{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:HUSPD2Y6QA53FYGD3IOQYWPM3I","short_pith_number":"pith:HUSPD2Y6","schema_version":"1.0","canonical_sha256":"3d24f1eb1e803bb2e0c3da1d0c59ecda01fc73b24cdc9b63a9488a20bf1bed2a","source":{"kind":"arxiv","id":"2504.15426","version":1},"attestation_state":"computed","paper":{"title":"Helicons in multi-Weyl semimetals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.str-el","authors_text":"Amit Gupta, Shiv Kumar Ram","submitted_at":"2025-04-21T20:35:51Z","abstract_excerpt":"Helicons are transverse electromagnetic modes in three dimension(3D) electron systems in the presence of a static magnetic field. This modes have been proposed in isotropic or single Weyl semimetals(sWSMs) (Francesco M.D. Pellegrino et al, Phys. Rev. B 92, 201407(R) (2015)). In this work, we extend our study to investigate helicons modes in gapless multi-Weyl semimetals(mWSMs) within semiclassical Boltzmann approach and discuss the differences that arise compared to single Weyl semimetals."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2504.15426","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-04-21T20:35:51Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"e479ffea74f7cb735b66c371ce2daf5da82a1ee3ae03e02cf580436c1725f09b","abstract_canon_sha256":"33fc64839ba326aef214ec601586d1084d29428b8759391795c93742cda663a6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:52:24.430879Z","signature_b64":"gx9CsX3MHhiyjSb+8PNsDlHSVmdM78PyiZlA3KEMTQzhp674AqVpFnVUo9ON637L4MWGHmD7YZmWQEggANrEDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3d24f1eb1e803bb2e0c3da1d0c59ecda01fc73b24cdc9b63a9488a20bf1bed2a","last_reissued_at":"2026-07-05T10:52:24.430371Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:52:24.430371Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Helicons in multi-Weyl semimetals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.str-el","authors_text":"Amit Gupta, Shiv Kumar Ram","submitted_at":"2025-04-21T20:35:51Z","abstract_excerpt":"Helicons are transverse electromagnetic modes in three dimension(3D) electron systems in the presence of a static magnetic field. This modes have been proposed in isotropic or single Weyl semimetals(sWSMs) (Francesco M.D. Pellegrino et al, Phys. Rev. B 92, 201407(R) (2015)). In this work, we extend our study to investigate helicons modes in gapless multi-Weyl semimetals(mWSMs) within semiclassical Boltzmann approach and discuss the differences that arise compared to single Weyl semimetals."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.15426","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/2504.15426/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2504.15426","created_at":"2026-07-05T10:52:24.430434+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.15426v1","created_at":"2026-07-05T10:52:24.430434+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.15426","created_at":"2026-07-05T10:52:24.430434+00:00"},{"alias_kind":"pith_short_12","alias_value":"HUSPD2Y6QA53","created_at":"2026-07-05T10:52:24.430434+00:00"},{"alias_kind":"pith_short_16","alias_value":"HUSPD2Y6QA53FYGD","created_at":"2026-07-05T10:52:24.430434+00:00"},{"alias_kind":"pith_short_8","alias_value":"HUSPD2Y6","created_at":"2026-07-05T10:52:24.430434+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I","json":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I.json","graph_json":"https://pith.science/api/pith-number/HUSPD2Y6QA53FYGD3IOQYWPM3I/graph.json","events_json":"https://pith.science/api/pith-number/HUSPD2Y6QA53FYGD3IOQYWPM3I/events.json","paper":"https://pith.science/paper/HUSPD2Y6"},"agent_actions":{"view_html":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I","download_json":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I.json","view_paper":"https://pith.science/paper/HUSPD2Y6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.15426&json=true","fetch_graph":"https://pith.science/api/pith-number/HUSPD2Y6QA53FYGD3IOQYWPM3I/graph.json","fetch_events":"https://pith.science/api/pith-number/HUSPD2Y6QA53FYGD3IOQYWPM3I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I/action/storage_attestation","attest_author":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I/action/author_attestation","sign_citation":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I/action/citation_signature","submit_replication":"https://pith.science/pith/HUSPD2Y6QA53FYGD3IOQYWPM3I/action/replication_record"}},"created_at":"2026-07-05T10:52:24.430434+00:00","updated_at":"2026-07-05T10:52:24.430434+00:00"}