{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:5JNUOADAH2OBPWDEX7DTEQU362","short_pith_number":"pith:5JNUOADA","canonical_record":{"source":{"id":"cond-mat/0307699","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-07-29T10:11:26Z","cross_cats_sorted":["cond-mat.dis-nn","hep-lat"],"title_canon_sha256":"136e86c81ca725b456fb999d0303f62e3e39dd78838af6a76ec983ce21ce992c","abstract_canon_sha256":"5cb52873aaec52b75367c4df06aea09667b2acbb1da004d1675d3418841623c3"},"schema_version":"1.0"},"canonical_sha256":"ea5b4700603e9c17d864bfc732429bf68c3aba6d99e9ab8c89444daae9edf9db","source":{"kind":"arxiv","id":"cond-mat/0307699","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0307699","created_at":"2026-05-18T01:06:57Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0307699v3","created_at":"2026-05-18T01:06:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0307699","created_at":"2026-05-18T01:06:57Z"},{"alias_kind":"pith_short_12","alias_value":"5JNUOADAH2OB","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"5JNUOADAH2OBPWDE","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"5JNUOADA","created_at":"2026-05-18T12:25:51Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:5JNUOADAH2OBPWDEX7DTEQU362","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0307699","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-07-29T10:11:26Z","cross_cats_sorted":["cond-mat.dis-nn","hep-lat"],"title_canon_sha256":"136e86c81ca725b456fb999d0303f62e3e39dd78838af6a76ec983ce21ce992c","abstract_canon_sha256":"5cb52873aaec52b75367c4df06aea09667b2acbb1da004d1675d3418841623c3"},"schema_version":"1.0"},"canonical_sha256":"ea5b4700603e9c17d864bfc732429bf68c3aba6d99e9ab8c89444daae9edf9db","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:57.046810Z","signature_b64":"HJunBkdJaaZoR0V5XovgLbm9FkDTmMrM3jfouusNnPIFZF8ammHRSZKtbnB0lNRkLd3YGK1PFcYRdP7jg9fQAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ea5b4700603e9c17d864bfc732429bf68c3aba6d99e9ab8c89444daae9edf9db","last_reissued_at":"2026-05-18T01:06:57.046151Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:57.046151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0307699","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":"2026-05-18T01:06:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PNZY4sFPON3eg0zihHCOxNwCG7sV8HcKJapa/jSk9U20Gj4v0kvLvpl4tNRs5sAEcgIE30I5FgQoO15ArqDVBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:49:52.774406Z"},"content_sha256":"52f809c038204ada06c24b8a6eb29e7018287decb5be3f184b56a2eaf586fae4","schema_version":"1.0","event_id":"sha256:52f809c038204ada06c24b8a6eb29e7018287decb5be3f184b56a2eaf586fae4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:5JNUOADAH2OBPWDEX7DTEQU362","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Crossover behavior in three-dimensional dilute spin systems","license":"","headline":"","cross_cats":["cond-mat.dis-nn","hep-lat"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andrea Pelissetto, Ettore Vicari, Pasquale Calabrese, Pietro Parruccini","submitted_at":"2003-07-29T10:11:26Z","abstract_excerpt":"We study the crossover behaviors that can be observed in the high-temperature phase of three-dimensional dilute spin systems, using a field-theoretical approach. In particular, for randomly dilute Ising systems we consider the Gaussian-to-random and the pure-Ising-to-random crossover, determining the corresponding crossover functions for the magnetic susceptibility and the correlation length. Moreover, for the physically interesting cases of dilute Ising, XY, and Heisenberg systems, we estimate several universal ratios of scaling-correction amplitudes entering the high-temperature Wegner expan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0307699","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":"2026-05-18T01:06:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8qRuTsj5Jj4FuQ1CT0Ke2oN1OXRyEjnWVzC3hi3gEIPVM7vng/heHBYx49PigUo39heI0dSQ6jrKAquCHH7dDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T15:49:52.774813Z"},"content_sha256":"ba39fb5bd3c95decacb0b16238c83de8d1d536b22a15e8ee53249537b854dfc1","schema_version":"1.0","event_id":"sha256:ba39fb5bd3c95decacb0b16238c83de8d1d536b22a15e8ee53249537b854dfc1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5JNUOADAH2OBPWDEX7DTEQU362/bundle.json","state_url":"https://pith.science/pith/5JNUOADAH2OBPWDEX7DTEQU362/