{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6ASLBPENMKTE4ZWNIHOJBIZZIT","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":"decd0764213e0a492925ae94a2b10018cf767eb1fd7d1ac55986942751aadc36","cross_cats_sorted":["nlin.PS","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-29T13:04:29Z","title_canon_sha256":"97cb5e6133d037ce1bac4fb323f1a6ef9c1848eb12a6cb9ff87c1470b4768acf"},"schema_version":"1.0","source":{"id":"1407.7713","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1407.7713","created_at":"2026-05-18T01:24:11Z"},{"alias_kind":"arxiv_version","alias_value":"1407.7713v1","created_at":"2026-05-18T01:24:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.7713","created_at":"2026-05-18T01:24:11Z"},{"alias_kind":"pith_short_12","alias_value":"6ASLBPENMKTE","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6ASLBPENMKTE4ZWN","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6ASLBPEN","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:140f6e9246739337c9f799c2c3b32ae582f0cfb5f44239e0dd0e62d939b93d23","target":"graph","created_at":"2026-05-18T01:24:11Z","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":"Semiconductor microcavities operating in the polaritonic regime are highly non-linear, high speed systems due to the unique half-light, half-matter nature of polaritons. Here, we report for the first time the observation of propagating multi-soliton polariton patterns consisting of multi-peak structures either along (x) or perpendicular to (y) the direction of propagation. Soliton arrays of up to 5 solitons are observed, with the number of solitons controlled by the size or power of the triggering laser pulse. The break-up along the x direction occurs due to interplay of bistability, negative ","authors_text":"A. V. Gorbach, D. N. Krizhanovskii, D. V. Skryabin, E. A. Cerda-M\\'endez, E. Cancellieri, F. Fras, J. K. Chana, K. Biermann, M. Sich, M. S. Skolnick, P. V. Santos, R. Hey","cross_cats":["nlin.PS","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-29T13:04:29Z","title":"Spatial patterns of dissipative polariton solitons in semiconductor microcavities"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.7713","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:d6435a124d5d094da2dcde20e7d6e1a7b5011923e165f1a52e7110624d7db584","target":"record","created_at":"2026-05-18T01:24:11Z","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":"decd0764213e0a492925ae94a2b10018cf767eb1fd7d1ac55986942751aadc36","cross_cats_sorted":["nlin.PS","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-07-29T13:04:29Z","title_canon_sha256":"97cb5e6133d037ce1bac4fb323f1a6ef9c1848eb12a6cb9ff87c1470b4768acf"},"schema_version":"1.0","source":{"id":"1407.7713","kind":"arxiv","version":1}},"canonical_sha256":"f024b0bc8d62a64e66cd41dc90a33944e6605fd283858222ed1ffa2220d6b379","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f024b0bc8d62a64e66cd41dc90a33944e6605fd283858222ed1ffa2220d6b379","first_computed_at":"2026-05-18T01:24:11.174465Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:24:11.174465Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aeTdfjxn91aL/bc78eZF9b0czfofvuTHZ93WXfoAn8w4FfoowhHEFmehz3ZrxoIrz0XQYWYWDpAeaNN9vU+8Cw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:24:11.174898Z","signed_message":"canonical_sha256_bytes"},"source_id":"1407.7713","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d6435a124d5d094da2dcde20e7d6e1a7b5011923e165f1a52e7110624d7db584","sha256:140f6e9246739337c9f799c2c3b32ae582f0cfb5f44239e0dd0e62d939b93d23"],"state_sha256":"c0d9a03ccc0aaf58b3d20f8014d7a8987978c27162ab1d5fac2a026a9fc95bb7"}