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Following our previous work [M.~Lepers \\textit{et.~al.}, Phys.~Rev.~A \\textbf{88}, 032709 (2013)] we use the sum-over-state formula inherent to the second-order perturbation theory, composed of the contributions from the transitions within "},"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":"1502.05636","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-02-19T17:23:28Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"40f2428865fc58d15640602c7e0d709c554668a49afd245403e11d9d4c0804a7","abstract_canon_sha256":"7814d00a8ed5882e309d5b9041347b8633bcadcf5b030e7bdd1ea6f618cb4f4d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:26:45.927568Z","signature_b64":"8MkSHAIIcFV2Sl9LN4thivgpKRFDzg/HQNfagPPB7Q4YJvxmKgKYt1IyeeBaEzbh/uuCb2/wZ12FTCOI6TVQBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39a0068d4927fac3c55bc8e50bbf8dc96229cd73fbd8141e5f4aadb1c55f7645","last_reissued_at":"2026-05-18T02:26:45.927081Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:26:45.927081Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Long-range interactions between polar bialkali ground-state molecules in arbitrary vibrational levels","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"M. 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