{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:3SELJO7NXDGIKNNI54T5HKAOBU","short_pith_number":"pith:3SELJO7N","canonical_record":{"source":{"id":"1603.02771","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-03-09T02:56:30Z","cross_cats_sorted":["physics.atom-ph","physics.optics"],"title_canon_sha256":"ae75e5236db046444f2d4344cd55b9c6b4dc0d3f644bb2adbfec51ccd301bf3e","abstract_canon_sha256":"bad46d8719e4185025007f84c28c5615281ef6f10bcf73d355054ea597eb1690"},"schema_version":"1.0"},"canonical_sha256":"dc88b4bbedb8cc8535a8ef27d3a80e0d2ae824296c407ebeb9ed4be188b98bf4","source":{"kind":"arxiv","id":"1603.02771","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.02771","created_at":"2026-05-18T00:36:19Z"},{"alias_kind":"arxiv_version","alias_value":"1603.02771v2","created_at":"2026-05-18T00:36:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.02771","created_at":"2026-05-18T00:36:19Z"},{"alias_kind":"pith_short_12","alias_value":"3SELJO7NXDGI","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"3SELJO7NXDGIKNNI","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"3SELJO7N","created_at":"2026-05-18T12:29:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:3SELJO7NXDGIKNNI54T5HKAOBU","target":"record","payload":{"canonical_record":{"source":{"id":"1603.02771","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-03-09T02:56:30Z","cross_cats_sorted":["physics.atom-ph","physics.optics"],"title_canon_sha256":"ae75e5236db046444f2d4344cd55b9c6b4dc0d3f644bb2adbfec51ccd301bf3e","abstract_canon_sha256":"bad46d8719e4185025007f84c28c5615281ef6f10bcf73d355054ea597eb1690"},"schema_version":"1.0"},"canonical_sha256":"dc88b4bbedb8cc8535a8ef27d3a80e0d2ae824296c407ebeb9ed4be188b98bf4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:36:19.676288Z","signature_b64":"19cIa9iVMnIKtej09lR5am8FI3QYxyHAZY1Z/70qhI7D4A9buTsUmBVGEkcPEQI69FUQ4/5nXqTATYNVoS0RBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dc88b4bbedb8cc8535a8ef27d3a80e0d2ae824296c407ebeb9ed4be188b98bf4","last_reissued_at":"2026-05-18T00:36:19.675533Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:36:19.675533Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1603.02771","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":"2026-05-18T00:36:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8LG0kqZHe6/TShqjiQtYp9i5RiX7TEibTewt5UjbwgQTHVy9wmWW4C1yjyQuAE03IGz1ArWX3mGVPgox1pY/BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:41:06.652918Z"},"content_sha256":"b306d8094413fdcee887eef0e6864a344e82446930205f3a1a98dff457553646","schema_version":"1.0","event_id":"sha256:b306d8094413fdcee887eef0e6864a344e82446930205f3a1a98dff457553646"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:3SELJO7NXDGIKNNI54T5HKAOBU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Atom-atom interactions around the band edge of a photonic crystal waveguide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atom-ph","physics.optics"],"primary_cat":"quant-ph","authors_text":"A. Asenjo-Garcia, A. Goban, D. E. Chang, H. J. Kimble, J. D. Hood, M. Lu, S.-P. Yu","submitted_at":"2016-03-09T02:56:30Z","abstract_excerpt":"Tailoring the interactions between quantum emitters and single photons constitutes one of the cornerstones of quantum optics. Coupling a quantum emitter to the band edge of a photonic crystal waveguide (PCW) provides a unique platform for tuning these interactions. In particular, the crossover from propagating fields $E(x) \\propto e^{\\pm ik_x x}$ outside the bandgap to localized fields $E(x) \\propto e^{-\\kappa_x |x|}$ within the bandgap should be accompanied by a transition from largely dissipative atom-atom interactions to a regime where dispersive atom-atom interactions are dominant. Here, w"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.02771","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":"2026-05-18T00:36:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wVpyhgZguqi9Nqpo2esXtJaG0AaEu4mkKtfxcGUiTd1c5bSKkA56Xq+nGpCII2Yi/KqodB+EzNgHzwqk0LzHBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:41:06.653393Z"},"content_sha256":"e01917eea4c36bb1e34aaa7069a5b7bf64ce237523a1d32c03bdf5ce7c3a4c2a","schema_version":"1.0","event_id":"sha256:e01917eea4c36bb1e34aaa7069a5b7bf64ce237523a1d32c03bdf5ce7c3a4c2a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3SELJO7NXDGIKNNI54T5HKAOBU/bundle.json","state_url":"https://pith.