{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:2APH7YOTMPQZ2YXFP7VBLY7UPE","short_pith_number":"pith:2APH7YOT","schema_version":"1.0","canonical_sha256":"d01e7fe1d363e19d62e57fea15e3f4793a2790ee150133bc1eef64a8b85f6750","source":{"kind":"arxiv","id":"2012.11708","version":2},"attestation_state":"computed","paper":{"title":"Fractons from a liquid of singlet pairs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hernan B. Xavier, Rodrigo G. Pereira","submitted_at":"2020-12-21T22:10:40Z","abstract_excerpt":"Fracton phases of matter feature a variety of exciting phenomena stemming from the restricted mobility of their quasiparticles. Here we consider a model of interacting electrons in one dimension that describes hopping of spin-singlet pairs and obeys both charge and dipole conservation laws. The model contains Bethe ansatz integrable sectors which allow us to solve the ground state and calculate the exact spin and single-electron excitation gaps. We observe hallmarks of fractonic behavior, including localization of single-electron excitations and propensity to clustering. Our results demonstrat"},"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":"2012.11708","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2020-12-21T22:10:40Z","cross_cats_sorted":[],"title_canon_sha256":"2b989aaeeedb6823505c41016a0022acc11f5adccec4243ad07ff2d3e2d7089e","abstract_canon_sha256":"efd54803d0867b47ed119fd1a1d2e2d6954210ea6bcb455daf8e789bd1506a04"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:11:25.625109Z","signature_b64":"4Zox3HhI+/HdJ1SGqz6sLbv0AUes8v31L8qGnDEZ1Xmqh+R+BQgYQoYmVObmAj8T55zwWA9bcvZSStCZvYVnDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d01e7fe1d363e19d62e57fea15e3f4793a2790ee150133bc1eef64a8b85f6750","last_reissued_at":"2026-07-05T02:11:25.624777Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:11:25.624777Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fractons from a liquid of singlet pairs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hernan B. Xavier, Rodrigo G. Pereira","submitted_at":"2020-12-21T22:10:40Z","abstract_excerpt":"Fracton phases of matter feature a variety of exciting phenomena stemming from the restricted mobility of their quasiparticles. Here we consider a model of interacting electrons in one dimension that describes hopping of spin-singlet pairs and obeys both charge and dipole conservation laws. The model contains Bethe ansatz integrable sectors which allow us to solve the ground state and calculate the exact spin and single-electron excitation gaps. We observe hallmarks of fractonic behavior, including localization of single-electron excitations and propensity to clustering. Our results demonstrat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.11708","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2012.11708/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":"2012.11708","created_at":"2026-07-05T02:11:25.624834+00:00"},{"alias_kind":"arxiv_version","alias_value":"2012.11708v2","created_at":"2026-07-05T02:11:25.624834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.11708","created_at":"2026-07-05T02:11:25.624834+00:00"},{"alias_kind":"pith_short_12","alias_value":"2APH7YOTMPQZ","created_at":"2026-07-05T02:11:25.624834+00:00"},{"alias_kind":"pith_short_16","alias_value":"2APH7YOTMPQZ2YXF","created_at":"2026-07-05T02:11:25.624834+00:00"},{"alias_kind":"pith_short_8","alias_value":"2APH7YOT","created_at":"2026-07-05T02:11:25.624834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.13951","citing_title":"Weak ergodicity breaking with isolated integrable sectors","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE","json":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE.json","graph_json":"https://pith.science/api/pith-number/2APH7YOTMPQZ2YXFP7VBLY7UPE/graph.json","events_json":"https://pith.science/api/pith-number/2APH7YOTMPQZ2YXFP7VBLY7UPE/events.json","paper":"https://pith.science/paper/2APH7YOT"},"agent_actions":{"view_html":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE","download_json":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE.json","view_paper":"https://pith.science/paper/2APH7YOT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2012.11708&json=true","fetch_graph":"https://pith.science/api/pith-number/2APH7YOTMPQZ2YXFP7VBLY7UPE/graph.json","fetch_events":"https://pith.science/api/pith-number/2APH7YOTMPQZ2YXFP7VBLY7UPE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE/action/storage_attestation","attest_author":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE/action/author_attestation","sign_citation":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE/action/citation_signature","submit_replication":"https://pith.science/pith/2APH7YOTMPQZ2YXFP7VBLY7UPE/action/replication_record"}},"created_at":"2026-07-05T02:11:25.624834+00:00","updated_at":"2026-07-05T02:11:25.624834+00:00"}