{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:XKFTE22QVGLBWBWAIAMMXQ5UZI","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":"0742a2b9c7072dfdfe0ef22cfc4edb491bc77470a016157fb88a48206558e367","cross_cats_sorted":["cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2025-06-18T17:39:04Z","title_canon_sha256":"52fee3b01b9f3967845dadefaf1779b012a2ecbdd6d5d2438fc912cb7ff7b6a4"},"schema_version":"1.0","source":{"id":"2506.15661","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.15661","created_at":"2026-05-20T00:05:30Z"},{"alias_kind":"arxiv_version","alias_value":"2506.15661v3","created_at":"2026-05-20T00:05:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.15661","created_at":"2026-05-20T00:05:30Z"},{"alias_kind":"pith_short_12","alias_value":"XKFTE22QVGLB","created_at":"2026-05-20T00:05:30Z"},{"alias_kind":"pith_short_16","alias_value":"XKFTE22QVGLBWBWA","created_at":"2026-05-20T00:05:30Z"},{"alias_kind":"pith_short_8","alias_value":"XKFTE22Q","created_at":"2026-05-20T00:05:30Z"}],"graph_snapshots":[{"event_id":"sha256:3646db9123028d137dc29fd77f6f84ece181bdfc033fc486dca7401219ffbc3d","target":"graph","created_at":"2026-05-20T00:05:30Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"Coupling itinerant electrons to a noncollinear classical exchange field can induce anisotropic Josephson coupling between superconducting d vectors, analogous to the Dzyaloshinskii-Moriya and Γ-type interactions in magnetism."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The perturbative treatment of the s-d model on a geometrically frustrated lattice assumes that the local spins remain classical and noncollinear without significant quantum fluctuations or back-action from the superconducting electrons."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Noncollinear classical exchange fields on geometrically frustrated lattices induce anisotropic Josephson couplings between triplet d-vectors, enabling spatial pairing textures, anomalous vortices, and a chirality-proportional Josephson diode effect."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Coupling electrons to noncollinear spins on frustrated lattices induces anisotropic Josephson coupling between triplet d-vectors."}],"snapshot_sha256":"7f95778abe3980a6f47d7a73081aaabb7d7c7fa3048162c89bb883e47b4c9008"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2506.15661/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We demonstrate that coupling itinerant electrons to a noncollinear classical exchange field can induce anisotropic Josephson coupling between superconducting $d$ vectors, analogous to the Dzyaloshinskii-Moriya and $\\Gamma$-type interactions in magnetism. Using perturbative methods, we analyze an $s$-$d$ model on a geometrically frustrated lattice. Noncollinear local spin textures generate spin triplet pairing correlations and can favor spatially varying superconducting order due to anisotropic Josephson couplings between $d$ vectors, endowing a ``pliability'' to the pairing order that competes","authors_text":"Grayson R. Frazier, Junyi Zhang, Yi Li","cross_cats":["cond-mat.str-el"],"headline":"Coupling electrons to noncollinear spins on frustrated lattices induces anisotropic Josephson coupling between triplet d-vectors.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2025-06-18T17:39:04Z","title":"Anisotropic Josephson coupling of $d$ vectors in triplet superconductors arising from frustrated spin textures"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.15661","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-19T08:49:13.385393Z","id":"1d618a5f-ba89-4410-bc89-01fbc97b598c","model_set":{"reader":"grok-4.3"},"one_line_summary":"Noncollinear classical exchange fields on geometrically frustrated lattices induce anisotropic Josephson couplings between triplet d-vectors, enabling spatial pairing textures, anomalous vortices, and a chirality-proportional Josephson diode effect.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Coupling electrons to noncollinear spins on frustrated lattices induces anisotropic Josephson coupling between triplet d-vectors.","strongest_claim":"Coupling itinerant electrons to a noncollinear classical exchange field can induce anisotropic Josephson coupling between superconducting d vectors, analogous to the Dzyaloshinskii-Moriya and Γ-type interactions in magnetism.","weakest_assumption":"The perturbative treatment of the s-d model on a geometrically frustrated lattice assumes that the local spins remain classical and noncollinear without significant quantum fluctuations or back-action from the superconducting electrons."}},"verdict_id":"1d618a5f-ba89-4410-bc89-01fbc97b598c"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:84b3b0273ba9597b5e63adcc61b1833ee9a0dbd9f4a3211ba0be5a69c1edd162","target":"record","created_at":"2026-05-20T00:05:30Z","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":"0742a2b9c7072dfdfe0ef22cfc4edb491bc77470a016157fb88a48206558e367","cross_cats_sorted":["cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2025-06-18T17:39:04Z","title_canon_sha256":"52fee3b01b9f3967845dadefaf1779b012a2ecbdd6d5d2438fc912cb7ff7b6a4"},"schema_version":"1.0","source":{"id":"2506.15661","kind":"arxiv","version":3}},"canonical_sha256":"ba8b326b50a9961b06c04018cbc3b4ca37dc00d2a788fdd03ae270e170214170","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ba8b326b50a9961b06c04018cbc3b4ca37dc00d2a788fdd03ae270e170214170","first_computed_at":"2026-05-20T00:05:30.320568Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:05:30.320568Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"FeIpyLxvQwz9KMvzNjL5MATX/i+19ABSRALXat+hYAkfrEf0v2auYizHj97Nqxl361ZOskz9glBFi30zY4OTBQ==","signature_status":"signed_v1","signed_at":"2026-05-20T00:05:30.321721Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.15661","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:84b3b0273ba9597b5e63adcc61b1833ee9a0dbd9f4a3211ba0be5a69c1edd162","sha256:3646db9123028d137dc29fd77f6f84ece181bdfc033fc486dca7401219ffbc3d"],"state_sha256":"dc5d79f1a3d1d93c143e5a3b4491e382d240eb217e7232486d1af198c569be71"}