{"as_of":"2026-08-13T21:02:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:dfcfabcca811ce063476ba432ec604bf7f09a2fcd23177945f7b9274e9c6b26e","coverage":[{"denominator":57,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":57,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-04T11:38:06.211415Z","state":"measured"},{"denominator":58,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":58,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-13T06:32:02.005865+00:00","state":"measured"},{"denominator":1,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":1,"source":"paper_references, paper_reference_links","source_observed_at":"2026-07-11T22:51:38.921909Z","state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[{"citation":{"cited_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2510.04164","snapshot_observed_at":"2026-07-11T22:51:38.921909Z","title":"Yosprakob, W.-L","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.03939","last_updated":"2026-07-04T16:16:45Z","snapshot_observed_at":"2026-07-11T22:51:37.468449Z","submitted_at":"2026-07-04T16:16:45Z","title":"Disentangling Haldane Phase by Generalized Clifford Circuits","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-07-11T22:51:38.921909Z"},"links":{"cited_paper":"/paper/2510.04164","citing_paper":"/paper/2607.03939"},"observation_digest":"sha256:d7537bc6f8be2d4a70fe0659ce8fc9a6298a5fdace62b2df6f778235552d4191","observation_id":"97740e86-75d3-44a8-b0e8-0dcf03652247","resolution":{"observed_at":"2026-07-11T22:51:38.921909Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2510.04164/citation-record","integrity":"/paper/2510.04164/integrity","json":"/paper/2510.04164/citation-record.json","paper":"/paper/2510.04164"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:37:59.542964Z","title":null,"venue":null,"work_id":null,"year":1987},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-04T11:37:59.542964Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:00c60d568f8e486ca6fee619eb2a4a686b1121543ef4d17e4e0014a29cb32660","observation_id":"0d786bf2-0aca-40c5-a4e2-259659c4343e","resolution":{"observed_at":"2026-08-04T11:37:59.542964Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:37:59.913890Z","title":"Dagotto, Correlated electrons in high-temperature supercon- ductors, Rev","venue":null,"work_id":null,"year":1994},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-04T11:37:59.913890Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:3fdca6539d5aca92bc3d6580d05e915e1285b453a1df5aa8cb9115b56c21bf1b","observation_id":"9aebb873-2645-4b4b-9515-e9ee55dacd3b","resolution":{"observed_at":"2026-08-04T11:37:59.913890Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:00.603025Z","title":"Georges, G","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:00.603025Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:90608e7effe4f77a2e2d98db11278a33089e104738470af57296ddb69750b292","observation_id":"8db96b04-1c70-46cd-8cac-4801c318ec84","resolution":{"observed_at":"2026-08-04T11:38:00.603025Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.129856Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.129856Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:80e35fc0a635566895066cfebab4bd56ebbe4117515285f3b041dbafcefac372","observation_id":"c4c384c5-889a-4e70-87e7-6749aa932140","resolution":{"observed_at":"2026-08-04T11:38:01.129856Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.169544Z","title":null,"venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.169544Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:0e5a0756d4967289d14608de6915ba06da6e14aa055f2966249b398cfdd2dac8","observation_id":"725ff5ab-6b7e-4d09-ac89-d0fba0975eb8","resolution":{"observed_at":"2026-08-04T11:38:01.169544Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.328928Z","title":null,"venue":null,"work_id":null,"year":1974},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.328928Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:ceef1456c6aaac27598dbd4bf3f2b47c2e529977f87c3608b074af9dc5e6b774","observation_id":"d73c55d1-6093-49e4-b99d-0ddb84bf06f5","resolution":{"observed_at":"2026-08-04T11:38:01.328928Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.373214Z","title":"Bazavov, D","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.373214Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:551b70bcef6836e01e7da2640bc39dfa165fccf1ee2cff80365e594ef4322bbe","observation_id":"f8655139-0fba-4e10-9cae-a3f6e7be68dd","resolution":{"observed_at":"2026-08-04T11:38:01.373214Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.447845Z","title":"Gattringer and C","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.447845Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:f4be306a9c51a3e1047e94b995eb516b2925806de223f8f8301e3adea7574712","observation_id":"1f891ae8-03c4-42c7-b028-3e438ac48f1e","resolution":{"observed_at":"2026-08-04T11:38:01.447845Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.518417Z","title":null,"venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.518417Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:a2d48be49bb4c2061bc1313dd29ca7df7606fd76cb46f2c6e7b4f84066703356","observation_id":"b778141a-c8ba-4387-b7ad-436141f513ef","resolution":{"observed_at":"2026-08-04T11:38:01.518417Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.588972Z","title":"Berges