{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:6HAV7JUJMEELEPO253Y6YCVQXE","short_pith_number":"pith:6HAV7JUJ","canonical_record":{"source":{"id":"1412.6611","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2014-12-20T05:51:02Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"db86b9b6e2325e1fc914f8d0727304e7c27b1bcf3ff81d90750d41acece5b17b","abstract_canon_sha256":"a8585744a2eea1499b8096e6c04dc33b6ef2d23340f6bb1a47edb8fc96ae7799"},"schema_version":"1.0"},"canonical_sha256":"f1c15fa6896108b23ddaeef1ec0ab0b9103e19b04eeb5665d849badd452f00cc","source":{"kind":"arxiv","id":"1412.6611","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.6611","created_at":"2026-05-18T01:41:16Z"},{"alias_kind":"arxiv_version","alias_value":"1412.6611v1","created_at":"2026-05-18T01:41:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.6611","created_at":"2026-05-18T01:41:16Z"},{"alias_kind":"pith_short_12","alias_value":"6HAV7JUJMEEL","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6HAV7JUJMEELEPO2","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6HAV7JUJ","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:6HAV7JUJMEELEPO253Y6YCVQXE","target":"record","payload":{"canonical_record":{"source":{"id":"1412.6611","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2014-12-20T05:51:02Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"title_canon_sha256":"db86b9b6e2325e1fc914f8d0727304e7c27b1bcf3ff81d90750d41acece5b17b","abstract_canon_sha256":"a8585744a2eea1499b8096e6c04dc33b6ef2d23340f6bb1a47edb8fc96ae7799"},"schema_version":"1.0"},"canonical_sha256":"f1c15fa6896108b23ddaeef1ec0ab0b9103e19b04eeb5665d849badd452f00cc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:16.325407Z","signature_b64":"69oI4dTWZ/csDSetEKx20crM255AHM303+F10YeMFcEQ/2hv2qFO9H8H3eqTvvpAt9X7eWH3bX8vAEZtH1WGBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f1c15fa6896108b23ddaeef1ec0ab0b9103e19b04eeb5665d849badd452f00cc","last_reissued_at":"2026-05-18T01:41:16.324941Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:16.324941Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.6611","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":"2026-05-18T01:41:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Khiidl4YiFT39rDktqAF29g5aWc0TIQqC77s7PExSKD76h3h8nDBUBk0FUl+Wc2gDAsfMcl98M+h+CLPjnoRDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T19:27:06.015332Z"},"content_sha256":"2ffeb804bef4147909077d1c171ec35ada2b87f66105d91e93f2a70bdd022578","schema_version":"1.0","event_id":"sha256:2ffeb804bef4147909077d1c171ec35ada2b87f66105d91e93f2a70bdd022578"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:6HAV7JUJMEELEPO253Y6YCVQXE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamics of impurity attraction and repulsion of an intrinsic localized mode in a driven 1-D cantilever array","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics"],"primary_cat":"nlin.PS","authors_text":"A. J. Sievers, B. E. Hubbard, B. Ilic, M. Sato, S. Shige, T. Ishikawa, W. Shi, Y. Sada, Y. Soga","submitted_at":"2014-12-20T05:51:02Z","abstract_excerpt":"Both low frequency and high frequency impurity modes have been produced in a SiN micromechanical cantilever array by illumination with either an infrared or visible laser. When such laser-induced impurities are placed near a driven intrinsic localized mode (ILM) it is either repelled or attracted. By measuring the linear response spectrum for these two cases it was found that vibrational hopping of the ILM takes place when the natural frequency of the ILM and an even symmetry linear local mode are symmetrically located about the driven ILM frequency so that parametric excitation of these two l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.6611","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":"2026-05-18T01:41:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gIu23MWigCTMLsfprwOPBNom2Kfum74sQP6nfQkf5DdpVhMreEmZNITYfUrcP/wXT1C40+izrYr1lKKBepWuDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T19:27:06.015687Z"},"content_sha256":"f494c524bdc71159801935720d7fd514c3556958f1f1d231de20d54b6f4d0f91","schema_version":"1.0","event_id":"sha256:f494c524bdc71159801935720d7fd514c3556958f1f1d231de20d54b6f4d0f91"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6HAV7JUJMEELEPO253Y6YCVQXE/bundle.json","state_url":"https://pith.science/pith/6HAV7JUJMEELEPO253Y6YCVQXE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6HAV7JUJMEELEPO253Y6YCVQXE/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":"2026-06-02T19:27:06Z","links":{"resolver":"https://pith.science/pith/6HAV7JUJMEELEPO253Y6YCVQXE","bundle":"https://pith.science/pith/6HAV7JUJMEELEPO253Y6YCVQXE/bundle.json","state":"https://pith.science/pith/6HAV7JUJMEELEPO253Y6YCVQXE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6HAV7JUJMEELEPO253Y6YCVQXE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:6HAV7JUJMEELEPO253Y6YCVQXE","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":"a8585744a2eea1499b8096e6c04dc33b6ef2d23340f6bb1a47edb8fc96ae7799","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2014-12-20T05:51:02Z","title_canon_sha256":"db86b9b6e2325e1fc914f8d0727304e7c27b1bcf3ff81d90750d41acece5b17b"},"schema_version":"1.0","source":{"id":"1412.6611","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.6611","created_at":"2026-05-18T01:41:16Z"},{"alias_kind":"arxiv_version","alias_value":"1412.6611v1","created_at":"2026-05-18T01:41:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.6611","created_at":"2026-05-18T01:41:16Z"},{"alias_kind":"pith_short_12","alias_value":"6HAV7JUJMEEL","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"6HAV7JUJMEELEPO2","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"6HAV7JUJ","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:f494c524bdc71159801935720d7fd514c3556958f1f1d231de20d54b6f4d0f91","target":"graph","created_at":"2026-05-18T01:41:16Z","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":"Both low frequency and high frequency impurity modes have been produced in a SiN micromechanical cantilever array by illumination with either an infrared or visible laser. When such laser-induced impurities are placed near a driven intrinsic localized mode (ILM) it is either repelled or attracted. By measuring the linear response spectrum for these two cases it was found that vibrational hopping of the ILM takes place when the natural frequency of the ILM and an even symmetry linear local mode are symmetrically located about the driven ILM frequency so that parametric excitation of these two l","authors_text":"A. J. Sievers, B. E. Hubbard, B. Ilic, M. Sato, S. Shige, T. Ishikawa, W. Shi, Y. Sada, Y. Soga","cross_cats":["cond-mat.mes-hall","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2014-12-20T05:51:02Z","title":"Dynamics of impurity attraction and repulsion of an intrinsic localized mode in a driven 1-D cantilever array"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.6611","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":"sha256:2ffeb804bef4147909077d1c171ec35ada2b87f66105d91e93f2a70bdd022578","target":"record","created_at":"2026-05-18T01:41:16Z","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":"a8585744a2eea1499b8096e6c04dc33b6ef2d23340f6bb1a47edb8fc96ae7799","cross_cats_sorted":["cond-mat.mes-hall","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.PS","submitted_at":"2014-12-20T05:51:02Z","title_canon_sha256":"db86b9b6e2325e1fc914f8d0727304e7c27b1bcf3ff81d90750d41acece5b17b"},"schema_version":"1.0","source":{"id":"1412.6611","kind":"arxiv","version":1}},"canonical_sha256":"f1c15fa6896108b23ddaeef1ec0ab0b9103e19b04eeb5665d849badd452f00cc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f1c15fa6896108b23ddaeef1ec0ab0b9103e19b04eeb5665d849badd452f00cc","first_computed_at":"2026-05-18T01:41:16.324941Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:41:16.324941Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"69oI4dTWZ/csDSetEKx20crM255AHM303+F10YeMFcEQ/2hv2qFO9H8H3eqTvvpAt9X7eWH3bX8vAEZtH1WGBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:41:16.325407Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.6611","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2ffeb804bef4147909077d1c171ec35ada2b87f66105d91e93f2a70bdd022578","sha256:f494c524bdc71159801935720d7fd514c3556958f1f1d231de20d54b6f4d0f91"],"state_sha256":"50200b776b4dc809740914dc804f20d87889d46c4191486282adcad8606fcfb8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z94q9yzEr+hsTk1Rtm8sHoGxTtxPkQyVQE+ZKnGE26xGJG+Cp5lXJ6Dz3pJrhTOQLGAM/pJLIUgcGeluUvgPDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T19:27:06.017656Z","bundle_sha256":"183463f9c2d3efa4ac26540794e54b2c9318c9b0e06c16e15f6a1fcf66008c55"}}