{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:SP5KGYK2IGDQ3Z6XDFXYOOYRAH","short_pith_number":"pith:SP5KGYK2","canonical_record":{"source":{"id":"1710.02424","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-06T14:31:37Z","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"title_canon_sha256":"39f52ec8c2c01e80d4171ba97fb6d218de5ad5c91f17bc2968fc4826b4c7b515","abstract_canon_sha256":"34a0d667beabc7f246b9f2de40175ce5915f3c9513455a5790b56e1f6217e122"},"schema_version":"1.0"},"canonical_sha256":"93faa3615a41870de7d7196f873b1101c1fbde56be0ab194775cdf9963088a00","source":{"kind":"arxiv","id":"1710.02424","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.02424","created_at":"2026-05-18T00:01:38Z"},{"alias_kind":"arxiv_version","alias_value":"1710.02424v3","created_at":"2026-05-18T00:01:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02424","created_at":"2026-05-18T00:01:38Z"},{"alias_kind":"pith_short_12","alias_value":"SP5KGYK2IGDQ","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"SP5KGYK2IGDQ3Z6X","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"SP5KGYK2","created_at":"2026-05-18T12:31:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:SP5KGYK2IGDQ3Z6XDFXYOOYRAH","target":"record","payload":{"canonical_record":{"source":{"id":"1710.02424","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-06T14:31:37Z","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"title_canon_sha256":"39f52ec8c2c01e80d4171ba97fb6d218de5ad5c91f17bc2968fc4826b4c7b515","abstract_canon_sha256":"34a0d667beabc7f246b9f2de40175ce5915f3c9513455a5790b56e1f6217e122"},"schema_version":"1.0"},"canonical_sha256":"93faa3615a41870de7d7196f873b1101c1fbde56be0ab194775cdf9963088a00","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:01:38.942760Z","signature_b64":"bUqvKgu+G33d07txuhEzvPULQWB8u6jhks7e5ZMDm6HZIBUvgB5BA66bOn3iYoIjF72mnUUxIHl0Kx037EPgCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"93faa3615a41870de7d7196f873b1101c1fbde56be0ab194775cdf9963088a00","last_reissued_at":"2026-05-18T00:01:38.942331Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:01:38.942331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1710.02424","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:01:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Vc307MVgPtj3qoKkXDfyEMaOMN3+aVVLXhwIeLIpwAvkXaSBbLJ7q5mHvcUJ+8ISzeORunh2I7OhI5RiTfCjCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T21:20:57.263417Z"},"content_sha256":"d4a20099da1c178c1e68970d9d9c3c8f22fe133e1b75bf47b3f863e92d1b44cf","schema_version":"1.0","event_id":"sha256:d4a20099da1c178c1e68970d9d9c3c8f22fe133e1b75bf47b3f863e92d1b44cf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:SP5KGYK2IGDQ3Z6XDFXYOOYRAH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Effective Three-Body Interactions in Jaynes-Cummings-Hubbard Systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Andrew M. Martin, Srivatsa B. Prasad","submitted_at":"2017-10-06T14:31:37Z","abstract_excerpt":"A generalisation of the Jaynes-Cummings-Hubbard model for coupled-cavity arrays is introduced, where the embedded two-level system in each cavity is replaced by a $\\Xi$-type three-level system. We demonstrate that the resulting effective polariton-polariton interactions at each site are both two-body and three-body. By tuning the ratio of the two transition dipole matrix elements, we show that the strength and sign of the two-body interaction can be controlled whilst maintaining a three-body repulsion. We then proceed to demonstrate how different two-body and three-body interactions alter the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02424","kind":"arxiv","version":3},"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":"2026-05-18T00:01:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AOKyV+Ooyd0jKufM/x4Fk8dYJbDXN8MD75QY6kowuJlA/7oNAZ3DqkajNzfzlKAuRiz2cRFhZuHIJVOtvdeEAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-24T21:20:57.263770Z"},"content_sha256":"0b1d866a02022433b6fa042d39565f00f8abf46116d38b124cf204d38e784557","schema_version":"1.0","event_id":"sha256:0b1d866a02022433b6fa042d39565f00f8abf46116d38b124cf204d38e784557"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH/bundle.json","state_url":"https://pith.science/