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The production of $J/\\Psi$'s is based on the Lund string fragmentation model, while its interactions with hadrons are included by conventional cascade-type two-body collisions. Adopting 6 mb for the $J/\\Psi$-baryon cross sections and 3 mb for the $J/\\Psi$-meson cross sections above the $D\\bar{D}$ threshold, we find"},"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":"nucl-th/9609025","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1996-09-10T14:36:26Z","cross_cats_sorted":[],"title_canon_sha256":"4d6e16fbb19ba8cba1c8672ea17fdc400e9fe781d35975a1eed86da1af9769f3","abstract_canon_sha256":"7d717a1b11c810186dfd7a6d796d30f21eb582fd46c09f475a5c9e8aba015b80"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:18.482523Z","signature_b64":"vcWYrPVynsM00ErWu5M+XJf/1BrdhKxFlDe+LlHiOPJ0MCdde1S5h+wduNP/S3NJ59eIb3l9S7awYLX+wdpwAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4218f3ab2f8b24251d8bcda8bd1ed8c7bcc00a1824b916c657fd60ca63dacff2","last_reissued_at":"2026-05-18T01:05:18.482018Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:18.482018Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$J/\\Psi$ suppression in nuclear collisions at SPS energies","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"C.M. 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