{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:HWLCBEH7NSEBZFW4HLEWDK7IVH","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":"dcaa887749ac93b3af1f04732ff1f52e67615fca797a545492f22bd12b05bf58","cross_cats_sorted":["nlin.PS"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2021-12-14T03:22:01Z","title_canon_sha256":"d9dab82d30b218989ff6f90bf0360809d5d00d8c325da47b4be93e54860396f3"},"schema_version":"1.0","source":{"id":"2112.07136","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2112.07136","created_at":"2026-07-05T05:53:47Z"},{"alias_kind":"arxiv_version","alias_value":"2112.07136v2","created_at":"2026-07-05T05:53:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2112.07136","created_at":"2026-07-05T05:53:47Z"},{"alias_kind":"pith_short_12","alias_value":"HWLCBEH7NSEB","created_at":"2026-07-05T05:53:47Z"},{"alias_kind":"pith_short_16","alias_value":"HWLCBEH7NSEBZFW4","created_at":"2026-07-05T05:53:47Z"},{"alias_kind":"pith_short_8","alias_value":"HWLCBEH7","created_at":"2026-07-05T05:53:47Z"}],"graph_snapshots":[{"event_id":"sha256:c8e3529e750ac5e2b725c8ef9bee2bf713a2ca310751b869e225e4cba7db8455","target":"graph","created_at":"2026-07-05T05:53:47Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2112.07136/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Multi-soliton mode-locked laser waveforms are much sought as a complex light source for research and applications, but are difficult to manipulate effectively because of the elaborate and diverse interactions present. Here we present an experimental, numerical, and theoretical study of the interaction and control of the internal dynamics of a two-soliton waveform in a mode-locked fiber laser. Using the pumping current as a control agent, we demonstrate experimentally a two-orders-of-magnitude reduction in the separation of a bound soliton pair, inducing a dynamical transition between a loosely","authors_text":"Kfir Sulimany, Offek Tziperman, Omri Gat, Yaron Bromberg","cross_cats":["nlin.PS"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2021-12-14T03:22:01Z","title":"Soliton-pair dynamical transition in mode-locked lasers"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2112.07136","kind":"arxiv","version":2},"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:bd66e0246b6d147591f5c6720b4f0822a8f56fd44dc70bbe8011c3decfa18f24","target":"record","created_at":"2026-07-05T05:53:47Z","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":"dcaa887749ac93b3af1f04732ff1f52e67615fca797a545492f22bd12b05bf58","cross_cats_sorted":["nlin.PS"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2021-12-14T03:22:01Z","title_canon_sha256":"d9dab82d30b218989ff6f90bf0360809d5d00d8c325da47b4be93e54860396f3"},"schema_version":"1.0","source":{"id":"2112.07136","kind":"arxiv","version":2}},"canonical_sha256":"3d962090ff6c881c96dc3ac961abe8a9cf75bf7ad2cd45da40bd64855cc68a43","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3d962090ff6c881c96dc3ac961abe8a9cf75bf7ad2cd45da40bd64855cc68a43","first_computed_at":"2026-07-05T05:53:47.161744Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:53:47.161744Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ku/5YR1hBetaeTw9PJfS5d9BwF+8DhAJcwR9u02ENRSexLhds0LALjmLnyhD1ujQoMpyCACq+q91OCQkaxuwDw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:53:47.162129Z","signed_message":"canonical_sha256_bytes"},"source_id":"2112.07136","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bd66e0246b6d147591f5c6720b4f0822a8f56fd44dc70bbe8011c3decfa18f24","sha256:c8e3529e750ac5e2b725c8ef9bee2bf713a2ca310751b869e225e4cba7db8455"],"state_sha256":"e87010d81c70dff1054c99963d653cef708f4fcd20ec3b5e2b94050762e688e3"}