and K","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.588972Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:42a2436b69edaf77dbfce874929ad20f2291b99e7a828ac21db7eecc65b069d5","observation_id":"2ad0df13-12c7-4d07-b97f-b939dea79506","resolution":{"observed_at":"2026-08-04T11:38:01.588972Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.675986Z","title":"Satz, Colour deconfinement in nuclear collisions, Rep","venue":null,"work_id":null,"year":2000},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.675986Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:2eaa860f4d17d3f7f1a70bb1097e60d1e3dee5c852e2b40e7c489a1647f54032","observation_id":"cbcfc5b3-2e81-4383-837b-961e65d0ebee","resolution":{"observed_at":"2026-08-04T11:38:01.675986Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.772187Z","title":"Troyer and U.-J","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.772187Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:a83acce402488a3605ef72f2caa0d82152941eb8f610a7161930af8cab5dfe6a","observation_id":"a8449c22-2bfc-4190-841e-a7aaef9d986b","resolution":{"observed_at":"2026-08-04T11:38:01.772187Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.850240Z","title":null,"venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.850240Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:e5d02fb1b007c031a7e6af1fd8061d77973c1ead12ac91b7791c33831fb4510c","observation_id":"1d4e4ca5-1f6f-49aa-a7b4-edd6478df6be","resolution":{"observed_at":"2026-08-04T11:38:01.850240Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.932000Z","title":"Chandrasekharan and U.-J","venue":null,"work_id":null,"year":1999},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.932000Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:2bccab9b66c74865ca775979fe12f76f9d0af1d450c36e00cf6d4739c646101d","observation_id":"a9647d0c-6163-4348-a85b-4dbfd243e97b","resolution":{"observed_at":"2026-08-04T11:38:01.932000Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:01.978386Z","title":null,"venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:01.978386Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:1e6671bad5515b3703dd6ee6d62b627e089862c6404dfd2b434b51590ea8c4a2","observation_id":"79b93967-36c9-4073-8d44-b3a2cf66798c","resolution":{"observed_at":"2026-08-04T11:38:01.978386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.045039Z","title":null,"venue":null,"work_id":null,"year":1993},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.045039Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:6b27c64a1e9ef0530b61c875195c1810d43e8fa0371023ffddbdb0a4c2d08361","observation_id":"56b600a7-e38c-41d5-b5c0-ebfd2869efff","resolution":{"observed_at":"2026-08-04T11:38:02.045039Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.157975Z","title":"Schollw ¨ock, The density-matrix renormalization group, Rev","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.157975Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:4b7cd296b431425e6e9530ea8e1a9c43f2a1e9073178513d41184b8618af126d","observation_id":"64110b16-d172-494c-8962-561205d53c07","resolution":{"observed_at":"2026-08-04T11:38:02.157975Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.232820Z","title":"¨Ostlund and S","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.232820Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:f329258c387b4101abed666f6e6e38bf607c49a1d71abdb8802f9f8225dba074","observation_id":"23c5c22d-9a80-4104-a82b-efa9ec76726b","resolution":{"observed_at":"2026-08-04T11:38:02.232820Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.321955Z","title":"Verstraete, V","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.321955Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:379026b24693f59b2e7ad7511ecac52e85e880eaeb538b07b44020ce2014351e","observation_id":"65893b05-12b5-46bd-a443-0c1dba62ca7d","resolution":{"observed_at":"2026-08-04T11:38:02.321955Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.414163Z","title":null,"venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.414163Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:bcc3b684d86b8695d3d4b3568bced4657dcb46158247ff6ca5930215fb2bf4b5","observation_id":"ea041df1-ff60-44e0-a5ff-d798ea01830f","resolution":{"observed_at":"2026-08-04T11:38:02.414163Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.484316Z","title":"Schollw ¨ock, The density-matrix renormalization group in the age of matrix product states, Ann","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.484316Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:9dbdd6e4bf9eee686b3029c49bf845a86affd9df653f7a595c72f716b733c387","observation_id":"ed64f6c3-2766-40c9-9fae-2a2ba6991565","resolution":{"observed_at":"2026-08-04T11:38:02.484316Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.545880Z","title":"Or ´us, A practical introduction to tensor networks: Matrix product states and projected