{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:XOMB23SJEULVG45J4ZTAE32S3T","short_pith_number":"pith:XOMB23SJ","canonical_record":{"source":{"id":"1704.02394","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-04-07T22:42:51Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"bde87fe3ba4b65a90bb88a0805defac13a89fe28deee26d7e5ee249c3b882c9c","abstract_canon_sha256":"b819237e18b75af4be84f1e2f786b29826483aa2771aaf3c3c24f098be108012"},"schema_version":"1.0"},"canonical_sha256":"bb981d6e4925175373a9e666026f52dcd050582cd6a854c7ff6eaaa8d842349d","source":{"kind":"arxiv","id":"1704.02394","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.02394","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"arxiv_version","alias_value":"1704.02394v1","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.02394","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"pith_short_12","alias_value":"XOMB23SJEULV","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XOMB23SJEULVG45J","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XOMB23SJ","created_at":"2026-05-18T12:31:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:XOMB23SJEULVG45J4ZTAE32S3T","target":"record","payload":{"canonical_record":{"source":{"id":"1704.02394","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-04-07T22:42:51Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"bde87fe3ba4b65a90bb88a0805defac13a89fe28deee26d7e5ee249c3b882c9c","abstract_canon_sha256":"b819237e18b75af4be84f1e2f786b29826483aa2771aaf3c3c24f098be108012"},"schema_version":"1.0"},"canonical_sha256":"bb981d6e4925175373a9e666026f52dcd050582cd6a854c7ff6eaaa8d842349d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:43.547688Z","signature_b64":"BAVL4IV8gHUPu7Wco6OXBAs+P/0a0TibpZf7zLbkWxupnGPxxqn+DbJJqb5HT99XTI8D2JBaCEzy/QiDTr00Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb981d6e4925175373a9e666026f52dcd050582cd6a854c7ff6eaaa8d842349d","last_reissued_at":"2026-05-18T00:32:43.547071Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:43.547071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1704.02394","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":"2026-05-18T00:32:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mx3/CmHk+PbLlETKU7wc5soCQSGR4Pq4VOLBGdMK1R/RZGaez8qGKYxfNnBT+mrDhn2C2qA5w/2gYmIECDxhCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T13:26:20.984881Z"},"content_sha256":"ce0e5c3569d9a9b1d415624a1a330883baa9866ac40447478708971f731fd0a1","schema_version":"1.0","event_id":"sha256:ce0e5c3569d9a9b1d415624a1a330883baa9866ac40447478708971f731fd0a1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:XOMB23SJEULVG45J4ZTAE32S3T","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coherent Optomechanical State Transfer between Disparate Mechanical Resonators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.optics","authors_text":"Dirk Bouwmeester, Fernando Luna, Frank M. Buters, Hedwig J. Eerkens, Kier Heeck, Matthew J. Weaver, Sven de Man","submitted_at":"2017-04-07T22:42:51Z","abstract_excerpt":"Hybrid quantum systems have been developed with various mechanical, optical and microwave harmonic oscillators. The coupling produces a rich library of interactions including two mode squeezing, swapping interactions, back-action evasion and thermal control. In a multimode mechanical system, coupling resonators of different scales (both in frequency and mass) leverages the advantages of each resonance. For example: a high frequency, easily manipulated resonator could be entangled with a low frequency massive object for tests of gravitational decoherence. Here we demonstrate coherent optomechan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.02394","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":"2026-05-18T00:32:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yETYrYIDSpRd2R8wg+FPgTJoD78ZTmNNi9wSTpzSA+Fm/zmQGxALLuRJ5zBnsAhyMMihnF8xN3BASgOF/IwIBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T13:26:20.985489Z"},"content_sha256":"ca68ddbbd06857a5fb0ab2b1fcee6858eab72ff1651608dd86b5027d834f74c5","schema_version":"1.0","event_id":"sha256:ca68ddbbd06857a5fb0ab2b1fcee6858eab72ff1651608dd86b5027d834f74c5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XOMB23SJEULVG45J4ZTAE32S3T/bundle.json","state_url":"https://pith.science/pith