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The masses and current couplings of these diquark-antidiquark states are calculated by means of two-point correlation functions and taking into account the vacuum condensates up to eight dimensions. To compute the strong couplings of $Z_{\\overline{c}s}$ states with $D,\\ D_{s},\\ D^{\\ast},\\ D_{s}^{\\ast},\\ D_{s1}(2460),\\ D_{s0}^{\\ast}(2317),\\ \\pi$ and $K$ mesons we"},"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":"1710.01971","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-05T11:31:46Z","cross_cats_sorted":["hep-ex","hep-lat"],"title_canon_sha256":"eafbfaff1743e68b8c7eafb770ad9610074ab8940d4ff8c0d086e841572ee261","abstract_canon_sha256":"68d8e296b0ae68d8175324a07c1cea1d9aa09ba2ca9c280c0ec14c7f9d8171ae"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:26.396281Z","signature_b64":"NOMFAGe/QDcYEzXWk1UIVts6U6GzDF9kIt/oLig6LywC+4H1GltaAb0ydxlKXhhFYPm1bd9T/x0oHvn+KpYWDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04f4607586c4d3d4a62f03a739b079e3d8b47e01f5e7ebde23a57a652001e332","last_reissued_at":"2026-05-18T00:19:26.395746Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:26.395746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Testing the doubly charged charm-strange tetraquarks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","hep-lat"],"primary_cat":"hep-ph","authors_text":"H. 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