{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:GETKPW7WYTCE3OCD6DO5F6EAII","short_pith_number":"pith:GETKPW7W","canonical_record":{"source":{"id":"1010.0138","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-09-25T16:19:43Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"5fdf59c933d93f5c880246d0bc14b2c45e2ce6058fed2e0bf8d3e5421e057230","abstract_canon_sha256":"d531eb14eaacabb0bcfb04d1cae57422f6655bd9ea291468b98eb76dff8d45ec"},"schema_version":"1.0"},"canonical_sha256":"3126a7dbf6c4c44db843f0ddd2f880420452be952625e5342340e9dfdd76aeef","source":{"kind":"arxiv","id":"1010.0138","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.0138","created_at":"2026-05-18T04:38:58Z"},{"alias_kind":"arxiv_version","alias_value":"1010.0138v1","created_at":"2026-05-18T04:38:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.0138","created_at":"2026-05-18T04:38:58Z"},{"alias_kind":"pith_short_12","alias_value":"GETKPW7WYTCE","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"GETKPW7WYTCE3OCD","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"GETKPW7W","created_at":"2026-05-18T12:26:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:GETKPW7WYTCE3OCD6DO5F6EAII","target":"record","payload":{"canonical_record":{"source":{"id":"1010.0138","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-09-25T16:19:43Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"5fdf59c933d93f5c880246d0bc14b2c45e2ce6058fed2e0bf8d3e5421e057230","abstract_canon_sha256":"d531eb14eaacabb0bcfb04d1cae57422f6655bd9ea291468b98eb76dff8d45ec"},"schema_version":"1.0"},"canonical_sha256":"3126a7dbf6c4c44db843f0ddd2f880420452be952625e5342340e9dfdd76aeef","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:38:58.978860Z","signature_b64":"5OB2tkTg0UeG1lFNgbcQx8ej3r0zWLhNDzzY1jG6whsXSblB+/3e3Xm5gxW1EzWoIOYU4fNXgS2ALDkoD9LdDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3126a7dbf6c4c44db843f0ddd2f880420452be952625e5342340e9dfdd76aeef","last_reissued_at":"2026-05-18T04:38:58.978238Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:38:58.978238Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.0138","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":"2026-05-18T04:38:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"88JvFkmJpFOjU+yd0TUZq0buKe4iyHcfSrzP9qhVty6SN6+dydx/WVkub9e/J1O2eY/7EwS2RvtAStyOypumCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T12:10:50.049646Z"},"content_sha256":"39fd9b97934458d0c3936530331b0090ab671361c40027d1f9e59281352a07fd","schema_version":"1.0","event_id":"sha256:39fd9b97934458d0c3936530331b0090ab671361c40027d1f9e59281352a07fd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:GETKPW7WYTCE3OCD6DO5F6EAII","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coherent control of atomic excitation using off-resonant strong few-cycle pulses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Hichem Eleuch, Pankaj K. Jha, Yuri V. Rostovtsev","submitted_at":"2010-09-25T16:19:43Z","abstract_excerpt":"We study the dynamics of a two-level system driven by an off-resonant few-cycle pulse which has a phase jump $\\phi$ at $t=t_{0}$, in contrast to many cycle pulses, under non rotating-wave approximation (NRWA). We give a closed form analytical solution for the evolution of the probability amplitude $|C_{a} (t)|$ for the upper level. Using the appropriate pulse parameters like phase-jump $\\phi$, jump time $t_{0}$, pulse width $\\tau$, frequency $\\nu$ and Rabi frequency $\\Omega_{0}$ the population transfer, after the pulse is gone, can be optimized and for the pulse considered here, enhancement of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.0138","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":"2026-05-18T04:38:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gZoerUyHAcYigWcImCOyCsIYcq0YjwvoTgeAlnrxntNE7B5NsQlVT1ouFSCXwBC9mMJw6yYKeLA77mdbYRa2DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T12:10:50.049989Z"},"content_sha256":"6479914be7c2c8bb7353c5ffa5fe04d7aae1a72092ad64e8654a348c2da9c906","schema_version":"1.0","event_id":"sha256:6479914be7c2c8bb7353c5ffa5fe04d7aae1a72092ad64e8654a348c2da9c906"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GETKPW7WYTCE3OCD6DO5F6EAII/bundle.json","state_url":"https://pith.