{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:445XG7LRFASFADFDFTO4HHO62T","short_pith_number":"pith:445XG7LR","canonical_record":{"source":{"id":"2511.04253","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-11-06T10:39:23Z","cross_cats_sorted":[],"title_canon_sha256":"82f539347898d46005974e6f6990e8cd0dfc8245845aa9716a5143412b08679f","abstract_canon_sha256":"bb0d306f13509cfe5fcf61319dfc5febb515395f9b80b70f0144e82621f58b72"},"schema_version":"1.0"},"canonical_sha256":"e73b737d712824500ca32cddc39dded4ee5861088daf5ca80a9499f3942823dd","source":{"kind":"arxiv","id":"2511.04253","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2511.04253","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"arxiv_version","alias_value":"2511.04253v1","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.04253","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"pith_short_12","alias_value":"445XG7LRFASF","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"pith_short_16","alias_value":"445XG7LRFASFADFD","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"pith_short_8","alias_value":"445XG7LR","created_at":"2026-06-03T02:05:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:445XG7LRFASFADFDFTO4HHO62T","target":"record","payload":{"canonical_record":{"source":{"id":"2511.04253","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-11-06T10:39:23Z","cross_cats_sorted":[],"title_canon_sha256":"82f539347898d46005974e6f6990e8cd0dfc8245845aa9716a5143412b08679f","abstract_canon_sha256":"bb0d306f13509cfe5fcf61319dfc5febb515395f9b80b70f0144e82621f58b72"},"schema_version":"1.0"},"canonical_sha256":"e73b737d712824500ca32cddc39dded4ee5861088daf5ca80a9499f3942823dd","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-03T02:05:43.198503Z","signature_b64":"Jo9Kj5xWcZml5Tntjn7MdhylrYJPVQl6goD0S7by45kTEfMQKz99Bv/bxO+lKdl3Pb39sdiDb2yd7Z7beyqoAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e73b737d712824500ca32cddc39dded4ee5861088daf5ca80a9499f3942823dd","last_reissued_at":"2026-06-03T02:05:43.198015Z","signature_status":"signed_v1","first_computed_at":"2026-06-03T02:05:43.198015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2511.04253","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":"2026-06-03T02:05:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"E8bA+qalvWLmaMtcBTFDmQWwYzZLETxQ1V8rdL+DtBLEV7RWsHunzcDI7fCSRIYyYfJQAwLfpaZ+OJIUpdDmDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T12:53:44.467076Z"},"content_sha256":"39969a4708e5ad3729e734e10ae271f89ddf028198a5916a62622222608fd3cd","schema_version":"1.0","event_id":"sha256:39969a4708e5ad3729e734e10ae271f89ddf028198a5916a62622222608fd3cd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:445XG7LRFASFADFDFTO4HHO62T","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Photoelectron combs in ionization: Influence of rescattering and nondipole effects","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"J. Z. Kami\\'nski, K. Krajewska","submitted_at":"2025-11-06T10:39:23Z","abstract_excerpt":"Ionization by a sequence of extreme ultraviolet pulses is investigated based on the rigorous numerical solution of the time-dependent Schr\\\"odinger equation, when the driving laser field is treated exactly. This goes beyond the typically used first-order nondipole approximation and reveals the effects of radiation pressure to its full extent. Specifically, we observe the comb structures in both the momentum and the energy distributions of photoelectrons. The comb peaks are shifted, however, depending on the emission angle of electrons. While similar effect is observed already in the first-orde"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.04253","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/2511.04253/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":"2026-06-03T02:05:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+HggUQbXitNAPcyEnVLgDNFW183INrb7vqaOokzh6tkYdWsUWE0p5ye4fJ8Y5qLXZ+BBTSm3cIg7wxyagdNRBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T12:53:44.467939Z"},"content_sha256":"85edbce14377c7998b63c2295e7f0f0c5e3f1b9c1552c2b062ae78162fe87ee2","schema_version":"1.0","event_id":"sha256:85edbce14377c7998b63c2295e7f0f0c5e3f1b9c1552c2b062ae78162fe87ee2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/445XG7LRFASFADFDFTO4HHO62T/bundle.json","state_url":"https://pith.science/pith/445XG7LRFASFADFDFTO4HHO62T/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/445XG7LRFASFADFDFTO4HHO62T/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":"2026-06-07T12:53:44Z","links":{"resolver":"https://pith.science/pith/445XG7LRFASFADFDFTO4HHO62T","bundle":"https://pith.science/pith/445XG7LRFASFADFDFTO4HHO62T/bundle.json","state":"https://pith.science/pith/445XG7LRFASFADFDFTO4HHO62T/state.json","well_known_bundle":"https://pith.science/.well-known/pith/445XG7LRFASFADFDFTO4HHO62T/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:445XG7LRFASFADFDFTO4HHO62T","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":"bb0d306f13509cfe5fcf61319dfc5febb515395f9b80b70f0144e82621f58b72","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-11-06T10:39:23Z","title_canon_sha256":"82f539347898d46005974e6f6990e8cd0dfc8245845aa9716a5143412b08679f"},"schema_version":"1.0","source":{"id":"2511.04253","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2511.04253","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"arxiv_version","alias_value":"2511.04253v1","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2511.04253","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"pith_short_12","alias_value":"445XG7LRFASF","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"pith_short_16","alias_value":"445XG7LRFASFADFD","created_at":"2026-06-03T02:05:43Z"},{"alias_kind":"pith_short_8","alias_value":"445XG7LR","created_at":"2026-06-03T02:05:43Z"}],"graph_snapshots":[{"event_id":"sha256:85edbce14377c7998b63c2295e7f0f0c5e3f1b9c1552c2b062ae78162fe87ee2","target":"graph","created_at":"2026-06-03T02:05:43Z","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/2511.04253/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Ionization by a sequence of extreme ultraviolet pulses is investigated based on the rigorous numerical solution of the time-dependent Schr\\\"odinger equation, when the driving laser field is treated exactly. This goes beyond the typically used first-order nondipole approximation and reveals the effects of radiation pressure to its full extent. Specifically, we observe the comb structures in both the momentum and the energy distributions of photoelectrons. The comb peaks are shifted, however, depending on the emission angle of electrons. While similar effect is observed already in the first-orde","authors_text":"J. Z. Kami\\'nski, K. Krajewska","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-11-06T10:39:23Z","title":"Photoelectron combs in ionization: Influence of rescattering and nondipole effects"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2511.04253","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":"sha256:39969a4708e5ad3729e734e10ae271f89ddf028198a5916a62622222608fd3cd","target":"record","created_at":"2026-06-03T02:05:43Z","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":"bb0d306f13509cfe5fcf61319dfc5febb515395f9b80b70f0144e82621f58b72","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.atom-ph","submitted_at":"2025-11-06T10:39:23Z","title_canon_sha256":"82f539347898d46005974e6f6990e8cd0dfc8245845aa9716a5143412b08679f"},"schema_version":"1.0","source":{"id":"2511.04253","kind":"arxiv","version":1}},"canonical_sha256":"e73b737d712824500ca32cddc39dded4ee5861088daf5ca80a9499f3942823dd","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e73b737d712824500ca32cddc39dded4ee5861088daf5ca80a9499f3942823dd","first_computed_at":"2026-06-03T02:05:43.198015Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-03T02:05:43.198015Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Jo9Kj5xWcZml5Tntjn7MdhylrYJPVQl6goD0S7by45kTEfMQKz99Bv/bxO+lKdl3Pb39sdiDb2yd7Z7beyqoAQ==","signature_status":"signed_v1","signed_at":"2026-06-03T02:05:43.198503Z","signed_message":"canonical_sha256_bytes"},"source_id":"2511.04253","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:39969a4708e5ad3729e734e10ae271f89ddf028198a5916a62622222608fd3cd","sha256:85edbce14377c7998b63c2295e7f0f0c5e3f1b9c1552c2b062ae78162fe87ee2"],"state_sha256":"22758abc233bdbd94cc279219a712d77ee602d8db382a0cec596290b4727dacb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EO0UCMaKxMj/bquWeWfqxUjtxqdCQCRfs55ohxbzdAkYnU6hjW5Oe5oNfAxA1+IHaEDiM78sK9QalyzisbKFBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T12:53:44.472551Z","bundle_sha256":"6c9fd21ff117f89b96950ed61dd6b694390221bf759cf32b5f750051d696e4ca"}}