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r^\\prime| \\rightarrow +\\infty$, even though both $| \\Omega\\rangle$ and $| \\Psi\\rangle$ are quantum disordered states with short-range correlation. $\\phi(r)"},"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":"1312.0626","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-12-02T21:11:16Z","cross_cats_sorted":[],"title_canon_sha256":"2652ec73cb49f0b9766ce800c703849d6ae69a45e088baa6c1e3d4409a9189cd","abstract_canon_sha256":"7698fed325d25b5fbe65d6011c124c34ec777433784e1509538ac0bba36c8424"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:35:40.497472Z","signature_b64":"l4ty+nHHnyoKQRTucWtdJLOqJxogaRPg5GPc0LKX2NoTBE9z0EA4Ii5t4xfVSaCnhTmAFeqAzSoL110q/2EVAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ba4991e885fbb8ec4074f18dfa96eab234cb8652f1e60389f3de430beb28ff2c","last_reissued_at":"2026-05-18T01:35:40.496754Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:35:40.496754Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wave Function and Strange Correlator of Short Range Entangled states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Alex Rasmussen, Cenke Xu, Kevin Slagle, Yi-Zhuang You, Zhen Bi","submitted_at":"2013-12-02T21:11:16Z","abstract_excerpt":"We demonstrate the following conclusion: If $|\\Psi\\rangle$ is a $1d$ or $2d$ nontrivial short range entangled state, and $|\\Omega \\rangle$ is a trivial disordered state defined on the same Hilbert space, then the following quantity (so called strange correlator) $C(r, r^\\prime) = \\frac{\\langle \\Omega|\\phi(r) \\phi(r^\\prime) | \\Psi\\rangle}{\\langle \\Omega| \\Psi\\rangle}$ either saturates to a constant or decays as a power-law in the limit $|r - 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