science/pith/GETKPW7WYTCE3OCD6DO5F6EAII/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GETKPW7WYTCE3OCD6DO5F6EAII/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":"2026-06-24T12:10:50Z","links":{"resolver":"https://pith.science/pith/GETKPW7WYTCE3OCD6DO5F6EAII","bundle":"https://pith.science/pith/GETKPW7WYTCE3OCD6DO5F6EAII/bundle.json","state":"https://pith.science/pith/GETKPW7WYTCE3OCD6DO5F6EAII/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GETKPW7WYTCE3OCD6DO5F6EAII/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:GETKPW7WYTCE3OCD6DO5F6EAII","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":"d531eb14eaacabb0bcfb04d1cae57422f6655bd9ea291468b98eb76dff8d45ec","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-09-25T16:19:43Z","title_canon_sha256":"5fdf59c933d93f5c880246d0bc14b2c45e2ce6058fed2e0bf8d3e5421e057230"},"schema_version":"1.0","source":{"id":"1010.0138","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.0138","created_at":"2026-05-18T04:38:58Z"},{"alias_kind":"arxiv_version","alias_value":"1010.0138v1","created_at":"2026-05-18T04:38:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.0138","created_at":"2026-05-18T04:38:58Z"},{"alias_kind":"pith_short_12","alias_value":"GETKPW7WYTCE","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"GETKPW7WYTCE3OCD","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"GETKPW7W","created_at":"2026-05-18T12:26:07Z"}],"graph_snapshots":[{"event_id":"sha256:6479914be7c2c8bb7353c5ffa5fe04d7aae1a72092ad64e8654a348c2da9c906","target":"graph","created_at":"2026-05-18T04:38:58Z","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 study the dynamics of a two-level system driven by an off-resonant few-cycle pulse which has a phase jump $\\phi$ at $t=t_{0}$, in contrast to many cycle pulses, under non rotating-wave approximation (NRWA). We give a closed form analytical solution for the evolution of the probability amplitude $|C_{a} (t)|$ for the upper level. Using the appropriate pulse parameters like phase-jump $\\phi$, jump time $t_{0}$, pulse width $\\tau$, frequency $\\nu$ and Rabi frequency $\\Omega_{0}$ the population transfer, after the pulse is gone, can be optimized and for the pulse considered here, enhancement of","authors_text":"Hichem Eleuch, Pankaj K. Jha, Yuri V. Rostovtsev","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-09-25T16:19:43Z","title":"Coherent control of atomic excitation using off-resonant strong few-cycle pulses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.0138","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":"sha256:39fd9b97934458d0c3936530331b0090ab671361c40027d1f9e59281352a07fd","target":"record","created_at":"2026-05-18T04:38:58Z","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":"d531eb14eaacabb0bcfb04d1cae57422f6655bd9ea291468b98eb76dff8d45ec","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2010-09-25T16:19:43Z","title_canon_sha256":"5fdf59c933d93f5c880246d0bc14b2c45e2ce6058fed2e0bf8d3e5421e057230"},"schema_version":"1.0","source":{"id":"1010.0138","kind":"arxiv","version":1}},"canonical_sha256":"3126a7dbf6c4c44db843f0ddd2f880420452be952625e5342340e9dfdd76aeef","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3126a7dbf6c4c44db843f0ddd2f880420452be952625e5342340e9dfdd76aeef","first_computed_at":"2026-05-18T04:38:58.978238Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:38:58.978238Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5OB2tkTg0UeG1lFNgbcQx8ej3r0zWLhNDzzY1jG6whsXSblB+/3e3Xm5gxW1EzWoIOYU4fNXgS2ALDkoD9LdDw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:38:58.978860Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.0138","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:39fd9b97934458d0c3936530331b0090ab671361c40027d1f9e59281352a07fd","sha256:6479914be7c2c8bb7353c5ffa5fe04d7aae1a72092ad64e8654a348c2da9c906"],"state_sha256":"d6a83370f1741a048e76a5014b8b8ee8396eb53cae085869511293875d4d1dd6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/PiVscZW2t0675gFNUZzvrJUqf12lhlYFIjM+yyvRKi1SA0fJbr6EWzNevMCigrll/Tgl4wExpWVJE3tVQ6ZDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T12:10:50.052228Z","bundle_sha256":"e9ff695f3ff431605aab212a43b82e5ad79c02c82fc211271ebc60a9d91e7697"}}