{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:7Q3TNLCAL2SBH26HEQ2PKPQDF2","short_pith_number":"pith:7Q3TNLCA","canonical_record":{"source":{"id":"1412.5192","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-12-16T21:02:53Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"725bb3e65b9afe03a4061913155354fcb9962e442e8f607922a8463a1793ffb9","abstract_canon_sha256":"c07ca6124ed624c66d193cd891558616973fb29bb8dffa6e5b2880f365d784a1"},"schema_version":"1.0"},"canonical_sha256":"fc3736ac405ea413ebc72434f53e032eb339684f0d3a7eb42b6c687adf10f2d8","source":{"kind":"arxiv","id":"1412.5192","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5192","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5192v1","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5192","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"pith_short_12","alias_value":"7Q3TNLCAL2SB","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"7Q3TNLCAL2SBH26H","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"7Q3TNLCA","created_at":"2026-05-18T12:28:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:7Q3TNLCAL2SBH26HEQ2PKPQDF2","target":"record","payload":{"canonical_record":{"source":{"id":"1412.5192","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-12-16T21:02:53Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"725bb3e65b9afe03a4061913155354fcb9962e442e8f607922a8463a1793ffb9","abstract_canon_sha256":"c07ca6124ed624c66d193cd891558616973fb29bb8dffa6e5b2880f365d784a1"},"schema_version":"1.0"},"canonical_sha256":"fc3736ac405ea413ebc72434f53e032eb339684f0d3a7eb42b6c687adf10f2d8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:14.839542Z","signature_b64":"PfFOys8R9L/Lgi5QbdBaH4nCOkq4o+WC21TjRGNajMBDF7MLJdKmjUlT6vPSEXE+DHIRR8GXfVykdFM4PlziAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc3736ac405ea413ebc72434f53e032eb339684f0d3a7eb42b6c687adf10f2d8","last_reissued_at":"2026-05-18T01:18:14.838971Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:14.838971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.5192","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":"2026-05-18T01:18:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/eN2NLXHDdqIL0b+YbYG7gyCySAbBgSmSZkA/Y0V8xPXgahmwRTNC1sExQrQiabrk1n4Anxt9t5EpiCiedqNDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T14:30:31.250511Z"},"content_sha256":"7a871ad2b340b1df7136f6984d5e428ad37e8ee6851a90d4ff9193e9d821fc8a","schema_version":"1.0","event_id":"sha256:7a871ad2b340b1df7136f6984d5e428ad37e8ee6851a90d4ff9193e9d821fc8a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:7Q3TNLCAL2SBH26HEQ2PKPQDF2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Giant Narrowband Twin-Beam Generation along the Pump Energy Propagation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"Angela M. Perez, Gerd Leuchs, Kirill Yu. Spasibko, Maria V. Chekhova, Olga V. Tikhonova, Polina R. Sharapova","submitted_at":"2014-12-16T21:02:53Z","abstract_excerpt":"Walk-off effects, originating from the difference between the group and phase velocities, limit the efficiency of nonlinear optical interactions. While transverse walk-off can be eliminated by proper medium engineering, longitudinal walk-off is harder to avoid. In particular, ultrafast twin- beam generation via pulsed parametric down-conversion (PDC) and four-wave mixing (FWM) is only possible in short crystals or fibres or in double-path schemes. Here we show that in high-gain PDC, one can overcome the destructive role of both effects and even turn them into useful tools for shaping the emiss"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5192","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":"2026-05-18T01:18:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TwkGCoV/k7aKCRdeGCTkPr3ZNyht65tBKQQwhA4k+WZMT2FH2KNIPrC+46f7qY4FSQTMnShFw4CldUDoF3HsBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T14:30:31.251291Z"},"content_sha256":"86b0d474f5c7098c9600ad06db29b141a1e158b9f45d4a893e0d16af059ad92d","schema_version":"1.0","event_id":"sha256:86b0d474f5c7098c9600ad06db29b141a1e158b9f45d4a893e0d16af059ad92d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2/bundle.json","state_url":"https://pith.science/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