{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:WKZYHRUW5ECBHXMNRYQGTQPMQV","short_pith_number":"pith:WKZYHRUW","schema_version":"1.0","canonical_sha256":"b2b383c696e90413dd8d8e2069c1ec8571d93e17642e020e75289162336a6370","source":{"kind":"arxiv","id":"1711.01892","version":1},"attestation_state":"computed","paper":{"title":"Application of tensor network method to two dimensional lattice $\\mathcal{N}=1$ Wess-Zumino model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Daisuke Kadoh, Ryo Sakai, Shinji Takeda, Yoshifumi Nakamura, Yoshinobu Kuramashi, Yusuke Yoshimura","submitted_at":"2017-11-06T13:53:39Z","abstract_excerpt":"We study a tensor network formulation of the two dimensional lattice $\\mathcal{N}=1$ Wess-Zumino model with Wilson derivatives for both fermions and bosons. The tensor renormalization group allows us to compute the partition function without the sign problem, and basic ideas to obtain a tensor network for both fermion and scalar boson systems were already given in previous works. In addition to improving the methods, we have constructed a tensor network representation of the model including the Yukawa-type interaction of Majorana fermions and real scalar bosons. We present some numerical resul"},"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":"1711.01892","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2017-11-06T13:53:39Z","cross_cats_sorted":[],"title_canon_sha256":"864d0179c4f2f88f8b458dd7346fe4fec68b3dc5ed0712c37bc2c597441b2d28","abstract_canon_sha256":"8be065631b61c75d43b9f40915b2a6bbcc90e7d74f62da2c55972885e347bde5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:18:15.478359Z","signature_b64":"sTcsrmGvve83H6yccXuXYKjEY/7XK2bbOKLqN6tcUerg1Cly05Mj7RHk+MSISQzuf6hGwxsraPzGPvkv5ajSCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b2b383c696e90413dd8d8e2069c1ec8571d93e17642e020e75289162336a6370","last_reissued_at":"2026-05-18T00:18:15.477758Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:18:15.477758Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Application of tensor network method to two dimensional lattice $\\mathcal{N}=1$ Wess-Zumino model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Daisuke Kadoh, Ryo Sakai, Shinji Takeda, Yoshifumi Nakamura, Yoshinobu Kuramashi, Yusuke Yoshimura","submitted_at":"2017-11-06T13:53:39Z","abstract_excerpt":"We study a tensor network formulation of the two dimensional lattice $\\mathcal{N}=1$ Wess-Zumino model with Wilson derivatives for both fermions and bosons. The tensor renormalization group allows us to compute the partition function without the sign problem, and basic ideas to obtain a tensor network for both fermion and scalar boson systems were already given in previous works. In addition to improving the methods, we have constructed a tensor network representation of the model including the Yukawa-type interaction of Majorana fermions and real scalar bosons. We present some numerical resul"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1711.01892","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1711.01892","created_at":"2026-05-18T00:18:15.477845+00:00"},{"alias_kind":"arxiv_version","alias_value":"1711.01892v1","created_at":"2026-05-18T00:18:15.477845+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1711.01892","created_at":"2026-05-18T00:18:15.477845+00:00"},{"alias_kind":"pith_short_12","alias_value":"WKZYHRUW5ECB","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_16","alias_value":"WKZYHRUW5ECBHXMN","created_at":"2026-05-18T12:31:53.515858+00:00"},{"alias_kind":"pith_short_8","alias_value":"WKZYHRUW","created_at":"2026-05-18T12:31:53.515858+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/WKZYHRUW5ECBHXMNRYQGTQPMQV","json":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV.json","graph_json":"https://pith.science/api/pith-number/WKZYHRUW5ECBHXMNRYQGTQPMQV/graph.json","events_json":"https://pith.science/api/pith-number/WKZYHRUW5ECBHXMNRYQGTQPMQV/events.json","paper":"https://pith.science/paper/WKZYHRUW"},"agent_actions":{"view_html":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV","download_json":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV.json","view_paper":"https://pith.science/paper/WKZYHRUW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1711.01892&json=true","fetch_graph":"https://pith.science/api/pith-number/WKZYHRUW5ECBHXMNRYQGTQPMQV/graph.json","fetch_events":"https://pith.science/api/pith-number/WKZYHRUW5ECBHXMNRYQGTQPMQV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV/action/storage_attestation","attest_author":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV/action/author_attestation","sign_citation":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV/action/citation_signature","submit_replication":"https://pith.science/pith/WKZYHRUW5ECBHXMNRYQGTQPMQV/action/replication_record"}},"created_at":"2026-05-18T00:18:15.477845+00:00","updated_at":"2026-05-18T00:18:15.477845+00:00"}