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH/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":"2026-06-24T21:20:57Z","links":{"resolver":"https://pith.science/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH","bundle":"https://pith.science/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH/bundle.json","state":"https://pith.science/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SP5KGYK2IGDQ3Z6XDFXYOOYRAH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:SP5KGYK2IGDQ3Z6XDFXYOOYRAH","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":"34a0d667beabc7f246b9f2de40175ce5915f3c9513455a5790b56e1f6217e122","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-06T14:31:37Z","title_canon_sha256":"39f52ec8c2c01e80d4171ba97fb6d218de5ad5c91f17bc2968fc4826b4c7b515"},"schema_version":"1.0","source":{"id":"1710.02424","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1710.02424","created_at":"2026-05-18T00:01:38Z"},{"alias_kind":"arxiv_version","alias_value":"1710.02424v3","created_at":"2026-05-18T00:01:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02424","created_at":"2026-05-18T00:01:38Z"},{"alias_kind":"pith_short_12","alias_value":"SP5KGYK2IGDQ","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"SP5KGYK2IGDQ3Z6X","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"SP5KGYK2","created_at":"2026-05-18T12:31:43Z"}],"graph_snapshots":[{"event_id":"sha256:0b1d866a02022433b6fa042d39565f00f8abf46116d38b124cf204d38e784557","target":"graph","created_at":"2026-05-18T00:01:38Z","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":"A generalisation of the Jaynes-Cummings-Hubbard model for coupled-cavity arrays is introduced, where the embedded two-level system in each cavity is replaced by a $\\Xi$-type three-level system. We demonstrate that the resulting effective polariton-polariton interactions at each site are both two-body and three-body. By tuning the ratio of the two transition dipole matrix elements, we show that the strength and sign of the two-body interaction can be controlled whilst maintaining a three-body repulsion. We then proceed to demonstrate how different two-body and three-body interactions alter the ","authors_text":"Andrew M. Martin, Srivatsa B. Prasad","cross_cats":["cond-mat.mes-hall","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-06T14:31:37Z","title":"Effective Three-Body Interactions in Jaynes-Cummings-Hubbard Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02424","kind":"arxiv","version":3},"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:d4a20099da1c178c1e68970d9d9c3c8f22fe133e1b75bf47b3f863e92d1b44cf","target":"record","created_at":"2026-05-18T00:01:38Z","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":"34a0d667beabc7f246b9f2de40175ce5915f3c9513455a5790b56e1f6217e122","cross_cats_sorted":["cond-mat.mes-hall","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2017-10-06T14:31:37Z","title_canon_sha256":"39f52ec8c2c01e80d4171ba97fb6d218de5ad5c91f17bc2968fc4826b4c7b515"},"schema_version":"1.0","source":{"id":"1710.02424","kind":"arxiv","version":3}},"canonical_sha256":"93faa3615a41870de7d7196f873b1101c1fbde56be0ab194775cdf9963088a00","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"93faa3615a41870de7d7196f873b1101c1fbde56be0ab194775cdf9963088a00","first_computed_at":"2026-05-18T00:01:38.942331Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:01:38.942331Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bUqvKgu+G33d07txuhEzvPULQWB8u6jhks7e5ZMDm6HZIBUvgB5BA66bOn3iYoIjF72mnUUxIHl0Kx037EPgCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:01:38.942760Z","signed_message":"canonical_sha256_bytes"},"source_id":"1710.02424","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d4a20099da1c178c1e68970d9d9c3c8f22fe133e1b75bf47b3f863e92d1b44cf","sha256:0b1d866a02022433b6fa042d39565f00f8abf46116d38b124cf204d38e784557"],"state_sha256":"1793f83c7638b869a4b4393c36d3a8a4a7ff017eb06509c27b796aaf4d2d0079"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KFNWdJQ8EShHM6KLsXDToADvrvy/UwJ5pC6Btp+H1SL5jkmhebPA4lRDZQLEBkw278wCxH6OBSZsu0St1CXRCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-24T21:20:57.265759Z","bundle_sha256":"0e4d63093f02c38fb0497f162ff8be0bad5013b0a6a4dede519b81116204c536"}}