{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:TP373W34YHAOYMXH7OR3UR3PNN","short_pith_number":"pith:TP373W34","canonical_record":{"source":{"id":"1201.3992","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-01-19T08:41:29Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"014b4b3dcf629deeb5e3dd51185b1d2eb27ed9d3a3f9db6d5de8fd8a42d3be3f","abstract_canon_sha256":"3af6cb0a009ab63a7a998c04c854a369a729b3bc4c9fd27536b34bf9d063c610"},"schema_version":"1.0"},"canonical_sha256":"9bf7fddb7cc1c0ec32e7fba3ba476f6b4decdd5242d2d66a910c9175d04b5082","source":{"kind":"arxiv","id":"1201.3992","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.3992","created_at":"2026-05-18T04:04:16Z"},{"alias_kind":"arxiv_version","alias_value":"1201.3992v1","created_at":"2026-05-18T04:04:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.3992","created_at":"2026-05-18T04:04:16Z"},{"alias_kind":"pith_short_12","alias_value":"TP373W34YHAO","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"TP373W34YHAOYMXH","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"TP373W34","created_at":"2026-05-18T12:27:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:TP373W34YHAOYMXH7OR3UR3PNN","target":"record","payload":{"canonical_record":{"source":{"id":"1201.3992","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-01-19T08:41:29Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"014b4b3dcf629deeb5e3dd51185b1d2eb27ed9d3a3f9db6d5de8fd8a42d3be3f","abstract_canon_sha256":"3af6cb0a009ab63a7a998c04c854a369a729b3bc4c9fd27536b34bf9d063c610"},"schema_version":"1.0"},"canonical_sha256":"9bf7fddb7cc1c0ec32e7fba3ba476f6b4decdd5242d2d66a910c9175d04b5082","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:04:16.215396Z","signature_b64":"4KDuxjSvwwLDVcfptgj/2YtlCP5VZr01xCysbu1Cyq1or5miFY9W0u6FMHoaMA9N2Kro1ztqufCM6Z5czPeFCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9bf7fddb7cc1c0ec32e7fba3ba476f6b4decdd5242d2d66a910c9175d04b5082","last_reissued_at":"2026-05-18T04:04:16.214526Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:04:16.214526Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.3992","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":"2026-05-18T04:04:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iP+0MWNiNWTLhnUwIlDW3O4tZCbAXmwfjujp3z7hRko9/a6uti4AeePOTG4o8WwsXMcu8JewfuYTEKqGW8AxAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T05:24:13.495593Z"},"content_sha256":"163cde0601a06ea2df3f3403ac0c73dc20d8c7705b77f5cbba1dde997615a321","schema_version":"1.0","event_id":"sha256:163cde0601a06ea2df3f3403ac0c73dc20d8c7705b77f5cbba1dde997615a321"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:TP373W34YHAOYMXH7OR3UR3PNN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High harmonic spectra via dominant interaction Hamiltonians","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Carlos Zagoya, Christoph-Marian Goletz, Frank Grossmann, Jan M. Rost","submitted_at":"2012-01-19T08:41:29Z","abstract_excerpt":"We formulate the concept of dominant interaction Hamiltonians to obtain an integrable approximation to the dynamics of an electron exposed to a strong laser field and an atomic potential leading to high harmonic generation. The concept relies on local information in phase space to switch between the interactions. This information is provided by classical integrable trajectories from which we construct a semiclassical wave function. The high harmonic spectrum obtained is in excellent agreement with the accurate quantum spectrum. The separation in the atomic potential and laser coupling interact"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.3992","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":""},"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":"2026-05-18T04:04:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2tmcftujLTy4I7Rdox5K6kqCOYItQT/z3/kJtCtEOLdna4CqLEp41GnGX7Os6lzZHwEyJgxqkghWiioxaPcyBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T05:24:13.495956Z"},"content_sha256":"b6aab7d4946b82744b453d905d7ffdfb7342a7c2ab43d4890a0b4a0b86566fe8","schema_version":"1.0","event_id":"sha256:b6aab7d4946b82744b453d905d7ffdfb7342a7c2ab43d4890a0b4a0b86566fe8"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TP373W34YHAOYMXH7OR3UR3PNN/bundle.json