{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:SJUTDRCCK6FODVQVH44ZNVI4JL","short_pith_number":"pith:SJUTDRCC","canonical_record":{"source":{"id":"2605.24720","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-23T20:15:32Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"55ec662ee4bca8cdfe5d205b593f93c7f27010597cd55b9036c95e42943414db","abstract_canon_sha256":"f0fb5bc59ca76953e0f6aa3bd6ef08723547344bea29b402805b8e1d5f95c010"},"schema_version":"1.0"},"canonical_sha256":"926931c442578ae1d6153f3996d51c4ac8356221b874de8332e2663bd6014a5e","source":{"kind":"arxiv","id":"2605.24720","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.24720","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"arxiv_version","alias_value":"2605.24720v1","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.24720","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"pith_short_12","alias_value":"SJUTDRCCK6FO","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"pith_short_16","alias_value":"SJUTDRCCK6FODVQV","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"pith_short_8","alias_value":"SJUTDRCC","created_at":"2026-05-26T01:03:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:SJUTDRCCK6FODVQVH44ZNVI4JL","target":"record","payload":{"canonical_record":{"source":{"id":"2605.24720","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-23T20:15:32Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"55ec662ee4bca8cdfe5d205b593f93c7f27010597cd55b9036c95e42943414db","abstract_canon_sha256":"f0fb5bc59ca76953e0f6aa3bd6ef08723547344bea29b402805b8e1d5f95c010"},"schema_version":"1.0"},"canonical_sha256":"926931c442578ae1d6153f3996d51c4ac8356221b874de8332e2663bd6014a5e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-26T01:03:55.064522Z","signature_b64":"UcwNRf/uvYkogqSO2O1k1dLcIsJa9R7lcYODmEmzb84ty7GU5Ks6C9GZ6DD1lPTuOFnDUMD83bUJPdEVGSkhCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"926931c442578ae1d6153f3996d51c4ac8356221b874de8332e2663bd6014a5e","last_reissued_at":"2026-05-26T01:03:55.063983Z","signature_status":"signed_v1","first_computed_at":"2026-05-26T01:03:55.063983Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.24720","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":"2026-05-26T01:03:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KdVDR6HZw1tQHiNEb3uQaRoeXN+PvvaP6VCi6Sitol8itI+0gglqMAejCXW+Xkf+rOsxSg5mF5f6nYPlKFdQDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T06:13:41.572172Z"},"content_sha256":"967dc8478f9bc0de99a14c3a076adf6a3dd6f85816667814f17a056664a86802","schema_version":"1.0","event_id":"sha256:967dc8478f9bc0de99a14c3a076adf6a3dd6f85816667814f17a056664a86802"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:SJUTDRCCK6FODVQVH44ZNVI4JL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Printing: Laguerre-Gaussian Beam Induced Topological Magnetic Textures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexander V. Balatsky, Tien-Tien Yeh, Yuefei Liu","submitted_at":"2026-05-23T20:15:32Z","abstract_excerpt":"Structured light has become a practical tool for controlling matter by applying tailored, space- and time-dependent electromagnetic fields. We show that Laguerre-Gaussian pulses imprint non-collinear magnetic textures via the spatial structure of optical magnetic field. Our route offers a direct spatial selectivity determined by the optical features without relying on material anisotropic interactions. The proposed printing approach does not require interfacial anisotropy or bulk chirality, current-driven torques, or thermal quenching. We use micromagnetic simulations to demonstrate the potent"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.24720","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.24720/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-05-26T01:03:55Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vcAd6Nold7mKaigxpiOhdtd0t2/9BNXGGOWLHJp4JaPiOTpBGBW7R5Pz56kSLsZSztTRQdfvVUphKCpKY/inBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T06:13:41.572694Z"},"content_sha256":"5778c816d1192e7689d6ad6c8338087fde44fadfa61108ab5f7762abfe7330d7","schema_version":"1.0","event_id":"sha256:5778c816d1192e7689d6ad6c8338087fde44fadfa61108ab5f7762abfe7330d7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SJUTDRCCK6FODVQVH44ZNVI4JL/bundle.json","state_url":"https://pith.science