{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:5AKOJAMVKB4ZW3X6UFRIN4OOSJ","short_pith_number":"pith:5AKOJAMV","schema_version":"1.0","canonical_sha256":"e814e4819550799b6efea16286f1ce926354672a8edefe01320b41d024c9389a","source":{"kind":"arxiv","id":"1408.6465","version":3},"attestation_state":"computed","paper":{"title":"$D_{s3}^*(2860)$ and $D_{s1}^*(2860)$ as the 1D $c\\bar{s}$ states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Zhi-Gang Wang","submitted_at":"2014-08-11T02:04:57Z","abstract_excerpt":"In this article, we take the $D_{s3}^*(2860)$ and $D_{s1}^*(2860)$ as the $1^3{\\rm D}_3$ and $1^3{\\rm D}_1$ $c\\bar{s}$ states, respectively, study their strong decays with the heavy meson effective theory by including the chiral symmetry breaking corrections. We can reproduce the experimental data ${\\rm Br}\\left(D_{sJ}^*(2860)\\to D^*K\\right)/{\\rm Br}\\left(D_{sJ}^*(2860)\\to D K\\right) =1.10 \\pm 0.15 \\pm 0.19$ with suitable hadronic coupling constants, the assignment of the $D_{sJ}^*(2860)$ as the $D_{s3}^*(2860)$ is favored, the chiral symmetry breaking corrections are large. Furthermore, we ob"},"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":"1408.6465","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-11T02:04:57Z","cross_cats_sorted":[],"title_canon_sha256":"95e26a567c77475481e560f03fbd9bf5a704eb0b64e408a6e832603ac8aa4cd1","abstract_canon_sha256":"2387ac7d0df35c28bede3fbc036c5cbc3dcef5da9f254096742d721b141fc896"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:28:47.637677Z","signature_b64":"2q/UPpBnHMV3Mss4C/iHAns5Ug1oGP8gnvn8xFwGgfEqneqhvXOgZcZywlmpllw8lpER4i2QB7OEnRzMC39LDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e814e4819550799b6efea16286f1ce926354672a8edefe01320b41d024c9389a","last_reissued_at":"2026-05-18T02:28:47.637301Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:28:47.637301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$D_{s3}^*(2860)$ and $D_{s1}^*(2860)$ as the 1D $c\\bar{s}$ states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Zhi-Gang Wang","submitted_at":"2014-08-11T02:04:57Z","abstract_excerpt":"In this article, we take the $D_{s3}^*(2860)$ and $D_{s1}^*(2860)$ as the $1^3{\\rm D}_3$ and $1^3{\\rm D}_1$ $c\\bar{s}$ states, respectively, study their strong decays with the heavy meson effective theory by including the chiral symmetry breaking corrections. We can reproduce the experimental data ${\\rm Br}\\left(D_{sJ}^*(2860)\\to D^*K\\right)/{\\rm Br}\\left(D_{sJ}^*(2860)\\to D K\\right) =1.10 \\pm 0.15 \\pm 0.19$ with suitable hadronic coupling constants, the assignment of the $D_{sJ}^*(2860)$ as the $D_{s3}^*(2860)$ is favored, the chiral symmetry breaking corrections are large. 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