{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:H74IQW3T436N4XMCRRZXFGFT47","short_pith_number":"pith:H74IQW3T","canonical_record":{"source":{"id":"1812.05627","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-13T19:00:03Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"7d900723362808e976fccee9bf457465eadea6250862a220ec9dea751a0e1e78","abstract_canon_sha256":"f7a37965ce34e2cdc54fcb5f2c1db85a3ee6f5cdef9a11e3c3256462fe9b60dc"},"schema_version":"1.0"},"canonical_sha256":"3ff8885b73e6fcde5d828c737298b3e7fce285b8dcd032289c862ec3533b0415","source":{"kind":"arxiv","id":"1812.05627","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.05627","created_at":"2026-05-17T23:41:36Z"},{"alias_kind":"arxiv_version","alias_value":"1812.05627v2","created_at":"2026-05-17T23:41:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.05627","created_at":"2026-05-17T23:41:36Z"},{"alias_kind":"pith_short_12","alias_value":"H74IQW3T436N","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_16","alias_value":"H74IQW3T436N4XMC","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_8","alias_value":"H74IQW3T","created_at":"2026-05-18T12:32:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:H74IQW3T436N4XMCRRZXFGFT47","target":"record","payload":{"canonical_record":{"source":{"id":"1812.05627","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-13T19:00:03Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"7d900723362808e976fccee9bf457465eadea6250862a220ec9dea751a0e1e78","abstract_canon_sha256":"f7a37965ce34e2cdc54fcb5f2c1db85a3ee6f5cdef9a11e3c3256462fe9b60dc"},"schema_version":"1.0"},"canonical_sha256":"3ff8885b73e6fcde5d828c737298b3e7fce285b8dcd032289c862ec3533b0415","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:41:36.713297Z","signature_b64":"F4orKPzYobgeozMDn8QC5JpxKaIYJjYm3JTFGzF3D6FHECxfPnS/0xmpa5N0A7H2HoX1T07l9BpvtQ203/U4Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ff8885b73e6fcde5d828c737298b3e7fce285b8dcd032289c862ec3533b0415","last_reissued_at":"2026-05-17T23:41:36.712655Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:41:36.712655Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1812.05627","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:41:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PoDYfvfg7lJ6jvCyicxI0mnWZDpF4rgR/qykiSJuEqH0CdwLdFF3K8h2btK8a9S1WL0l564mpSXICiq4MBZ1Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T10:21:42.463705Z"},"content_sha256":"0d908b61a526b2d80b931a008ed0245e6349d1d60243ab8fe490e9a64bcb404f","schema_version":"1.0","event_id":"sha256:0d908b61a526b2d80b931a008ed0245e6349d1d60243ab8fe490e9a64bcb404f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:H74IQW3T436N4XMCRRZXFGFT47","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Single-hole wave function in two dimensions: A case study of the doped Mott insulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"D. N. Sheng, Qing-Rui Wang, Shuai Chen, Yang Qi, Zheng-Yu Weng","submitted_at":"2018-12-13T19:00:03Z","abstract_excerpt":"We study a ground-state ansatz for the single-hole doped $t$-$J$ model in two dimensions via a variational Monte Carlo (VMC) method. Such a single-hole wave function possesses finite angular momenta generated by hidden spin currents, which give rise to a novel ground state degeneracy in agreement with recent exact diagonalization (ED) and density matrix renormalization group (DMGR) results. We further show that the wave function can be decomposed into a quasiparticle component and an incoherent momentum distribution in excellent agreement with the DMRG results up to an $8\\times 8 $ lattice. Su"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.05627","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-17T23:41:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZcKlOoTqsM+vPJn9CMCP5njT0FmP1asaLwd0FHyIciThRfk1/dYtU507fTZ1FE8aNjIgUJWsevecMS96UonODw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T10:21:42.464026Z"},"content_sha256":"a7509fff815d2e48602a7d958d7a0ca32cb05a499d55e0f3eda22a57b61d2d1f","schema_version":"1.0","event_id":"sha256:a7509fff815d2e48602a7d958d7a0ca32cb05a499d55e0f3eda22a57b61d2d1f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/H74IQW3T436N4XMCRRZXFGFT47/bundle.json","state_url":"https://pith.science/pith/H74IQW3T436N4XMCRRZXFGFT47/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/H74IQW3