","state_url":"https://pith.science/pith/TP373W34YHAOYMXH7OR3UR3PNN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TP373W34YHAOYMXH7OR3UR3PNN/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":"2026-06-29T05:24:13Z","links":{"resolver":"https://pith.science/pith/TP373W34YHAOYMXH7OR3UR3PNN","bundle":"https://pith.science/pith/TP373W34YHAOYMXH7OR3UR3PNN/bundle.json","state":"https://pith.science/pith/TP373W34YHAOYMXH7OR3UR3PNN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TP373W34YHAOYMXH7OR3UR3PNN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:TP373W34YHAOYMXH7OR3UR3PNN","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":"3af6cb0a009ab63a7a998c04c854a369a729b3bc4c9fd27536b34bf9d063c610","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-01-19T08:41:29Z","title_canon_sha256":"014b4b3dcf629deeb5e3dd51185b1d2eb27ed9d3a3f9db6d5de8fd8a42d3be3f"},"schema_version":"1.0","source":{"id":"1201.3992","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.3992","created_at":"2026-05-18T04:04:16Z"},{"alias_kind":"arxiv_version","alias_value":"1201.3992v1","created_at":"2026-05-18T04:04:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.3992","created_at":"2026-05-18T04:04:16Z"},{"alias_kind":"pith_short_12","alias_value":"TP373W34YHAO","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"TP373W34YHAOYMXH","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"TP373W34","created_at":"2026-05-18T12:27:23Z"}],"graph_snapshots":[{"event_id":"sha256:b6aab7d4946b82744b453d905d7ffdfb7342a7c2ab43d4890a0b4a0b86566fe8","target":"graph","created_at":"2026-05-18T04:04:16Z","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":"We formulate the concept of dominant interaction Hamiltonians to obtain an integrable approximation to the dynamics of an electron exposed to a strong laser field and an atomic potential leading to high harmonic generation. The concept relies on local information in phase space to switch between the interactions. This information is provided by classical integrable trajectories from which we construct a semiclassical wave function. The high harmonic spectrum obtained is in excellent agreement with the accurate quantum spectrum. The separation in the atomic potential and laser coupling interact","authors_text":"Carlos Zagoya, Christoph-Marian Goletz, Frank Grossmann, Jan M. Rost","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-01-19T08:41:29Z","title":"High harmonic spectra via dominant interaction Hamiltonians"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.3992","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":"sha256:163cde0601a06ea2df3f3403ac0c73dc20d8c7705b77f5cbba1dde997615a321","target":"record","created_at":"2026-05-18T04:04:16Z","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":"3af6cb0a009ab63a7a998c04c854a369a729b3bc4c9fd27536b34bf9d063c610","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2012-01-19T08:41:29Z","title_canon_sha256":"014b4b3dcf629deeb5e3dd51185b1d2eb27ed9d3a3f9db6d5de8fd8a42d3be3f"},"schema_version":"1.0","source":{"id":"1201.3992","kind":"arxiv","version":1}},"canonical_sha256":"9bf7fddb7cc1c0ec32e7fba3ba476f6b4decdd5242d2d66a910c9175d04b5082","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9bf7fddb7cc1c0ec32e7fba3ba476f6b4decdd5242d2d66a910c9175d04b5082","first_computed_at":"2026-05-18T04:04:16.214526Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:04:16.214526Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4KDuxjSvwwLDVcfptgj/2YtlCP5VZr01xCysbu1Cyq1or5miFY9W0u6FMHoaMA9N2Kro1ztqufCM6Z5czPeFCg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:04:16.215396Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.3992","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:163cde0601a06ea2df3f3403ac0c73dc20d8c7705b77f5cbba1dde997615a321","sha256:b6aab7d4946b82744b453d905d7ffdfb7342a7c2ab43d4890a0b4a0b86566fe8"],"state_sha256":"e50ac8b3ce949b3dd89c4ee6d7fbe333c56b7213c7b5e49591568a7be63ed078"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CC5DKy4iyhEC2ScdzmXCCHcOkL1MDP1pVWZ1wRdwyGGHqDpd05ci3cQS1y8hTuE04UPjCf67HDViWbhk5VXiDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T05:24:13.497823Z","bundle_sha256":"dc5ec57fbcc56f4df629e23bd0c3dabfa0cfa7ad4720258e3c9e7b61090ada4a"}}