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The calculation of bond chaos then shows that the scaling of the free energy fluctuaions with system size $N$ is $\\Delta F \\sim N^\\mu$ with ${1/5}\\leq\\mu <{3/10}$, and very likely $\\mu={1}{5}$ exactly."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1001.0893","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-01-06T14:06:29Z","cross_cats_sorted":[],"title_canon_sha256":"21865272e0c5a70f5c58c443ac00331d98711a5a3b2c7721efcf0340d2904f03","abstract_canon_sha256":"3c60d976d8b7f700e457580b82b80adf24f54a079939b9897373d488a91eb23b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:49.605899Z","signature_b64":"TjFCN0QGB/rLbS/3vJk3Ji2VcoB6fNFOM67IAWHHuHYoPWdmOnAE5XadYjF4dd8ll3eSjg/gU67lmqLMA++ZBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1f3ed06f0496677a8dc2f6834203281d56c4796f6bd67e1d1cd08bdc9064c009","last_reissued_at":"2026-05-18T03:23:49.605400Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:49.605400Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sample-to-sample fluctuations and bond chaos in the $m$-component spin glass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"A. 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