T436N4XMCRRZXFGFT47/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":"2026-06-08T10:21:42Z","links":{"resolver":"https://pith.science/pith/H74IQW3T436N4XMCRRZXFGFT47","bundle":"https://pith.science/pith/H74IQW3T436N4XMCRRZXFGFT47/bundle.json","state":"https://pith.science/pith/H74IQW3T436N4XMCRRZXFGFT47/state.json","well_known_bundle":"https://pith.science/.well-known/pith/H74IQW3T436N4XMCRRZXFGFT47/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:H74IQW3T436N4XMCRRZXFGFT47","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":"f7a37965ce34e2cdc54fcb5f2c1db85a3ee6f5cdef9a11e3c3256462fe9b60dc","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-13T19:00:03Z","title_canon_sha256":"7d900723362808e976fccee9bf457465eadea6250862a220ec9dea751a0e1e78"},"schema_version":"1.0","source":{"id":"1812.05627","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1812.05627","created_at":"2026-05-17T23:41:36Z"},{"alias_kind":"arxiv_version","alias_value":"1812.05627v2","created_at":"2026-05-17T23:41:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.05627","created_at":"2026-05-17T23:41:36Z"},{"alias_kind":"pith_short_12","alias_value":"H74IQW3T436N","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_16","alias_value":"H74IQW3T436N4XMC","created_at":"2026-05-18T12:32:28Z"},{"alias_kind":"pith_short_8","alias_value":"H74IQW3T","created_at":"2026-05-18T12:32:28Z"}],"graph_snapshots":[{"event_id":"sha256:a7509fff815d2e48602a7d958d7a0ca32cb05a499d55e0f3eda22a57b61d2d1f","target":"graph","created_at":"2026-05-17T23:41:36Z","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"},"paper":{"abstract_excerpt":"We study a ground-state ansatz for the single-hole doped $t$-$J$ model in two dimensions via a variational Monte Carlo (VMC) method. Such a single-hole wave function possesses finite angular momenta generated by hidden spin currents, which give rise to a novel ground state degeneracy in agreement with recent exact diagonalization (ED) and density matrix renormalization group (DMGR) results. We further show that the wave function can be decomposed into a quasiparticle component and an incoherent momentum distribution in excellent agreement with the DMRG results up to an $8\\times 8 $ lattice. Su","authors_text":"D. N. Sheng, Qing-Rui Wang, Shuai Chen, Yang Qi, Zheng-Yu Weng","cross_cats":["cond-mat.supr-con"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-13T19:00:03Z","title":"Single-hole wave function in two dimensions: A case study of the doped Mott insulator"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.05627","kind":"arxiv","version":2},"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":"sha256:0d908b61a526b2d80b931a008ed0245e6349d1d60243ab8fe490e9a64bcb404f","target":"record","created_at":"2026-05-17T23:41:36Z","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":"f7a37965ce34e2cdc54fcb5f2c1db85a3ee6f5cdef9a11e3c3256462fe9b60dc","cross_cats_sorted":["cond-mat.supr-con"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-13T19:00:03Z","title_canon_sha256":"7d900723362808e976fccee9bf457465eadea6250862a220ec9dea751a0e1e78"},"schema_version":"1.0","source":{"id":"1812.05627","kind":"arxiv","version":2}},"canonical_sha256":"3ff8885b73e6fcde5d828c737298b3e7fce285b8dcd032289c862ec3533b0415","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3ff8885b73e6fcde5d828c737298b3e7fce285b8dcd032289c862ec3533b0415","first_computed_at":"2026-05-17T23:41:36.712655Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:41:36.712655Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"F4orKPzYobgeozMDn8QC5JpxKaIYJjYm3JTFGzF3D6FHECxfPnS/0xmpa5N0A7H2HoX1T07l9BpvtQ203/U4Ag==","signature_status":"signed_v1","signed_at":"2026-05-17T23:41:36.713297Z","signed_message":"canonical_sha256_bytes"},"source_id":"1812.05627","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0d908b61a526b2d80b931a008ed0245e6349d1d60243ab8fe490e9a64bcb404f","sha256:a7509fff815d2e48602a7d958d7a0ca32cb05a499d55e0f3eda22a57b61d2d1f"],"state_sha256":"71a7ef34e170d95189b9c06ff3852e92dbda6f9f75e52e4886e6c433a84a7e0f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GBSa9iaX31w7evzegICZtcjlFxlSpesGN+PmIgVQm0jCw8jTMdCeAJPynpy5PfARxmQBGixEP4VKl213wRLBAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T10:21:42.465783Z","bundle_sha256":"ce053cb88fa8f85521864070aee9928b6626a7f13d33e4ebfca4761a92f42dd6"}}