science/pith/3SELJO7NXDGIKNNI54T5HKAOBU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3SELJO7NXDGIKNNI54T5HKAOBU/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":"2026-05-26T20:41:06Z","links":{"resolver":"https://pith.science/pith/3SELJO7NXDGIKNNI54T5HKAOBU","bundle":"https://pith.science/pith/3SELJO7NXDGIKNNI54T5HKAOBU/bundle.json","state":"https://pith.science/pith/3SELJO7NXDGIKNNI54T5HKAOBU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3SELJO7NXDGIKNNI54T5HKAOBU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:3SELJO7NXDGIKNNI54T5HKAOBU","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":"bad46d8719e4185025007f84c28c5615281ef6f10bcf73d355054ea597eb1690","cross_cats_sorted":["physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-03-09T02:56:30Z","title_canon_sha256":"ae75e5236db046444f2d4344cd55b9c6b4dc0d3f644bb2adbfec51ccd301bf3e"},"schema_version":"1.0","source":{"id":"1603.02771","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.02771","created_at":"2026-05-18T00:36:19Z"},{"alias_kind":"arxiv_version","alias_value":"1603.02771v2","created_at":"2026-05-18T00:36:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.02771","created_at":"2026-05-18T00:36:19Z"},{"alias_kind":"pith_short_12","alias_value":"3SELJO7NXDGI","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_16","alias_value":"3SELJO7NXDGIKNNI","created_at":"2026-05-18T12:29:58Z"},{"alias_kind":"pith_short_8","alias_value":"3SELJO7N","created_at":"2026-05-18T12:29:58Z"}],"graph_snapshots":[{"event_id":"sha256:e01917eea4c36bb1e34aaa7069a5b7bf64ce237523a1d32c03bdf5ce7c3a4c2a","target":"graph","created_at":"2026-05-18T00:36:19Z","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":"Tailoring the interactions between quantum emitters and single photons constitutes one of the cornerstones of quantum optics. Coupling a quantum emitter to the band edge of a photonic crystal waveguide (PCW) provides a unique platform for tuning these interactions. In particular, the crossover from propagating fields $E(x) \\propto e^{\\pm ik_x x}$ outside the bandgap to localized fields $E(x) \\propto e^{-\\kappa_x |x|}$ within the bandgap should be accompanied by a transition from largely dissipative atom-atom interactions to a regime where dispersive atom-atom interactions are dominant. Here, w","authors_text":"A. Asenjo-Garcia, A. Goban, D. E. Chang, H. J. Kimble, J. D. Hood, M. Lu, S.-P. Yu","cross_cats":["physics.atom-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-03-09T02:56:30Z","title":"Atom-atom interactions around the band edge of a photonic crystal waveguide"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.02771","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:b306d8094413fdcee887eef0e6864a344e82446930205f3a1a98dff457553646","target":"record","created_at":"2026-05-18T00:36:19Z","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":"bad46d8719e4185025007f84c28c5615281ef6f10bcf73d355054ea597eb1690","cross_cats_sorted":["physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-03-09T02:56:30Z","title_canon_sha256":"ae75e5236db046444f2d4344cd55b9c6b4dc0d3f644bb2adbfec51ccd301bf3e"},"schema_version":"1.0","source":{"id":"1603.02771","kind":"arxiv","version":2}},"canonical_sha256":"dc88b4bbedb8cc8535a8ef27d3a80e0d2ae824296c407ebeb9ed4be188b98bf4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dc88b4bbedb8cc8535a8ef27d3a80e0d2ae824296c407ebeb9ed4be188b98bf4","first_computed_at":"2026-05-18T00:36:19.675533Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:36:19.675533Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"19cIa9iVMnIKtej09lR5am8FI3QYxyHAZY1Z/70qhI7D4A9buTsUmBVGEkcPEQI69FUQ4/5nXqTATYNVoS0RBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:36:19.676288Z","signed_message":"canonical_sha256_bytes"},"source_id":"1603.02771","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b306d8094413fdcee887eef0e6864a344e82446930205f3a1a98dff457553646","sha256:e01917eea4c36bb1e34aaa7069a5b7bf64ce237523a1d32c03bdf5ce7c3a4c2a"],"state_sha256":"313dab65307ccb1597559f6b386cfa4e06c2cacdfb457c75e9aa2fb4e29473e4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WtyAEwVSPcXsyLJBAAwOzDy4hcnfjfdV/5o0EQDfRsfA/whwdUUu8xbKCjm0g0lnRsh5l06BcUxj+JQyJ3YyAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T20:41:06.656701Z","bundle_sha256":"011db0b1be54f3f26fddbf55486d4101ed06b2b887107f44a04a271c5f1dd410"}}