entangled pair states, Ann","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.545880Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:378908a7d20e141c22429781ab3ab473afabc805c2e44177be1d62994451967c","observation_id":"6cdd762c-86d4-4bfb-a384-0fe1bcf54750","resolution":{"observed_at":"2026-08-04T11:38:02.545880Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.633670Z","title":null,"venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.633670Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:354987da13b9acf1f4522a89a01e7a8f5128c23b2262412951efee0888a8a540","observation_id":"6c95bf18-e97c-4ffc-922d-b604265e37a5","resolution":{"observed_at":"2026-08-04T11:38:02.633670Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.704864Z","title":"Jordan and E","venue":null,"work_id":null,"year":1928},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.704864Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:12cf91e22f3684167be292c44d782df4bb4b29a4d8b787c9e6ce499796843d3d","observation_id":"ae1b6356-e8b2-40a6-9395-899a1b8ebceb","resolution":{"observed_at":"2026-08-04T11:38:02.704864Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.778297Z","title":null,"venue":null,"work_id":null,"year":1961},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.778297Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:bee2ed67bc44067da0f1649a43e67285bec581d102c242a8909f9ee0c1010e3c","observation_id":"c0a3cd60-715f-4864-9773-87a30ffb20f3","resolution":{"observed_at":"2026-08-04T11:38:02.778297Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.852750Z","title":null,"venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.852750Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:15e4f3187addc0a385809eea0c71a9056b7415fcc0ef9f8c782c8d9ca235238a","observation_id":"a25ca66f-387d-48d6-bfe9-59318d56a681","resolution":{"observed_at":"2026-08-04T11:38:02.852750Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:02.971423Z","title":"Verstraete and J","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:02.971423Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:2869d139d07331ae85af8d2cf703ec539a825285530c9cef7cfeabfe59dde09c","observation_id":"7d725051-a439-45f6-87ea-7c510a813a75","resolution":{"observed_at":"2026-08-04T11:38:02.971423Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.069192Z","title":"Barthel, C","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.069192Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:5aa3a1f67610dbf5263c3a70daa9c382b36d9d7212683026205152e91a61c586","observation_id":"fe78470e-eddd-4262-bde8-602a0f61a1d1","resolution":{"observed_at":"2026-08-04T11:38:03.069192Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.162995Z","title":"Corboz and G","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.162995Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:d4aeed76c794ce1b02e7200c024e3d0cfa88d3f39a426753abc4f4c49b83421b","observation_id":"189970f5-6f80-4bd9-a963-77b52c3430f2","resolution":{"observed_at":"2026-08-04T11:38:03.162995Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.261065Z","title":"Pineda, T","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.261065Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:84594be6933b0a6dc188cac1b222e95182e29610870212266937bd506e0bf9da","observation_id":"82ada948-8d0f-4cbf-a874-f9d30bc5e988","resolution":{"observed_at":"2026-08-04T11:38:03.261065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.363001Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.363001Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:3a1a1de4a72d11999ae0fa9b90fcbf17b1e59f57c7af8026b6f435fc4b4ae7ff","observation_id":"2f8b1412-bdc2-4841-8e20-41b919bb4368","resolution":{"observed_at":"2026-08-04T11:38:03.363001Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.455449Z","title":"Corboz, G","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.455449Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:794165e3ada31c013239ded9d7fdae22f90d9ac2887b5034e7efe8ec79c10c26","observation_id":"af7c6c27-0418-4323-b45c-727b45a40b92","resolution":{"observed_at":"2026-08-04T11:38:03.455449Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.525057Z","title":"Bruognolo, J.-W","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.525057Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:577a91615ba4d280723b70dccf82f70da6bdff563f667ffee0003adee4dbd7d9","observation_id":"6d384f1a-4eed-41df-b60c-0354792f1bc8","resolution":{"observed_at":"2026-08-04T11:38:03.525057Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1004.2563","last_updated":"2010-04-15T07:10:53Z","snapshot_observed_at":"2026-08-10T10:28:10.272970Z","submitted_at":"2010-04-15T07:10:53Z","title":"Grassmann tensor network states and its renormalization for strongly correlated fermionic and bosonic states","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1004.2563","snapshot_observed_at":"2026-08-04T11:38:03.654911Z","title":null,"venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.654911Z"},"links":{"cited_paper":"/paper/1004.2563","citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:02ba02c9bc9011051a60046d7163fd44d5cafcd2b3a3961f8d27338bf9931bec","observation_id":"ff07200c-5a0a-441a-a3f0-7d4da4082ad5","resolution":{"observed_at":"2026-08-04T11:38:03.654911Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.748490Z","title":"Gu, Efficient