{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:56A2YHTPG6ZVJ7OIMHVMNW4OOJ","short_pith_number":"pith:56A2YHTP","canonical_record":{"source":{"id":"1307.4314","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2013-07-16T15:53:58Z","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph","physics.optics"],"title_canon_sha256":"a03392d045d081ba31b655c09119e8e55753188853417617fe0929048b96000f","abstract_canon_sha256":"df702ab18aa426df92edf3c7a3bc7175234635ccfdf3ff63e5f284a28c471109"},"schema_version":"1.0"},"canonical_sha256":"ef81ac1e6f37b354fdc861eac6db8e727f6f80e86891bff2ff8340d05a03ca81","source":{"kind":"arxiv","id":"1307.4314","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.4314","created_at":"2026-05-18T03:11:57Z"},{"alias_kind":"arxiv_version","alias_value":"1307.4314v1","created_at":"2026-05-18T03:11:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.4314","created_at":"2026-05-18T03:11:57Z"},{"alias_kind":"pith_short_12","alias_value":"56A2YHTPG6ZV","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"56A2YHTPG6ZVJ7OI","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"56A2YHTP","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:56A2YHTPG6ZVJ7OIMHVMNW4OOJ","target":"record","payload":{"canonical_record":{"source":{"id":"1307.4314","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2013-07-16T15:53:58Z","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph","physics.optics"],"title_canon_sha256":"a03392d045d081ba31b655c09119e8e55753188853417617fe0929048b96000f","abstract_canon_sha256":"df702ab18aa426df92edf3c7a3bc7175234635ccfdf3ff63e5f284a28c471109"},"schema_version":"1.0"},"canonical_sha256":"ef81ac1e6f37b354fdc861eac6db8e727f6f80e86891bff2ff8340d05a03ca81","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:11:57.200580Z","signature_b64":"hSMIjezGVXBmFuGC5tsQcNOwquJ8Fcqbb5tOmBrSgdlGBsy0kjWFj8keUQqwNSgkilMyr0EpQm2TVaoHe5cOCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef81ac1e6f37b354fdc861eac6db8e727f6f80e86891bff2ff8340d05a03ca81","last_reissued_at":"2026-05-18T03:11:57.199795Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:11:57.199795Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1307.4314","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":"2026-05-18T03:11:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"w1oth3+yIfA/Rp2pMgP2DN+TegMcFy0fp6/BnbTPFTpbXHG+HZAjLRl/ABrvskc6ld6fdUje51dthGqJoGWKBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T13:21:51.592617Z"},"content_sha256":"2d873f9e7f6756f8bcd5731d6f08c75212819dc15b57a9cae5a3095cc78a5988","schema_version":"1.0","event_id":"sha256:2d873f9e7f6756f8bcd5731d6f08c75212819dc15b57a9cae5a3095cc78a5988"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:56A2YHTPG6ZVJ7OIMHVMNW4OOJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical generation of interwoven soliton trains by nonlinear emission in binary Bose-Einstein condensates","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.atom-ph","physics.optics"],"primary_cat":"nlin.PS","authors_text":"Chandroth P. Jisha, David Novoa, V.A. Brazhnyi","submitted_at":"2013-07-16T15:53:58Z","abstract_excerpt":"We propose a method for the generation of trains of alternating bright solitons in two-component Bose-Einstein condensates, using controlled emission of nonlinear matter-waves in the uncoupled regime with spatially-varying intra-species interaction and out-of-phase oscillations of the ground states in the trap. Under this scheme, solitons are sequentially launched from the different components, and interact with each other through phase-independent cross-coupling. We obtain an analytical estimation of the critical condition for soliton emission using a geometric guiding model, in analogy with "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.4314","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":"2026-05-18T03:11:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vs5oxzgmvHZnX7EayUL3m6tnzRUKtkRVQDPiKC777SF72S++WCgGy6J/LRvAG3trgxKzBSCsqB2ODXdw5irpAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T13:21:51.592966Z"},"content_sha256":"38cb5e530e7904c3e92ae259fb667c941f0fa1978671dbeb064e9647196e8378","schema_version":"1.0","event_id":"sha256:38cb5e530e7904c3e92ae259fb667c941f0fa1978671dbeb064e9647196e8378"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ/bundle.json","state_url":"https://pith.science/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ/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":"2026-06-26T13:21:51Z","links":{"resolver":"https://pith.science/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ","bundle":"https://pith.science/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ/bundle.json","state":"https://pith.science/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/56A2YHTPG6ZVJ7OIMHVMNW4OOJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:56A2YHTPG6ZVJ7OIMHVMNW4OOJ","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":"df702ab18aa426df92edf3c7a3bc7175234635ccfdf3ff63e5f284a28c471109","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2013-07-16T15:53:58Z","title_canon_sha256":"a03392d045d081ba31b655c09119e8e55753188853417617fe0929048b96000f"},"schema_version":"1.0","source":{"id":"1307.4314","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1307.4314","created_at":"2026-05-18T03:11:57Z"},{"alias_kind":"arxiv_version","alias_value":"1307.4314v1","created_at":"2026-05-18T03:11:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1307.4314","created_at":"2026-05-18T03:11:57Z"},{"alias_kind":"pith_short_12","alias_value":"56A2YHTPG6ZV","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"56A2YHTPG6ZVJ7OI","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"56A2YHTP","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:38cb5e530e7904c3e92ae259fb667c941f0fa1978671dbeb064e9647196e8378","target":"graph","created_at":"2026-05-18T03:11:57Z","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":"We propose a method for the generation of trains of alternating bright solitons in two-component Bose-Einstein condensates, using controlled emission of nonlinear matter-waves in the uncoupled regime with spatially-varying intra-species interaction and out-of-phase oscillations of the ground states in the trap. Under this scheme, solitons are sequentially launched from the different components, and interact with each other through phase-independent cross-coupling. We obtain an analytical estimation of the critical condition for soliton emission using a geometric guiding model, in analogy with ","authors_text":"Chandroth P. Jisha, David Novoa, V.A. Brazhnyi","cross_cats":["cond-mat.quant-gas","physics.atom-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2013-07-16T15:53:58Z","title":"Dynamical generation of interwoven soliton trains by nonlinear emission in binary Bose-Einstein condensates"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1307.4314","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":"sha256:2d873f9e7f6756f8bcd5731d6f08c75212819dc15b57a9cae5a3095cc78a5988","target":"record","created_at":"2026-05-18T03:11:57Z","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":"df702ab18aa426df92edf3c7a3bc7175234635ccfdf3ff63e5f284a28c471109","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2013-07-16T15:53:58Z","title_canon_sha256":"a03392d045d081ba31b655c09119e8e55753188853417617fe0929048b96000f"},"schema_version":"1.0","source":{"id":"1307.4314","kind":"arxiv","version":1}},"canonical_sha256":"ef81ac1e6f37b354fdc861eac6db8e727f6f80e86891bff2ff8340d05a03ca81","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ef81ac1e6f37b354fdc861eac6db8e727f6f80e86891bff2ff8340d05a03ca81","first_computed_at":"2026-05-18T03:11:57.199795Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:11:57.199795Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hSMIjezGVXBmFuGC5tsQcNOwquJ8Fcqbb5tOmBrSgdlGBsy0kjWFj8keUQqwNSgkilMyr0EpQm2TVaoHe5cOCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:11:57.200580Z","signed_message":"canonical_sha256_bytes"},"source_id":"1307.4314","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2d873f9e7f6756f8bcd5731d6f08c75212819dc15b57a9cae5a3095cc78a5988","sha256:38cb5e530e7904c3e92ae259fb667c941f0fa1978671dbeb064e9647196e8378"],"state_sha256":"866defdd44c526be7b1ec110b7670fbd52be2de20c0fe4fe661cb2319df9d534"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pZ9TozojjyjjDvDcIguY1oQu7EKoO6/V7fLdKipqln7DIGixyEMqeX6oZlEbFMEAPsOVrTZq/GyH0o06FEMEAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T13:21:51.594984Z","bundle_sha256":"ea754503c9dcaf6103c7f74c15121e4090bc2dda40a32310d6d203209b278354"}}