2/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":"2026-05-31T14:30:31Z","links":{"resolver":"https://pith.science/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2","bundle":"https://pith.science/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2/bundle.json","state":"https://pith.science/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7Q3TNLCAL2SBH26HEQ2PKPQDF2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:7Q3TNLCAL2SBH26HEQ2PKPQDF2","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":"c07ca6124ed624c66d193cd891558616973fb29bb8dffa6e5b2880f365d784a1","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-12-16T21:02:53Z","title_canon_sha256":"725bb3e65b9afe03a4061913155354fcb9962e442e8f607922a8463a1793ffb9"},"schema_version":"1.0","source":{"id":"1412.5192","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.5192","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"arxiv_version","alias_value":"1412.5192v1","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.5192","created_at":"2026-05-18T01:18:14Z"},{"alias_kind":"pith_short_12","alias_value":"7Q3TNLCAL2SB","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_16","alias_value":"7Q3TNLCAL2SBH26H","created_at":"2026-05-18T12:28:19Z"},{"alias_kind":"pith_short_8","alias_value":"7Q3TNLCA","created_at":"2026-05-18T12:28:19Z"}],"graph_snapshots":[{"event_id":"sha256:86b0d474f5c7098c9600ad06db29b141a1e158b9f45d4a893e0d16af059ad92d","target":"graph","created_at":"2026-05-18T01:18:14Z","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":"Walk-off effects, originating from the difference between the group and phase velocities, limit the efficiency of nonlinear optical interactions. While transverse walk-off can be eliminated by proper medium engineering, longitudinal walk-off is harder to avoid. In particular, ultrafast twin- beam generation via pulsed parametric down-conversion (PDC) and four-wave mixing (FWM) is only possible in short crystals or fibres or in double-path schemes. Here we show that in high-gain PDC, one can overcome the destructive role of both effects and even turn them into useful tools for shaping the emiss","authors_text":"Angela M. Perez, Gerd Leuchs, Kirill Yu. Spasibko, Maria V. Chekhova, Olga V. Tikhonova, Polina R. Sharapova","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-12-16T21:02:53Z","title":"Giant Narrowband Twin-Beam Generation along the Pump Energy Propagation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.5192","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":"sha256:7a871ad2b340b1df7136f6984d5e428ad37e8ee6851a90d4ff9193e9d821fc8a","target":"record","created_at":"2026-05-18T01:18:14Z","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":"c07ca6124ed624c66d193cd891558616973fb29bb8dffa6e5b2880f365d784a1","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2014-12-16T21:02:53Z","title_canon_sha256":"725bb3e65b9afe03a4061913155354fcb9962e442e8f607922a8463a1793ffb9"},"schema_version":"1.0","source":{"id":"1412.5192","kind":"arxiv","version":1}},"canonical_sha256":"fc3736ac405ea413ebc72434f53e032eb339684f0d3a7eb42b6c687adf10f2d8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fc3736ac405ea413ebc72434f53e032eb339684f0d3a7eb42b6c687adf10f2d8","first_computed_at":"2026-05-18T01:18:14.838971Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:18:14.838971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PfFOys8R9L/Lgi5QbdBaH4nCOkq4o+WC21TjRGNajMBDF7MLJdKmjUlT6vPSEXE+DHIRR8GXfVykdFM4PlziAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:18:14.839542Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.5192","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7a871ad2b340b1df7136f6984d5e428ad37e8ee6851a90d4ff9193e9d821fc8a","sha256:86b0d474f5c7098c9600ad06db29b141a1e158b9f45d4a893e0d16af059ad92d"],"state_sha256":"553598cded248e45e543e6dc5bbd72fd94247c8d0c1a057a0cbfd2b686d133ac"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Qb9X1++nJd+7wBYUzVoSuUwINdFLO1M1gP41Ub7Im5JKEubmx4fK5H07VxmTRRr8xv846FhXI+cvpB1pX9+xBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T14:30:31.255390Z","bundle_sha256":"7db4466d1df891c830560a02c605069c37cceb813e18c869b26ab1f8f5a4be7c"}}