simulation of grassmann tensor product states, Phys","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.748490Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:2dde71e1b4e1d8a926cd32ea6372082cefe67fa5916155a88690c6a0191832b7","observation_id":"1b1e2ff0-41a6-48ce-9b36-b6df472bfc1b","resolution":{"observed_at":"2026-08-04T11:38:03.748490Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:03.849106Z","title":"Yosprakob, Grassmanntn: A python package for grassmann tensor network computations, SciPost Physics Codebases , 020 (2023)","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.849106Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:f411b0c1d543acf6110d7e682423e44a961d87190467d197cc0e368e8303d30c","observation_id":"084a7adc-b769-4779-9492-a900b21e0570","resolution":{"observed_at":"2026-08-04T11:38:03.849106Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"quant-ph/9807006","last_updated":"1998-07-01T19:34:39Z","snapshot_observed_at":"2026-08-13T13:22:45.686549Z","submitted_at":"1998-07-01T19:34:39Z","title":"The Heisenberg Representation of Quantum Computers","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"quant-ph/9807006","snapshot_observed_at":"2026-08-04T11:38:03.966574Z","title":"Gottesman, The heisenberg representation of quantum com- puters, arXiv quant-ph/9807006 (1998)","venue":null,"work_id":null,"year":1998},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:03.966574Z"},"links":{"cited_paper":"/paper/quant-ph/9807006","citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:eba22d62fe0031a2770a587328157ad289c901a7a0f4a16768ac2c33f1d4cd1f","observation_id":"16f1d6ed-da27-4a7e-b113-19cbf670fb72","resolution":{"observed_at":"2026-08-04T11:38:03.966574Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.036758Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.036758Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:c6f6fdd1f51e1f8d0caf8d8d1b82e39d3b1665742d68c31bcb4c5ead7d6dd13b","observation_id":"9043f850-e97b-40c3-901a-0a5117b80535","resolution":{"observed_at":"2026-08-04T11:38:04.036758Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.137995Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.137995Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:477795aebb770dc2cc23e0d2a2378bcb158e2108106f6977788bbf0d50cd1bb1","observation_id":"47436ec9-574d-4917-80c7-7cf64ffa2ddf","resolution":{"observed_at":"2026-08-04T11:38:04.137995Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.230213Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.230213Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:f356dacd340e59156fb26551c0308b10a27228a008b684da3f270a3da28b3256","observation_id":"cb23fb32-382c-4d81-af37-7310543d9eba","resolution":{"observed_at":"2026-08-04T11:38:04.230213Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.330375Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.330375Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:766c0cd64e1050cda8c358c51b89c915a362e492043bcda9500b649407eb3183","observation_id":"f524c013-5caf-4552-bacf-921f8e323505","resolution":{"observed_at":"2026-08-04T11:38:04.330375Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.417824Z","title":"Huang, X","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.417824Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:d6972356fda0489f17b62857be55547eede57eac13365c6f2dc665ec4362d054","observation_id":"15b90aed-328a-4167-bacd-658d277bc244","resolution":{"observed_at":"2026-08-04T11:38:04.417824Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.520284Z","title":"Huang, X","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.520284Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:eb45a2d29ac8e0d587307c9fcc09bc8fd17a155f876a27b7991f21baee2934a6","observation_id":"0dfa920b-dd40-4c34-b272-1b166f7207a5","resolution":{"observed_at":"2026-08-04T11:38:04.520284Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.607643Z","title":"Huang, X","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.607643Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:7260210bfbb16312068a21d10046ee963d5ab18777c7df4b95574ffdde8da7d5","observation_id":"d11b4eb8-cd93-4e65-8d83-164cd8810ca9","resolution":{"observed_at":"2026-08-04T11:38:04.607643Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.710162Z","title":"Tagliacozzo and