{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:RROQEINUYD2VYPOLURBNSIJQXG","short_pith_number":"pith:RROQEINU","canonical_record":{"source":{"id":"1610.04088","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T14:05:19Z","cross_cats_sorted":["physics.atom-ph","physics.comp-ph"],"title_canon_sha256":"e9ed54748dc705bd525ab6d87d997b8acd57597cd016ddbe5e97cbf48313cebe","abstract_canon_sha256":"c25adf37d1828f5f875ae3a83c35a897c24a0a8ddbea966c760533b28da8af45"},"schema_version":"1.0"},"canonical_sha256":"8c5d0221b4c0f55c3dcba442d92130b9a0e34640b24c87cede3d1809c2d48273","source":{"kind":"arxiv","id":"1610.04088","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04088","created_at":"2026-05-18T00:35:59Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04088v2","created_at":"2026-05-18T00:35:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04088","created_at":"2026-05-18T00:35:59Z"},{"alias_kind":"pith_short_12","alias_value":"RROQEINUYD2V","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RROQEINUYD2VYPOL","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RROQEINU","created_at":"2026-05-18T12:30:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:RROQEINUYD2VYPOLURBNSIJQXG","target":"record","payload":{"canonical_record":{"source":{"id":"1610.04088","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T14:05:19Z","cross_cats_sorted":["physics.atom-ph","physics.comp-ph"],"title_canon_sha256":"e9ed54748dc705bd525ab6d87d997b8acd57597cd016ddbe5e97cbf48313cebe","abstract_canon_sha256":"c25adf37d1828f5f875ae3a83c35a897c24a0a8ddbea966c760533b28da8af45"},"schema_version":"1.0"},"canonical_sha256":"8c5d0221b4c0f55c3dcba442d92130b9a0e34640b24c87cede3d1809c2d48273","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:59.711987Z","signature_b64":"fTfzxugY+oRdbTKgtDOxvmwpCT1cZZ4EoDRbkaE8owl9MxD9EihH9NF0UrLxCuNIpvu75nQnwTLb6fIVUCiqBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c5d0221b4c0f55c3dcba442d92130b9a0e34640b24c87cede3d1809c2d48273","last_reissued_at":"2026-05-18T00:35:59.711267Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:59.711267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.04088","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":"2026-05-18T00:35:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b7ddcFhhK/1ZDEc4IfuA3hi4+D5Q3X61ZrhagqfajoAgz1cE+Tb2lnX2VRBHN0AOc6tOtklV5c/PbrnaVE8wAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T01:53:41.929263Z"},"content_sha256":"dedb526b153bf41cabc79071338e133bfa64f46e5e9cb0f5fba609f5db708eb6","schema_version":"1.0","event_id":"sha256:dedb526b153bf41cabc79071338e133bfa64f46e5e9cb0f5fba609f5db708eb6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:RROQEINUYD2VYPOLURBNSIJQXG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Targeting Eigenstates by \"Simulated Measurements\" using a Decoherence based Nonlinear Schr\\\"odinger Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","physics.comp-ph"],"primary_cat":"quant-ph","authors_text":"Miller Mendoza, Oliver Furtmaier","submitted_at":"2016-10-13T14:05:19Z","abstract_excerpt":"Inspired by the idea of mimicking the measurement on a quantum system through a decoherence process to target specific eigenstates based on Born's law, i.e. the hiearchy of probabilities instead of the hierarchy of eigenvalues, we transform a Lindblad equation for the reduced density operator into a nonlinear Schr\\\"{o}dinger equation to obtain a computationally feasible simulation of the decoherent dynamics in the open quantum system. This gives the opportunity to target the eigenstates which have the largest $L^2$ overlap with an initial superposition state and hence more flexibility in the