{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:DQACLQSGRZP4MHDOWMJMEHP6Q4","short_pith_number":"pith:DQACLQSG","canonical_record":{"source":{"id":"1209.0926","kind":"arxiv","version":7},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-09-05T11:10:40Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"title_canon_sha256":"83dea7b2a5f89c1d09425c917f31c504e7842cc6189fedf8e2ad712bac1ba99e","abstract_canon_sha256":"2bff543c534ac7a05705dda509147bd7cc3fc1e713d86f5a4f5d6330fbd22c9b"},"schema_version":"1.0"},"canonical_sha256":"1c0025c2468e5fc61c6eb312c21dfe8717eba1a4e0fc31b0aa8c46a33a12f1ac","source":{"kind":"arxiv","id":"1209.0926","version":7},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1209.0926","created_at":"2026-05-18T03:31:32Z"},{"alias_kind":"arxiv_version","alias_value":"1209.0926v7","created_at":"2026-05-18T03:31:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.0926","created_at":"2026-05-18T03:31:32Z"},{"alias_kind":"pith_short_12","alias_value":"DQACLQSGRZP4","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"DQACLQSGRZP4MHDO","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"DQACLQSG","created_at":"2026-05-18T12:27:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:DQACLQSGRZP4MHDOWMJMEHP6Q4","target":"record","payload":{"canonical_record":{"source":{"id":"1209.0926","kind":"arxiv","version":7},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-09-05T11:10:40Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"title_canon_sha256":"83dea7b2a5f89c1d09425c917f31c504e7842cc6189fedf8e2ad712bac1ba99e","abstract_canon_sha256":"2bff543c534ac7a05705dda509147bd7cc3fc1e713d86f5a4f5d6330fbd22c9b"},"schema_version":"1.0"},"canonical_sha256":"1c0025c2468e5fc61c6eb312c21dfe8717eba1a4e0fc31b0aa8c46a33a12f1ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:31:32.696146Z","signature_b64":"HCz1yV3fHueEMp/kKD4G1loGgjFIsGPyKDuy4Ref/b3pXwPC0NWhorB+p2F6Cr86Gd5ZgNvul5qC2z8o5ZzVCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1c0025c2468e5fc61c6eb312c21dfe8717eba1a4e0fc31b0aa8c46a33a12f1ac","last_reissued_at":"2026-05-18T03:31:32.695458Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:31:32.695458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1209.0926","source_version":7,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:31:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cWBl/U998becqGr1KaVpUGFQXDc8LWF9T+DmtLpMfcvPDY++xlcyJz4cwq8gSXbPMITdodalrcgZcBqUISahAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T11:55:14.142332Z"},"content_sha256":"ffeed704708399393f0047d03ad5a617fe582ab9b56490a1617a7160abe314df","schema_version":"1.0","event_id":"sha256:ffeed704708399393f0047d03ad5a617fe582ab9b56490a1617a7160abe314df"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:DQACLQSGRZP4MHDOWMJMEHP6Q4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Metallic spin-glasses beyond mean-field: An approach to the impurity-concentration dependence of the freezing temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Eduardo Cuervo-Reyes","submitted_at":"2012-09-05T11:10:40Z","abstract_excerpt":"A relation between the freezing temperature ($T^{}_{\\rm g}$) and the exchange couplings ($J^{}_{ij}$) in metallic spin-glasses is derived, taking the spin-correlations ($G^{}_{ij}$) into account. This approach does not involve a disorder-average. The expansion of the correlations to first order in $J^{}_{ij}/T^{}_{\\rm g}$ leads to the molecular-field result from Thouless-Anderson-Palmer. Employing the current theory of the spin-interaction in disordered metals, an equation for $T^{}_{\\rm g}$ as a function of the concentration of impurities is obtained, which reproduces the available data from "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.0926","kind":"arxiv","version":7},"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":"2026-05-18T03:31:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fVOJfgM1eTfbS03TqOAlyq0ZGQMKHVRn4Wtgf2zt7Ur04OUGA0fNvpulK1VwHA4sXjvccvRseY95hJTGwmY1BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T11:55:14.142687Z"},"content_sha256":"73cdf9e2047ee4ca0142a4ae2aa822331fb80fa600a102ce9bfc6cdf323fcbdb","schema_version":"1.0","event_id":"sha256:73cdf9e2047ee4ca0142a4ae2aa822331fb80fa600a102ce9bfc6cdf323fcbdb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4/bundle.json","state_url":"https://pith.science/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4/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":"2026-06-06T11:55:14Z","links":{"resolver":"https://pith.science/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4","bundle":"https://pith.science/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4/bundle.json","state":"https://pith.science/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DQACLQSGRZP4MHDOWMJMEHP6Q4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:DQACLQSGRZP4MHDOWMJMEHP6Q4","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":"2bff543c534ac7a05705dda509147bd7cc3fc1e713d86f5a4f5d6330fbd22c9b","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-09-05T11:10:40Z","title_canon_sha256":"83dea7b2a5f89c1d09425c917f31c504e7842cc6189fedf8e2ad712bac1ba99e"},"schema_version":"1.0","source":{"id":"1209.0926","kind":"arxiv","version":7}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1209.0926","created_at":"2026-05-18T03:31:32Z"},{"alias_kind":"arxiv_version","alias_value":"1209.0926v7","created_at":"2026-05-18T03:31:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.0926","created_at":"2026-05-18T03:31:32Z"},{"alias_kind":"pith_short_12","alias_value":"DQACLQSGRZP4","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"DQACLQSGRZP4MHDO","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"DQACLQSG","created_at":"2026-05-18T12:27:04Z"}],"graph_snapshots":[{"event_id":"sha256:73cdf9e2047ee4ca0142a4ae2aa822331fb80fa600a102ce9bfc6cdf323fcbdb","target":"graph","created_at":"2026-05-18T03:31:32Z","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":"A relation between the freezing temperature ($T^{}_{\\rm g}$) and the exchange couplings ($J^{}_{ij}$) in metallic spin-glasses is derived, taking the spin-correlations ($G^{}_{ij}$) into account. This approach does not involve a disorder-average. The expansion of the correlations to first order in $J^{}_{ij}/T^{}_{\\rm g}$ leads to the molecular-field result from Thouless-Anderson-Palmer. Employing the current theory of the spin-interaction in disordered metals, an equation for $T^{}_{\\rm g}$ as a function of the concentration of impurities is obtained, which reproduces the available data from ","authors_text":"Eduardo Cuervo-Reyes","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-09-05T11:10:40Z","title":"Metallic spin-glasses beyond mean-field: An approach to the impurity-concentration dependence of the freezing temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.0926","kind":"arxiv","version":7},"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:ffeed704708399393f0047d03ad5a617fe582ab9b56490a1617a7160abe314df","target":"record","created_at":"2026-05-18T03:31:32Z","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":"2bff543c534ac7a05705dda509147bd7cc3fc1e713d86f5a4f5d6330fbd22c9b","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-09-05T11:10:40Z","title_canon_sha256":"83dea7b2a5f89c1d09425c917f31c504e7842cc6189fedf8e2ad712bac1ba99e"},"schema_version":"1.0","source":{"id":"1209.0926","kind":"arxiv","version":7}},"canonical_sha256":"1c0025c2468e5fc61c6eb312c21dfe8717eba1a4e0fc31b0aa8c46a33a12f1ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1c0025c2468e5fc61c6eb312c21dfe8717eba1a4e0fc31b0aa8c46a33a12f1ac","first_computed_at":"2026-05-18T03:31:32.695458Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:31:32.695458Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"HCz1yV3fHueEMp/kKD4G1loGgjFIsGPyKDuy4Ref/b3pXwPC0NWhorB+p2F6Cr86Gd5ZgNvul5qC2z8o5ZzVCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:31:32.696146Z","signed_message":"canonical_sha256_bytes"},"source_id":"1209.0926","source_kind":"arxiv","source_version":7}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ffeed704708399393f0047d03ad5a617fe582ab9b56490a1617a7160abe314df","sha256:73cdf9e2047ee4ca0142a4ae2aa822331fb80fa600a102ce9bfc6cdf323fcbdb"],"state_sha256":"13e9a8f530c1903280a3314b3d3cf84cb3537d478e5702d6c2b5cdf71f47e21e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JKgrtEE5StDqeI7/VXt1RsYeEitP8XlTqQ8RLg2UO5ItckwMliLnAThhiG8BYnHqc0pcwOyOKIA5bOAmbIw4Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T11:55:14.145061Z","bundle_sha256":"23680cc1ec61546f16824946800c8836470a00cad5a5ddf8891b2de28717d118"}}