/pith/SJUTDRCCK6FODVQVH44ZNVI4JL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SJUTDRCCK6FODVQVH44ZNVI4JL/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":"2026-08-07T06:13:41Z","links":{"resolver":"https://pith.science/pith/SJUTDRCCK6FODVQVH44ZNVI4JL","bundle":"https://pith.science/pith/SJUTDRCCK6FODVQVH44ZNVI4JL/bundle.json","state":"https://pith.science/pith/SJUTDRCCK6FODVQVH44ZNVI4JL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SJUTDRCCK6FODVQVH44ZNVI4JL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:SJUTDRCCK6FODVQVH44ZNVI4JL","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":"f0fb5bc59ca76953e0f6aa3bd6ef08723547344bea29b402805b8e1d5f95c010","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-23T20:15:32Z","title_canon_sha256":"55ec662ee4bca8cdfe5d205b593f93c7f27010597cd55b9036c95e42943414db"},"schema_version":"1.0","source":{"id":"2605.24720","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.24720","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"arxiv_version","alias_value":"2605.24720v1","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.24720","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"pith_short_12","alias_value":"SJUTDRCCK6FO","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"pith_short_16","alias_value":"SJUTDRCCK6FODVQV","created_at":"2026-05-26T01:03:55Z"},{"alias_kind":"pith_short_8","alias_value":"SJUTDRCC","created_at":"2026-05-26T01:03:55Z"}],"graph_snapshots":[{"event_id":"sha256:5778c816d1192e7689d6ad6c8338087fde44fadfa61108ab5f7762abfe7330d7","target":"graph","created_at":"2026-05-26T01:03:55Z","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/2605.24720/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Structured light has become a practical tool for controlling matter by applying tailored, space- and time-dependent electromagnetic fields. We show that Laguerre-Gaussian pulses imprint non-collinear magnetic textures via the spatial structure of optical magnetic field. Our route offers a direct spatial selectivity determined by the optical features without relying on material anisotropic interactions. The proposed printing approach does not require interfacial anisotropy or bulk chirality, current-driven torques, or thermal quenching. We use micromagnetic simulations to demonstrate the potent","authors_text":"Alexander V. Balatsky, Tien-Tien Yeh, Yuefei Liu","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-23T20:15:32Z","title":"Quantum Printing: Laguerre-Gaussian Beam Induced Topological Magnetic Textures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2605.24720","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":"sha256:967dc8478f9bc0de99a14c3a076adf6a3dd6f85816667814f17a056664a86802","target":"record","created_at":"2026-05-26T01:03:55Z","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":"f0fb5bc59ca76953e0f6aa3bd6ef08723547344bea29b402805b8e1d5f95c010","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-05-23T20:15:32Z","title_canon_sha256":"55ec662ee4bca8cdfe5d205b593f93c7f27010597cd55b9036c95e42943414db"},"schema_version":"1.0","source":{"id":"2605.24720","kind":"arxiv","version":1}},"canonical_sha256":"926931c442578ae1d6153f3996d51c4ac8356221b874de8332e2663bd6014a5e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"926931c442578ae1d6153f3996d51c4ac8356221b874de8332e2663bd6014a5e","first_computed_at":"2026-05-26T01:03:55.063983Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-26T01:03:55.063983Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UcwNRf/uvYkogqSO2O1k1dLcIsJa9R7lcYODmEmzb84ty7GU5Ks6C9GZ6DD1lPTuOFnDUMD83bUJPdEVGSkhCQ==","signature_status":"signed_v1","signed_at":"2026-05-26T01:03:55.064522Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.24720","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:967dc8478f9bc0de99a14c3a076adf6a3dd6f85816667814f17a056664a86802","sha256:5778c816d1192e7689d6ad6c8338087fde44fadfa61108ab5f7762abfe7330d7"],"state_sha256":"55bfe298d1cc34a2ed73fc66677ba1671edc161826398bc62595dd7bf3f1f38f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5/z07v0da7MSPUvU4z34wP1JC1RtshOw/pnGxkK6dGmzzDYRzohUDlawUlYJaYkTgyK6EllWtkxSG6dSg5qlBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T06:13:41.578253Z","bundle_sha256":"3e05558a0426fb2d30169a92bc5496c9461d441847304e3131ddeff3ebb4cdd5"}}