s"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04088","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":"2026-05-18T00:35:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sL40n5HhNqWESi2VkFEWCNzlF8Y505PHrvmYZ4ogPje+44tyzTzGlfJwCPnm4mOYIeq7rGd43gpWF5hqD4y+Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-02T01:53:41.929654Z"},"content_sha256":"8596f6dfd5aab7d373e904274ed53879d7f296207d5f9759479a01862f82cebf","schema_version":"1.0","event_id":"sha256:8596f6dfd5aab7d373e904274ed53879d7f296207d5f9759479a01862f82cebf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RROQEINUYD2VYPOLURBNSIJQXG/bundle.json","state_url":"https://pith.science/pith/RROQEINUYD2VYPOLURBNSIJQXG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RROQEINUYD2VYPOLURBNSIJQXG/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":"2026-07-02T01:53:41Z","links":{"resolver":"https://pith.science/pith/RROQEINUYD2VYPOLURBNSIJQXG","bundle":"https://pith.science/pith/RROQEINUYD2VYPOLURBNSIJQXG/bundle.json","state":"https://pith.science/pith/RROQEINUYD2VYPOLURBNSIJQXG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RROQEINUYD2VYPOLURBNSIJQXG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:RROQEINUYD2VYPOLURBNSIJQXG","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":"c25adf37d1828f5f875ae3a83c35a897c24a0a8ddbea966c760533b28da8af45","cross_cats_sorted":["physics.atom-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T14:05:19Z","title_canon_sha256":"e9ed54748dc705bd525ab6d87d997b8acd57597cd016ddbe5e97cbf48313cebe"},"schema_version":"1.0","source":{"id":"1610.04088","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04088","created_at":"2026-05-18T00:35:59Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04088v2","created_at":"2026-05-18T00:35:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04088","created_at":"2026-05-18T00:35:59Z"},{"alias_kind":"pith_short_12","alias_value":"RROQEINUYD2V","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RROQEINUYD2VYPOL","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RROQEINU","created_at":"2026-05-18T12:30:41Z"}],"graph_snapshots":[{"event_id":"sha256:8596f6dfd5aab7d373e904274ed53879d7f296207d5f9759479a01862f82cebf","target":"graph","created_at":"2026-05-18T00:35:59Z","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":"Inspired by the idea of mimicking the measurement on a quantum system through a decoherence process to target specific eigenstates based on Born's law, i.e. the hiearchy of probabilities instead of the hierarchy of eigenvalues, we transform a Lindblad equation for the reduced density operator into a nonlinear Schr\\\"{o}dinger equation to obtain a computationally feasible simulation of the decoherent dynamics in the open quantum system. This gives the opportunity to target the eigenstates which have the largest $L^2$ overlap with an initial superposition state and hence more flexibility in the s","authors_text":"Miller Mendoza, Oliver Furtmaier","cross_cats":["physics.atom-ph","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T14:05:19Z","title":"Targeting Eigenstates by \"Simulated Measurements\" using a Decoherence based Nonlinear Schr\\\"odinger Equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04088","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:dedb526b153bf41cabc79071338e133bfa64f46e5e9cb0f5fba609f5db708eb6","target":"record","created_at":"2026-05-18T00:35:59Z","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":"c25adf37d1828f5f875ae3a83c35a897c24a0a8ddbea966c760533b28da8af45","cross_cats_sorted":["physics.atom-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-10-13T14:05:19Z","title_canon_sha256":"e9ed54748dc705bd525ab6d87d997b8acd57597cd016ddbe5e97cbf48313cebe"},"schema_version":"1.0","source":{"id":"1610.04088","kind":"arxiv","version":2}},"canonical_sha256":"8c5d0221b4c0f55c3dcba442d92130b9a0e34640b24c87cede3d1809c2d48273","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8c5d0221b4c0f55c3dcba442d92130b9a0e34640b24c87cede3d1809c2d48273","first_computed_at":"2026-05-18T00:35:59.711267Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:59.711267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"fTfzxugY+oRdbTKgtDOxvmwpCT1cZZ4EoDRbkaE8owl9MxD9EihH9NF0UrLxCuNIpvu75nQnwTLb6fIVUCiqBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:59.711987Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.04088","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dedb526b153bf41cabc79071338e133bfa64f46e5e9cb0f5fba609f5db708eb6","sha256:8596f6dfd5aab7d373e904274ed53879d7f296207d5f9759479a01862f82cebf"],"state_sha256":"ac3d888f2196e3df3967be060ae31dd2341de23edf97703be299be85a6dbd556"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2rmV6IAgwL2FO3c4FQIQxDM7+gbypuPVS013TBCTRn87TuLyX8OoFRVAuYG5BCm2rad8oZNyPdXzxNpY7HJ6DQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-02T01:53:41.931889Z","bundle_sha256":"294fde4020428d8e9c7b040d2e08d283e73a7c20ae9757d33a935f495f12048e"}}