{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:LPXITCAMDGMKESO7TAWNO74M43","short_pith_number":"pith:LPXITCAM","canonical_record":{"source":{"id":"1703.03430","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-09T19:17:04Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b45f54ea2158526f4e382b746903f5b53c468f9c6b894d10e242903694dad1ab","abstract_canon_sha256":"27f48cc13abe19c13e246e083f007d120117f09f5ff7a1791b8ef7331815859e"},"schema_version":"1.0"},"canonical_sha256":"5bee89880c1998a249df982cd77f8ce6efce1eea3382192d70d274008ba05b40","source":{"kind":"arxiv","id":"1703.03430","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.03430","created_at":"2026-05-18T00:37:52Z"},{"alias_kind":"arxiv_version","alias_value":"1703.03430v3","created_at":"2026-05-18T00:37:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.03430","created_at":"2026-05-18T00:37:52Z"},{"alias_kind":"pith_short_12","alias_value":"LPXITCAMDGMK","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LPXITCAMDGMKESO7","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LPXITCAM","created_at":"2026-05-18T12:31:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:LPXITCAMDGMKESO7TAWNO74M43","target":"record","payload":{"canonical_record":{"source":{"id":"1703.03430","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-09T19:17:04Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b45f54ea2158526f4e382b746903f5b53c468f9c6b894d10e242903694dad1ab","abstract_canon_sha256":"27f48cc13abe19c13e246e083f007d120117f09f5ff7a1791b8ef7331815859e"},"schema_version":"1.0"},"canonical_sha256":"5bee89880c1998a249df982cd77f8ce6efce1eea3382192d70d274008ba05b40","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:52.587906Z","signature_b64":"EEw5VikMwYgxu6ZVWYwBMyehIT/UBZER4W7NzCf68SBb1Rn0vA54AsPlQ9PFm02cB28mW6PAMBEUQ61nCb+LBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5bee89880c1998a249df982cd77f8ce6efce1eea3382192d70d274008ba05b40","last_reissued_at":"2026-05-18T00:37:52.587267Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:52.587267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.03430","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:37:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gpXaVsg3tCb/LUFCUW3DFV3dX/uO1Q4IIS0O3Hs1yZqfdeWTkaamMaPns9ILBLkIPm8LsWxCtUfKdPIiVaVNBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T05:03:11.850809Z"},"content_sha256":"33c11e56cde715d1e9b27ebbba007c380d200d1292880589ebe2d2764a61d04b","schema_version":"1.0","event_id":"sha256:33c11e56cde715d1e9b27ebbba007c380d200d1292880589ebe2d2764a61d04b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:LPXITCAMDGMKESO7TAWNO74M43","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Long-range critical exponents near the short-range crossover","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"cond-mat.stat-mech","authors_text":"Bernardo Zan, Connor Behan, Leonardo Rastelli, Slava Rychkov","submitted_at":"2017-03-09T19:17:04Z","abstract_excerpt":"The $d$-dimensional long-range Ising model, defined by spin-spin interactions decaying with the distance as the power $1/r^{d+s}$, admits a second order phase transition with continuously varying critical exponents. At $s = s_*$, the phase transition crosses over to the usual short-range universality class. The standard field-theoretic description of this family of models is strongly coupled at the crossover. We find a new description, which is instead weakly coupled near the crossover, and use it to compute critical exponents. The existence of two complementary UV descriptions of the same lon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.03430","kind":"arxiv","version":3},"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":"2026-05-18T00:37:52Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8/HrD7cVD8DhXdsCr17Q4PBP1Z118hD2GU0UlQN3ZUKuYa3IstZn+6iQOwerSPX2tfJVdMGxR77Gno33IoXfDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T05:03:11.851507Z"},"content_sha256":"849a06ca947528a70fc94bd7445b4a11c6f0b33b4e74e8598001f9efa19a4e30","schema_version":"1.0","event_id":"sha256:849a06ca947528a70fc94bd7445b4a11c6f0b33b4e74e8598001f9efa19a4e30"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LPXITCAMDGMKESO7TAWNO74M43/bundle.json","state_url":"https://pith.science/pith/LPXITCAMDGMKESO7TAWNO74M43/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LPXITCAMDGMKESO7TAWNO74M43/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":"2026-05-30T05:03:11Z","links":{"resolver":"https://pith.science/pith/LPXITCAMDGMKESO7TAWNO74M43","bundle":"https://pith.science/pith/LPXITCAMDGMKESO7TAWNO74M43/bundle.json","state":"https://pith.science/pith/LPXITCAMDGMKESO7TAWNO74M43/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LPXITCAMDGMKESO7TAWNO74M43/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:LPXITCAMDGMKESO7TAWNO74M43","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":"27f48cc13abe19c13e246e083f007d120117f09f5ff7a1791b8ef7331815859e","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-09T19:17:04Z","title_canon_sha256":"b45f54ea2158526f4e382b746903f5b53c468f9c6b894d10e242903694dad1ab"},"schema_version":"1.0","source":{"id":"1703.03430","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.03430","created_at":"2026-05-18T00:37:52Z"},{"alias_kind":"arxiv_version","alias_value":"1703.03430v3","created_at":"2026-05-18T00:37:52Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.03430","created_at":"2026-05-18T00:37:52Z"},{"alias_kind":"pith_short_12","alias_value":"LPXITCAMDGMK","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_16","alias_value":"LPXITCAMDGMKESO7","created_at":"2026-05-18T12:31:28Z"},{"alias_kind":"pith_short_8","alias_value":"LPXITCAM","created_at":"2026-05-18T12:31:28Z"}],"graph_snapshots":[{"event_id":"sha256:849a06ca947528a70fc94bd7445b4a11c6f0b33b4e74e8598001f9efa19a4e30","target":"graph","created_at":"2026-05-18T00:37:52Z","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":"The $d$-dimensional long-range Ising model, defined by spin-spin interactions decaying with the distance as the power $1/r^{d+s}$, admits a second order phase transition with continuously varying critical exponents. At $s = s_*$, the phase transition crosses over to the usual short-range universality class. The standard field-theoretic description of this family of models is strongly coupled at the crossover. We find a new description, which is instead weakly coupled near the crossover, and use it to compute critical exponents. The existence of two complementary UV descriptions of the same lon","authors_text":"Bernardo Zan, Connor Behan, Leonardo Rastelli, Slava Rychkov","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-09T19:17:04Z","title":"Long-range critical exponents near the short-range crossover"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.03430","kind":"arxiv","version":3},"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":"sha256:33c11e56cde715d1e9b27ebbba007c380d200d1292880589ebe2d2764a61d04b","target":"record","created_at":"2026-05-18T00:37:52Z","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":"27f48cc13abe19c13e246e083f007d120117f09f5ff7a1791b8ef7331815859e","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-09T19:17:04Z","title_canon_sha256":"b45f54ea2158526f4e382b746903f5b53c468f9c6b894d10e242903694dad1ab"},"schema_version":"1.0","source":{"id":"1703.03430","kind":"arxiv","version":3}},"canonical_sha256":"5bee89880c1998a249df982cd77f8ce6efce1eea3382192d70d274008ba05b40","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5bee89880c1998a249df982cd77f8ce6efce1eea3382192d70d274008ba05b40","first_computed_at":"2026-05-18T00:37:52.587267Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:37:52.587267Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EEw5VikMwYgxu6ZVWYwBMyehIT/UBZER4W7NzCf68SBb1Rn0vA54AsPlQ9PFm02cB28mW6PAMBEUQ61nCb+LBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:37:52.587906Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.03430","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:33c11e56cde715d1e9b27ebbba007c380d200d1292880589ebe2d2764a61d04b","sha256:849a06ca947528a70fc94bd7445b4a11c6f0b33b4e74e8598001f9efa19a4e30"],"state_sha256":"1e14a0c23762208a54bdc638482950c8aa992d9d96978064b3a60525d33136c5"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1soWrYM7xz0scdkcnGcvzm4t9rK5pZPTOWqIBd6WrCCQ0/7HYz6c8CjK/j6ucgLM4q3BjDwaTD1Bgj/x8MWRDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T05:03:11.855255Z","bundle_sha256":"7dbc680cc4db9b749f61693095b17caea1533d1e4210dd4a9714c6aaf97522bc"}}