{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:3WJUIH7EHBXG7HKSH37WMCSPPX","short_pith_number":"pith:3WJUIH7E","canonical_record":{"source":{"id":"1801.03118","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-01-09T19:30:00Z","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","hep-th"],"title_canon_sha256":"015f406cfe96a5fc9b34670eee1c9d44b0fe86187668269c0a20b024c04715f2","abstract_canon_sha256":"db810d3144c5b0420d957a80a3565fe1ba4ed46f031f0815ca557531e90fc736"},"schema_version":"1.0"},"canonical_sha256":"dd93441fe4386e6f9d523eff660a4f7dcfa1243cb1f61eeda8bc79037b1a37ba","source":{"kind":"arxiv","id":"1801.03118","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.03118","created_at":"2026-05-18T00:15:09Z"},{"alias_kind":"arxiv_version","alias_value":"1801.03118v2","created_at":"2026-05-18T00:15:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.03118","created_at":"2026-05-18T00:15:09Z"},{"alias_kind":"pith_short_12","alias_value":"3WJUIH7EHBXG","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_16","alias_value":"3WJUIH7EHBXG7HKS","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_8","alias_value":"3WJUIH7E","created_at":"2026-05-18T12:32:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:3WJUIH7EHBXG7HKSH37WMCSPPX","target":"record","payload":{"canonical_record":{"source":{"id":"1801.03118","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-01-09T19:30:00Z","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","hep-th"],"title_canon_sha256":"015f406cfe96a5fc9b34670eee1c9d44b0fe86187668269c0a20b024c04715f2","abstract_canon_sha256":"db810d3144c5b0420d957a80a3565fe1ba4ed46f031f0815ca557531e90fc736"},"schema_version":"1.0"},"canonical_sha256":"dd93441fe4386e6f9d523eff660a4f7dcfa1243cb1f61eeda8bc79037b1a37ba","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:09.849886Z","signature_b64":"Rd4exLCAlOFgZN3bzx9CAekr4zqYZLBW/J9S13MuT3Dk4qa84qRtLFDdwdwoKHtoUPZ2DkjsSHhTB0Gvr11sDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dd93441fe4386e6f9d523eff660a4f7dcfa1243cb1f61eeda8bc79037b1a37ba","last_reissued_at":"2026-05-18T00:15:09.849386Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:09.849386Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.03118","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":"2026-05-18T00:15:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HdlLU//08TP9HV+mUijq8HODaM6Ef01n8CIx1q9O7MYvtRN9KslpbpBvuxWhfACnHoqQOJdLTu9Y4iqWJNo5Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T01:54:42.939525Z"},"content_sha256":"456409b4a8cd4ac06dd57be52d5c53db6ed38712d884f2926a27d3f610ed61aa","schema_version":"1.0","event_id":"sha256:456409b4a8cd4ac06dd57be52d5c53db6ed38712d884f2926a27d3f610ed61aa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:3WJUIH7EHBXG7HKSH37WMCSPPX","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonperturbative renormalization-group approach preserving the momentum dependence of correlation functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"F\\'elix Rose, Nicolas Dupuis","submitted_at":"2018-01-09T19:30:00Z","abstract_excerpt":"We present an approximation scheme of the nonperturbative renormalization group that preserves the momentum dependence of correlation functions. This approximation scheme can be seen as a simple improvement of the local potential approximation (LPA) where the derivative terms in the effective action are promoted to arbitrary momentum-dependent functions. As in the LPA the only field dependence comes from the effective potential, which allows us to solve the renormalization-group equations at a relatively modest numerical cost (as compared, e.g., to the Blaizot--Mend\\'ez-Galain--Wschebor