{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:ZASCIMPGACWTF3BPFYKWMC4GRV","short_pith_number":"pith:ZASCIMPG","canonical_record":{"source":{"id":"1705.01124","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-02T18:18:01Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"0b5e3086e20fd393dff0823d0e44add3d911a65d9ea9937726c5054ead384120","abstract_canon_sha256":"be102e20829fda1f70d44217bcc2b47b3f50eadae16469a1dffe4e94b2d63708"},"schema_version":"1.0"},"canonical_sha256":"c8242431e600ad32ec2f2e15660b868d4695f0e650e05825328b9b6985a1d2bc","source":{"kind":"arxiv","id":"1705.01124","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.01124","created_at":"2026-05-18T00:23:39Z"},{"alias_kind":"arxiv_version","alias_value":"1705.01124v1","created_at":"2026-05-18T00:23:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01124","created_at":"2026-05-18T00:23:39Z"},{"alias_kind":"pith_short_12","alias_value":"ZASCIMPGACWT","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_16","alias_value":"ZASCIMPGACWTF3BP","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_8","alias_value":"ZASCIMPG","created_at":"2026-05-18T12:31:59Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:ZASCIMPGACWTF3BPFYKWMC4GRV","target":"record","payload":{"canonical_record":{"source":{"id":"1705.01124","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-02T18:18:01Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"0b5e3086e20fd393dff0823d0e44add3d911a65d9ea9937726c5054ead384120","abstract_canon_sha256":"be102e20829fda1f70d44217bcc2b47b3f50eadae16469a1dffe4e94b2d63708"},"schema_version":"1.0"},"canonical_sha256":"c8242431e600ad32ec2f2e15660b868d4695f0e650e05825328b9b6985a1d2bc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:23:39.147775Z","signature_b64":"229RNOH7MBVbPBTRvfLxbaZZWmjdUyLBuDcEV7Ia1ktnYNjWxLNxfdqGDV7nAzNU4LHGyCdtZ3/8WoKIEieaCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c8242431e600ad32ec2f2e15660b868d4695f0e650e05825328b9b6985a1d2bc","last_reissued_at":"2026-05-18T00:23:39.146924Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:23:39.146924Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.01124","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":"2026-05-18T00:23:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oQYMLhrEj4GcsMz1U/7EgUB9mgrThLl8UR6nu+G828CcRj2Zi2I2Sgvvn8pAhQelJ8Xo0c0N6kb3HgwdkP1qCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T17:40:48.970930Z"},"content_sha256":"daf97fcc4d82febef762e901eb82701ba38980342a292c06f072e3826b3ba64d","schema_version":"1.0","event_id":"sha256:daf97fcc4d82febef762e901eb82701ba38980342a292c06f072e3826b3ba64d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:ZASCIMPGACWTF3BPFYKWMC4GRV","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Theory of optically controlled anisotropic polariton transport in semiconductor double microcavities","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"E. Baudin, J. Tignon, K.P. Chan, M. Babilon, N.H. Kwong, O. Lafont, P. Lewandowski, P.T. Leung, R. Binder, S.M.H. Luk, S. Schumacher","submitted_at":"2017-05-02T18:18:01Z","abstract_excerpt":"Exciton polaritons in semiconductor microcavities exhibit many fundamental physical effects, with some of them amenable to being controlled by external fields. The polariton transport is affected by the polaritonic spin-orbit interaction, which is caused by the splitting of transverse-electric and transverse-magnetic (TE-TM) modes. This is the basis for a polaritonic Hall effect, called optical spin Hall effect (OSHE), which is related to the formation of spin/polarization textures in momentum space, determining anisotropic ballistic transport, as well as related textures in real space. Owing "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01124","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":"2026-05-18T00:23:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JFmbbuiHyaaV6+6GuBjO+2pFK/UCbqjcSiA8bbr9F46v2GfqysYKYMMVAiq3zrzCM2/JJiXV44AOuvtyhzClAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T17:40:48.971633Z"},"content_sha256":"4ee9d199ae016acc6e1ee6cdafb19d81785fc768131a82b3019787483b6b1164","schema_version":"1.0","event_id":"sha256:4ee9d199ae016acc6e1ee6cdafb19d81785fc768131a82b3019787483b6b1164"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZASCIMPGACWTF3BPFYKWMC4GRV/bundle.json","state_url":"https://pith.science/pith/ZASCIMPGACWTF3BPFYKWMC4GRV/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZASCIMPGACWTF3BPFYKWMC4GRV/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":"2026-05-25T17:40:48Z","links":{"resolver":"https://pith.science/pith/ZASCIMPGACWTF3BPFYKWMC4GRV","bundle":"https://pith.science/pith/ZASCIMPGACWTF3BPFYKWMC4GRV/bundle.json","state":"https://pith.science/pith/ZASCIMPGACWTF3BPFYKWMC4GRV/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZASCIMPGACWTF3BPFYKWMC4GRV/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:ZASCIMPGACWTF3BPFYKWMC4GRV","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":"be102e20829fda1f70d44217bcc2b47b3f50eadae16469a1dffe4e94b2d63708","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-02T18:18:01Z","title_canon_sha256":"0b5e3086e20fd393dff0823d0e44add3d911a65d9ea9937726c5054ead384120"},"schema_version":"1.0","source":{"id":"1705.01124","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.01124","created_at":"2026-05-18T00:23:39Z"},{"alias_kind":"arxiv_version","alias_value":"1705.01124v1","created_at":"2026-05-18T00:23:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.01124","created_at":"2026-05-18T00:23:39Z"},{"alias_kind":"pith_short_12","alias_value":"ZASCIMPGACWT","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_16","alias_value":"ZASCIMPGACWTF3BP","created_at":"2026-05-18T12:31:59Z"},{"alias_kind":"pith_short_8","alias_value":"ZASCIMPG","created_at":"2026-05-18T12:31:59Z"}],"graph_snapshots":[{"event_id":"sha256:4ee9d199ae016acc6e1ee6cdafb19d81785fc768131a82b3019787483b6b1164","target":"graph","created_at":"2026-05-18T00:23:39Z","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":"Exciton polaritons in semiconductor microcavities exhibit many fundamental physical effects, with some of them amenable to being controlled by external fields. The polariton transport is affected by the polaritonic spin-orbit interaction, which is caused by the splitting of transverse-electric and transverse-magnetic (TE-TM) modes. This is the basis for a polaritonic Hall effect, called optical spin Hall effect (OSHE), which is related to the formation of spin/polarization textures in momentum space, determining anisotropic ballistic transport, as well as related textures in real space. Owing ","authors_text":"E. Baudin, J. Tignon, K.P. Chan, M. Babilon, N.H. Kwong, O. Lafont, P. Lewandowski, P.T. Leung, R. Binder, S.M.H. Luk, S. Schumacher","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-02T18:18:01Z","title":"Theory of optically controlled anisotropic polariton transport in semiconductor double microcavities"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.01124","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:daf97fcc4d82febef762e901eb82701ba38980342a292c06f072e3826b3ba64d","target":"record","created_at":"2026-05-18T00:23:39Z","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":"be102e20829fda1f70d44217bcc2b47b3f50eadae16469a1dffe4e94b2d63708","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-02T18:18:01Z","title_canon_sha256":"0b5e3086e20fd393dff0823d0e44add3d911a65d9ea9937726c5054ead384120"},"schema_version":"1.0","source":{"id":"1705.01124","kind":"arxiv","version":1}},"canonical_sha256":"c8242431e600ad32ec2f2e15660b868d4695f0e650e05825328b9b6985a1d2bc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c8242431e600ad32ec2f2e15660b868d4695f0e650e05825328b9b6985a1d2bc","first_computed_at":"2026-05-18T00:23:39.146924Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:23:39.146924Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"229RNOH7MBVbPBTRvfLxbaZZWmjdUyLBuDcEV7Ia1ktnYNjWxLNxfdqGDV7nAzNU4LHGyCdtZ3/8WoKIEieaCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:23:39.147775Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.01124","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:daf97fcc4d82febef762e901eb82701ba38980342a292c06f072e3826b3ba64d","sha256:4ee9d199ae016acc6e1ee6cdafb19d81785fc768131a82b3019787483b6b1164"],"state_sha256":"a3d9f88462e0d51e428c38176f9e7a1b7213292a7dd23a2ec1c607dfd0ca7adf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"SmDCFDGSBS/re/58RYJYm2tQIs/PLcQK9KNxJW27BAU15WTuoF48Zr9TVQD00hSWCGxANl3qD411j51McSUqBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T17:40:48.975585Z","bundle_sha256":"d9f199daa63ebf12ca49a12c3d8e8c6e04571ac1dffbd387a4ef19d4021a2ea3"}}