G","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.710162Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:8a54db27920f2c26367f6066219c079a9ebe6d02f6b2ce9ba752db0bc295b27d","observation_id":"89076c81-67b9-4b6e-950a-5857cf17152f","resolution":{"observed_at":"2026-08-04T11:38:04.710162Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.811984Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.811984Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:d549fac06eedd0e32e5bb3db07e8d3a8ffee87deefca8472980b3fdb0cc52fcd","observation_id":"2c754822-f5ce-4674-ba7e-7475e9355d78","resolution":{"observed_at":"2026-08-04T11:38:04.811984Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.878839Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.878839Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:ff73e0ca621c37cc26041f2d71e27333e8ffaee01521ed858e7b00a134421d56","observation_id":"c23c6ebe-d3f5-423c-b034-cc1c0787f003","resolution":{"observed_at":"2026-08-04T11:38:04.878839Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:04.977140Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:04.977140Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:894dede794d52380135ca7206953a83204ab6d5f18128b6cfb5282cae1e0863c","observation_id":"2fcc6647-77f2-4b45-9d65-2c04760ea04f","resolution":{"observed_at":"2026-08-04T11:38:04.977140Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:05.090410Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:05.090410Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:d66f876baf49ed40f0c2a29efc91ac138cd2e6ac73d00491e9b5acff8b39a619","observation_id":"a3fcd5db-52d1-4cd6-9b66-9fdc98658488","resolution":{"observed_at":"2026-08-04T11:38:05.090410Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:05.254691Z","title":"Masot-Llima and A","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:05.254691Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:424639a8adef234571dca8942b2913de54195ef798f45f9f8457309a37233e18","observation_id":"96b23ecb-b11f-4289-9953-be27cab2ece7","resolution":{"observed_at":"2026-08-04T11:38:05.254691Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:05.476966Z","title":null,"venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:05.476966Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:0be51da0ea12d04f1946f04051a9bf2ded353ad478122f73904d62db9eca6c04","observation_id":"f9f3cccb-e75b-4856-9b02-fb3a18d4a022","resolution":{"observed_at":"2026-08-04T11:38:05.476966Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:05.588648Z","title":"Collura, G","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:05.588648Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:855209d58c6586ce9a40408427a745b45421d17ec3cd2309bf6b09700a1b2eaf","observation_id":"7e1ca7af-1761-4b41-95af-4dfce16416f1","resolution":{"observed_at":"2026-08-04T11:38:05.588648Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:05.939997Z","title":null,"venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:05.939997Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:dab526ae67e7d31e8ce08278997c8b553dce360fae2f66d66a1fb1412f7acea0","observation_id":"c52efe1e-8290-4c61-99af-263b0bc9d93d","resolution":{"observed_at":"2026-08-04T11:38:05.939997Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:05.996326Z","title":"Harper, A","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:05.996326Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:fc0bb4b016bf204212e5bbcc7076454ca31bdee465d56b5e4ecdb25439c3eedb","observation_id":"b14a621d-b023-47dc-94eb-bc91caea8057","resolution":{"observed_at":"2026-08-04T11:38:05.996326Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:06.056741Z","title":"Hoshino and Y","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:06.056741Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:939c299cee2b5c171045a38b8dba23cb0cc966e88c7af4d5d9d7ee7e23a57376","observation_id":"f8bf7b1e-5b24-4ba0-8bd9-d50730153fe1","resolution":{"observed_at":"2026-08-04T11:38:06.056741Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:06.118750Z","title":"Collura, J","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:06.118750Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:acd012b9a6dc07a5f4dd7bc5a91a318676ebdcf65ed8e0933a5b8b12189cfece","observation_id":"e5aa99c5-f663-4580-a307-7210f9542134","resolution":{"observed_at":"2026-08-04T11:38:06.118750Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-04T11:38:06.211415Z","title":"Sierant, P","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States","version":3},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-04T11:38:06.211415Z"},"links":{"citing_paper":"/paper/2510.04164"},"observation_digest":"sha256:733eb0e670dc93333e23f47ac03e1a2280f98fb74edbba0a34a3dfe68ffe5a90","observation_id":"d93012b2-c22c-43d3-a769-5489aff5f35e","resolution":{"observed_at":"2026-08-04T11:38:06.211415Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2510.04164","last_updated":"2026-06-06T01:39:00Z","latest_version":3,"primary_category":"quant-ph","snapshot_observed_at":"2026-08-04T11:37:58.990541Z","submitted_at":"2025-10-05T11:42:28Z","title":"Clifford Circuits Augmented Grassmann Matrix Product States"},"reference_resolution":{"displayed":57,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":57,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":57},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-13T06:32:02.005865+00:00","source":"crossref"},{"observed_at":"2026-08-13T06:31:53.387327+00:00","source":"retraction_watch"}],"thesis":"As of 13 August 2026, this Paper Citation Record lists 57 of 57 outbound references and 1 inbound Pith citation observation for arXiv:2510.04164."}