{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:YMCFOEOZYITA6ZHX5MIHTY6PBA","short_pith_number":"pith:YMCFOEOZ","schema_version":"1.0","canonical_sha256":"c3045711d9c2260f64f7eb1079e3cf082efcebc13d15a3853e6f5937e6abd5ba","source":{"kind":"arxiv","id":"1112.5164","version":2},"attestation_state":"computed","paper":{"title":"Asymptotic scattering and duality in the one-dimensional three-state quantum Potts model on a lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Akos Rapp, Gabor Takacs, Gergely Zarand, Peter Schmitteckert","submitted_at":"2011-12-21T21:00:02Z","abstract_excerpt":"We determine numerically the single-particle and the two-particle spectrum of the three-state quantum Potts model on a lattice by using the density matrix renormalization group method, and extract information on the asymptotic (small momentum) S-matrix of the quasiparticles. The low energy part of the finite size spectrum can be understood in terms of a simple effective model introduced in a previous work, and is consistent with an asymptotic S-matrix of an exchange form below a momentum scale $p^*$. This scale appears to vanish faster than the Compton scale, $mc$, as one approaches the critic"},"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":"1112.5164","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-12-21T21:00:02Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"1c3bc1a32305c1e7ae278cfec1be505f0786add13ba754bfe05c60c9286a83e6","abstract_canon_sha256":"1c660f7bdcfe7c782dd06d545dc228d4111373a8079e8ca3a3063ea4fe22a58e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:35:14.285253Z","signature_b64":"hN/YXw06e2kQnDAMakeDbCnT4s+ssni+Jz70MYuZ2268mGKB4efWuhYuvNniGWc7qnoLw2ZzR9qG+Zp8zW0XDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c3045711d9c2260f64f7eb1079e3cf082efcebc13d15a3853e6f5937e6abd5ba","last_reissued_at":"2026-05-18T03:35:14.284583Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:35:14.284583Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Asymptotic scattering and duality in the one-dimensional three-state quantum Potts model on a lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Akos Rapp, Gabor Takacs, Gergely Zarand, Peter Schmitteckert","submitted_at":"2011-12-21T21:00:02Z","abstract_excerpt":"We determine numerically the single-particle and the two-particle spectrum of the three-state quantum Potts model on a lattice by using the density matrix renormalization group method, and extract information on the asymptotic (small momentum) S-matrix of the quasiparticles. The low energy part of the finite size spectrum can be understood in terms of a simple effective model introduced in a previous work, and is consistent with an asymptotic S-matrix of an exchange form below a momentum scale $p^*$. This scale appears to vanish faster than the Compton scale, $mc$, as one approaches the critic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.5164","kind":"arxiv","version":2},"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":"1112.5164","created_at":"2026-05-18T03:35:14.284683+00:00"},{"alias_kind":"arxiv_version","alias_value":"1112.5164v2","created_at":"2026-05-18T03:35:14.284683+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.5164","created_at":"2026-05-18T03:35:14.284683+00:00"},{"alias_kind":"pith_short_12","alias_value":"YMCFOEOZYITA","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"YMCFOEOZYITA6ZHX","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"YMCFOEOZ","created_at":"2026-05-18T12:26:47.523578+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/YMCFOEOZYITA6ZHX5MIHTY6PBA","json":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA.json","graph_json":"https://pith.science/api/pith-number/YMCFOEOZYITA6ZHX5MIHTY6PBA/graph.json","events_json":"https://pith.science/api/pith-number/YMCFOEOZYITA6ZHX5MIHTY6PBA/events.json","paper":"https://pith.science/paper/YMCFOEOZ"},"agent_actions":{"view_html":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA","download_json":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA.json","view_paper":"https://pith.science/paper/YMCFOEOZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1112.5164&json=true","fetch_graph":"https://pith.science/api/pith-number/YMCFOEOZYITA6ZHX5MIHTY6PBA/graph.json","fetch_events":"https://pith.science/api/pith-number/YMCFOEOZYITA6ZHX5MIHTY6PBA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA/action/storage_attestation","attest_author":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA/action/author_attestation","sign_citation":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA/action/citation_signature","submit_replication":"https://pith.science/pith/YMCFOEOZYITA6ZHX5MIHTY6PBA/action/replication_record"}},"created_at":"2026-05-18T03:35:14.284683+00:00","updated_at":"2026-05-18T03:35:14.284683+00:00"}