the x-ray thermal diffuse scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.02940","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:cda985780bfbae9e5c8ef509b7739e381d84e3d107713c8d73610d3f28cdb7a7","target":"record","created_at":"2026-07-05T09:57:27Z","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":"50b335e8be8bff81c25c91a2dfef0d2f365f22c6216ed192150d38cc0d98aeaa","cross_cats_sorted":["physics.app-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-01-06T11:26:29Z","title_canon_sha256":"8bd42c4a77878b0caa6f7a7d4b1f80d16cf775e57766742b9bb9ad09663fab7e"},"schema_version":"1.0","source":{"id":"2501.02940","kind":"arxiv","version":1}},"canonical_sha256":"9c24b931f050e7252585afbeb0d4c741765972cd1b34c09d0c376e158b813cab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9c24b931f050e7252585afbeb0d4c741765972cd1b34c09d0c376e158b813cab","first_computed_at":"2026-07-05T09:57:27.831569Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:57:27.831569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"daz7kWehcM0B55SIn4b2VIcUYnGF0Cfc0N9oiPgoQgFNmvpPnwyKKwm5M4BZH4L7vr2gRMpcw4yZJj7sqbCUCw==","signature_status":"signed_v1","signed_at":"2026-07-05T09:57:27.832043Z","signed_message":"canonical_sha256_bytes"},"source_id":"2501.02940","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cda985780bfbae9e5c8ef509b7739e381d84e3d107713c8d73610d3f28cdb7a7","sha256:b53c5fc99d79301be140b0f3bdb109c5cc62e1393b978f7a32d53418e144c946"],"state_sha256":"cfa4a7a3b9178abec931a19a13a776c7830da2c21e271019dd8a9f839acb0ca2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l+YK+v5JGPPhKU7GeFmNZaNTotCrx29i60yCcZqTWiFbgd6KgiNOmtMVzrbFdMshRiVycq2lurhei2+xVEWkCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-11T08:12:57.923988Z","bundle_sha256":"1bdb6ba61dfed3b9b16b40d770cedfffbceed7c95c933e8d82ed0ee1b99ca598"}}