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5JNUOADAH2OBPWDEX7DTEQU362/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":"2026-05-27T15:49:52Z","links":{"resolver":"https://pith.science/pith/5JNUOADAH2OBPWDEX7DTEQU362","bundle":"https://pith.science/pith/5JNUOADAH2OBPWDEX7DTEQU362/bundle.json","state":"https://pith.science/pith/5JNUOADAH2OBPWDEX7DTEQU362/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5JNUOADAH2OBPWDEX7DTEQU362/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:5JNUOADAH2OBPWDEX7DTEQU362","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":"5cb52873aaec52b75367c4df06aea09667b2acbb1da004d1675d3418841623c3","cross_cats_sorted":["cond-mat.dis-nn","hep-lat"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-07-29T10:11:26Z","title_canon_sha256":"136e86c81ca725b456fb999d0303f62e3e39dd78838af6a76ec983ce21ce992c"},"schema_version":"1.0","source":{"id":"cond-mat/0307699","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0307699","created_at":"2026-05-18T01:06:57Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0307699v3","created_at":"2026-05-18T01:06:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0307699","created_at":"2026-05-18T01:06:57Z"},{"alias_kind":"pith_short_12","alias_value":"5JNUOADAH2OB","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_16","alias_value":"5JNUOADAH2OBPWDE","created_at":"2026-05-18T12:25:51Z"},{"alias_kind":"pith_short_8","alias_value":"5JNUOADA","created_at":"2026-05-18T12:25:51Z"}],"graph_snapshots":[{"event_id":"sha256:ba39fb5bd3c95decacb0b16238c83de8d1d536b22a15e8ee53249537b854dfc1","target":"graph","created_at":"2026-05-18T01:06:57Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study the crossover behaviors that can be observed in the high-temperature phase of three-dimensional dilute spin systems, using a field-theoretical approach. In particular, for randomly dilute Ising systems we consider the Gaussian-to-random and the pure-Ising-to-random crossover, determining the corresponding crossover functions for the magnetic susceptibility and the correlation length. Moreover, for the physically interesting cases of dilute Ising, XY, and Heisenberg systems, we estimate several universal ratios of scaling-correction amplitudes entering the high-temperature Wegner expan","authors_text":"Andrea Pelissetto, Ettore Vicari, Pasquale Calabrese, Pietro Parruccini","cross_cats":["cond-mat.dis-nn","hep-lat"],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-07-29T10:11:26Z","title":"Crossover behavior in three-dimensional dilute spin systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0307699","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":"sha256:52f809c038204ada06c24b8a6eb29e7018287decb5be3f184b56a2eaf586fae4","target":"record","created_at":"2026-05-18T01:06:57Z","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":"5cb52873aaec52b75367c4df06aea09667b2acbb1da004d1675d3418841623c3","cross_cats_sorted":["cond-mat.dis-nn","hep-lat"],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2003-07-29T10:11:26Z","title_canon_sha256":"136e86c81ca725b456fb999d0303f62e3e39dd78838af6a76ec983ce21ce992c"},"schema_version":"1.0","source":{"id":"cond-mat/0307699","kind":"arxiv","version":3}},"canonical_sha256":"ea5b4700603e9c17d864bfc732429bf68c3aba6d99e9ab8c89444daae9edf9db","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ea5b4700603e9c17d864bfc732429bf68c3aba6d99e9ab8c89444daae9edf9db","first_computed_at":"2026-05-18T01:06:57.046151Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:06:57.046151Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HJunBkdJaaZoR0V5XovgLbm9FkDTmMrM3jfouusNnPIFZF8ammHRSZKtbnB0lNRkLd3YGK1PFcYRdP7jg9fQAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:06:57.046810Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0307699","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:52f809c038204ada06c24b8a6eb29e7018287decb5be3f184b56a2eaf586fae4","sha256:ba39fb5bd3c95decacb0b16238c83de8d1d536b22a15e8ee53249537b854dfc1"],"state_sha256":"7d27e64fd7ac29d78effafd3d8e16d105c839fa101abd7e7e482a40d0593fbc6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v+sTqrCE4609xtGgg+KNZfzpUYoLFzDXwDgGvi2FzFh5Q2CjWRvFEZqo7xsMsbbJhEavOQNWlA4mpsGgrjvWBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T15:49:52.777268Z","bundle_sha256":"60beec4978571ff112e60e4f0ba0fa7ca704b91d95477d936e969054e120f9a9"}}