approx"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.03118","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":"2026-05-18T00:15:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JmR7a4KGL8Dwf6QnhvS01VXBCLviTC43qLyR04THJ46uF/z0Yr2qGXbsp/0mXzHDdLtFUbpic4Gw1rOzvPh3Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T01:54:42.940210Z"},"content_sha256":"7d149e9682c1271d338400c6392192f152a9519f0430db5506057855dd678590","schema_version":"1.0","event_id":"sha256:7d149e9682c1271d338400c6392192f152a9519f0430db5506057855dd678590"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3WJUIH7EHBXG7HKSH37WMCSPPX/bundle.json","state_url":"https://pith.science/pith/3WJUIH7EHBXG7HKSH37WMCSPPX/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3WJUIH7EHBXG7HKSH37WMCSPPX/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":"2026-06-09T01:54:42Z","links":{"resolver":"https://pith.science/pith/3WJUIH7EHBXG7HKSH37WMCSPPX","bundle":"https://pith.science/pith/3WJUIH7EHBXG7HKSH37WMCSPPX/bundle.json","state":"https://pith.science/pith/3WJUIH7EHBXG7HKSH37WMCSPPX/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3WJUIH7EHBXG7HKSH37WMCSPPX/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:3WJUIH7EHBXG7HKSH37WMCSPPX","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":"db810d3144c5b0420d957a80a3565fe1ba4ed46f031f0815ca557531e90fc736","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-01-09T19:30:00Z","title_canon_sha256":"015f406cfe96a5fc9b34670eee1c9d44b0fe86187668269c0a20b024c04715f2"},"schema_version":"1.0","source":{"id":"1801.03118","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.03118","created_at":"2026-05-18T00:15:09Z"},{"alias_kind":"arxiv_version","alias_value":"1801.03118v2","created_at":"2026-05-18T00:15:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.03118","created_at":"2026-05-18T00:15:09Z"},{"alias_kind":"pith_short_12","alias_value":"3WJUIH7EHBXG","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_16","alias_value":"3WJUIH7EHBXG7HKS","created_at":"2026-05-18T12:32:05Z"},{"alias_kind":"pith_short_8","alias_value":"3WJUIH7E","created_at":"2026-05-18T12:32:05Z"}],"graph_snapshots":[{"event_id":"sha256:7d149e9682c1271d338400c6392192f152a9519f0430db5506057855dd678590","target":"graph","created_at":"2026-05-18T00:15:09Z","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 present an approximation scheme of the nonperturbative renormalization group that preserves the momentum dependence of correlation functions. This approximation scheme can be seen as a simple improvement of the local potential approximation (LPA) where the derivative terms in the effective action are promoted to arbitrary momentum-dependent functions. As in the LPA the only field dependence comes from the effective potential, which allows us to solve the renormalization-group equations at a relatively modest numerical cost (as compared, e.g., to the Blaizot--Mend\\'ez-Galain--Wschebor approx","authors_text":"F\\'elix Rose, Nicolas Dupuis","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-01-09T19:30:00Z","title":"Nonperturbative renormalization-group approach preserving the momentum dependence of correlation functions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.03118","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":"sha256:456409b4a8cd4ac06dd57be52d5c53db6ed38712d884f2926a27d3f610ed61aa","target":"record","created_at":"2026-05-18T00:15:09Z","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":"db810d3144c5b0420d957a80a3565fe1ba4ed46f031f0815ca557531e90fc736","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-01-09T19:30:00Z","title_canon_sha256":"015f406cfe96a5fc9b34670eee1c9d44b0fe86187668269c0a20b024c04715f2"},"schema_version":"1.0","source":{"id":"1801.03118","kind":"arxiv","version":2}},"canonical_sha256":"dd93441fe4386e6f9d523eff660a4f7dcfa1243cb1f61eeda8bc79037b1a37ba","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dd93441fe4386e6f9d523eff660a4f7dcfa1243cb1f61eeda8bc79037b1a37ba","first_computed_at":"2026-05-18T00:15:09.849386Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:15:09.849386Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Rd4exLCAlOFgZN3bzx9CAekr4zqYZLBW/J9S13MuT3Dk4qa84qRtLFDdwdwoKHtoUPZ2DkjsSHhTB0Gvr11sDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:15:09.849886Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.03118","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:456409b4a8cd4ac06dd57be52d5c53db6ed38712d884f2926a27d3f610ed61aa","sha256:7d149e9682c1271d338400c6392192f152a9519f0430db5506057855dd678590"],"state_sha256":"e8dd9c4e858b5c7b9b26ea1beaa8b2b2f1833bc4598b80e839d346c9e6de6160"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZvgcCXB6fULCMGTmb8aMF9QfZXEBCXP5c5LRyefFJP46i6xeSRPXM75qL/IOZhsD/+Ci2UEDhlSuUFNPQyRdBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T01:54:42.944930Z","bundle_sha256":"09600963c4415f92670586b6329f3aedf30b1b8300410d626bd7bc1ee96ba77d"}}