/XOMB23SJEULVG45J4ZTAE32S3T/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XOMB23SJEULVG45J4ZTAE32S3T/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":"2026-06-08T13:26:20Z","links":{"resolver":"https://pith.science/pith/XOMB23SJEULVG45J4ZTAE32S3T","bundle":"https://pith.science/pith/XOMB23SJEULVG45J4ZTAE32S3T/bundle.json","state":"https://pith.science/pith/XOMB23SJEULVG45J4ZTAE32S3T/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XOMB23SJEULVG45J4ZTAE32S3T/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:XOMB23SJEULVG45J4ZTAE32S3T","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":"b819237e18b75af4be84f1e2f786b29826483aa2771aaf3c3c24f098be108012","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-04-07T22:42:51Z","title_canon_sha256":"bde87fe3ba4b65a90bb88a0805defac13a89fe28deee26d7e5ee249c3b882c9c"},"schema_version":"1.0","source":{"id":"1704.02394","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.02394","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"arxiv_version","alias_value":"1704.02394v1","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.02394","created_at":"2026-05-18T00:32:43Z"},{"alias_kind":"pith_short_12","alias_value":"XOMB23SJEULV","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_16","alias_value":"XOMB23SJEULVG45J","created_at":"2026-05-18T12:31:56Z"},{"alias_kind":"pith_short_8","alias_value":"XOMB23SJ","created_at":"2026-05-18T12:31:56Z"}],"graph_snapshots":[{"event_id":"sha256:ca68ddbbd06857a5fb0ab2b1fcee6858eab72ff1651608dd86b5027d834f74c5","target":"graph","created_at":"2026-05-18T00:32:43Z","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":"Hybrid quantum systems have been developed with various mechanical, optical and microwave harmonic oscillators. The coupling produces a rich library of interactions including two mode squeezing, swapping interactions, back-action evasion and thermal control. In a multimode mechanical system, coupling resonators of different scales (both in frequency and mass) leverages the advantages of each resonance. For example: a high frequency, easily manipulated resonator could be entangled with a low frequency massive object for tests of gravitational decoherence. Here we demonstrate coherent optomechan","authors_text":"Dirk Bouwmeester, Fernando Luna, Frank M. Buters, Hedwig J. Eerkens, Kier Heeck, Matthew J. Weaver, Sven de Man","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-04-07T22:42:51Z","title":"Coherent Optomechanical State Transfer between Disparate Mechanical Resonators"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.02394","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:ce0e5c3569d9a9b1d415624a1a330883baa9866ac40447478708971f731fd0a1","target":"record","created_at":"2026-05-18T00:32:43Z","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":"b819237e18b75af4be84f1e2f786b29826483aa2771aaf3c3c24f098be108012","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2017-04-07T22:42:51Z","title_canon_sha256":"bde87fe3ba4b65a90bb88a0805defac13a89fe28deee26d7e5ee249c3b882c9c"},"schema_version":"1.0","source":{"id":"1704.02394","kind":"arxiv","version":1}},"canonical_sha256":"bb981d6e4925175373a9e666026f52dcd050582cd6a854c7ff6eaaa8d842349d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"bb981d6e4925175373a9e666026f52dcd050582cd6a854c7ff6eaaa8d842349d","first_computed_at":"2026-05-18T00:32:43.547071Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:32:43.547071Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BAVL4IV8gHUPu7Wco6OXBAs+P/0a0TibpZf7zLbkWxupnGPxxqn+DbJJqb5HT99XTI8D2JBaCEzy/QiDTr00Bw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:32:43.547688Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.02394","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ce0e5c3569d9a9b1d415624a1a330883baa9866ac40447478708971f731fd0a1","sha256:ca68ddbbd06857a5fb0ab2b1fcee6858eab72ff1651608dd86b5027d834f74c5"],"state_sha256":"8a848cc85104878db5050a34eecfd3ce27fd16d28bf8c0ff3b6ccb0ca63cb29a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"o/tcAZYYZAKIWq/+sg5ZFR3z7YFqN94ZZdtGZewvIOBuowM1iQlw+AABdeKWFT0UBv86CnAOsRYD2Zym9DTaDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T13:26:20.988245Z","bundle_sha256":"8d05ef807d1bb70c991d1a093c712e21adc5296f9268e14086f0a1a401fd2bae"}}