{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:PXE26547M23Q2X45WC6QAPHY22","short_pith_number":"pith:PXE26547","canonical_record":{"source":{"id":"2604.11646","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-04-13T15:57:34Z","cross_cats_sorted":["hep-ex","hep-th","nucl-ex","nucl-th"],"title_canon_sha256":"2ef6cfc68dda1b30b17084d52c6abb5368a547c16a6cb2e7964dd6dd0c7e476f","abstract_canon_sha256":"ddb3dbcf3734bd9aa05db46cf745c4d576812bb3169a8e11417de321850bc022"},"schema_version":"1.0"},"canonical_sha256":"7dc9af779f66b70d5f9db0bd003cf8d6b43f1891cdd2e6f7c80df51735cf1fd9","source":{"kind":"arxiv","id":"2604.11646","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.11646","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"arxiv_version","alias_value":"2604.11646v2","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.11646","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"pith_short_12","alias_value":"PXE26547M23Q","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"pith_short_16","alias_value":"PXE26547M23Q2X45","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"pith_short_8","alias_value":"PXE26547","created_at":"2026-06-23T03:13:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:PXE26547M23Q2X45WC6QAPHY22","target":"record","payload":{"canonical_record":{"source":{"id":"2604.11646","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-04-13T15:57:34Z","cross_cats_sorted":["hep-ex","hep-th","nucl-ex","nucl-th"],"title_canon_sha256":"2ef6cfc68dda1b30b17084d52c6abb5368a547c16a6cb2e7964dd6dd0c7e476f","abstract_canon_sha256":"ddb3dbcf3734bd9aa05db46cf745c4d576812bb3169a8e11417de321850bc022"},"schema_version":"1.0"},"canonical_sha256":"7dc9af779f66b70d5f9db0bd003cf8d6b43f1891cdd2e6f7c80df51735cf1fd9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-23T03:13:57.214786Z","signature_b64":"b+CK0vZ724mnDBdyDkQcxLmbd1EmBWnDFzDQPDmApb4aiQFEktSRSAy2ZNpMqvXFaXQ7Ol0N8aqUfX6vIut6Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7dc9af779f66b70d5f9db0bd003cf8d6b43f1891cdd2e6f7c80df51735cf1fd9","last_reissued_at":"2026-06-23T03:13:57.214061Z","signature_status":"signed_v1","first_computed_at":"2026-06-23T03:13:57.214061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2604.11646","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-23T03:13:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mk2TMZLLgsksCRDP/rkMfyKHfFysWHM4jXbL0txgFI80JMk5hk5PiIil4I9RYUoDhLkNGphF8ZPfFoHf9OS+Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T23:39:39.185406Z"},"content_sha256":"def41a1beb3bddd652baab5bec532ac644af1e721fa7263c544b5809b9c617c4","schema_version":"1.0","event_id":"sha256:def41a1beb3bddd652baab5bec532ac644af1e721fa7263c544b5809b9c617c4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:PXE26547M23Q2X45WC6QAPHY22","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"This paper supplies the TQ4Q2.0 fragmentation functions for all-heavy tetraquarks in high-energy hadronic collisions.","cross_cats":["hep-ex","hep-th","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"Francesco Giovanni Celiberto","submitted_at":"2026-04-13T15:57:34Z","abstract_excerpt":"We present the TQ4Q2.0 fragmentation functions for the production of all-heavy (fully heavy) $S$-wave tetraquarks ($T_{4Q}$) with scalar ($0^{++}$), axial-vector ($1^{+-}$), and tensor ($2^{++}$) quantum numbers in high-energy hadronic collisions. This work extends the previous TQ4Q1.1 framework by incorporating nonconstituent heavy-quark contributions and introducing a replica-based uncertainty-quantification strategy derived from multi-scale variations (MHOUs). The construction follows a nonrelativistic QCD factorization approach, combining gluon- and heavy-quark-initiated fragmentation chan"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"We present the TQ4Q2.0 fragmentation functions for the production of all-heavy (fully heavy) S-wave tetraquarks (T_{4Q}) with scalar (0^{++}), axial-vector (1^{+-}), and tensor (2^{++}) quantum numbers in high-energy hadronic collisions.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"Initial-scale inputs are modeled through updated potential-inspired wave functions, and the NRQCD factorization framework applies at leading power to these tetraquark states.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"The authors construct and publicly release the TQ4Q2.0 fragmentation functions for all-heavy S-wave tetraquarks via NRQCD factorization, extending prior work with nonconstituent contributions and replica-based uncertainties.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"This paper supplies the TQ4Q2.0 fragmentation functions for all-heavy tetraquarks in high-energy hadronic collisions.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"7cb8e7b69249211f012a5eb27cadea825f1ac27a20087ce1689c72661a0241d8"},"source":{"id":"2604.11646","kind":"arxiv","version":2},"verdict":{"id":"84112211-1d6e-4b8e-89c3-178cc5b60766","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-10T15:10:13.559454Z","strongest_claim":"We present the TQ4Q2.0 fragmentation functions for the production of all-heavy (fully heavy) S-wave tetraquarks (T_{4Q}) with scalar (0^{++}), axial-vector (1^{+-}), and tensor (2^{++}) quantum numbers in high-energy hadronic collisions.","one_line_summary":"The authors construct and publicly release the TQ4Q2.0 fragmentation functions for all-heavy S-wave tetraquarks via NRQCD factorization, extending prior work with nonconstituent contributions and replica-based uncertainties.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"Initial-scale inputs are modeled through updated potential-inspired wave functions, and the NRQCD factorization framework applies at leading power to these tetraquark states.","pith_extraction_headline":"This paper supplies the TQ4Q2.0 fragmentation functions for all-heavy tetraquarks in high-energy hadronic collisions."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2604.11646/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"84112211-1d6e-4b8e-89c3-178cc5b60766"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-23T03:13:57Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aU4SLZ6uaG0PUu/ByLX4SGQSxQE9lpoWRvRqMjc0KNCX51EPh0xLxxqHHoLl9arkDaEyEQkfL5Z9nNLD/odvAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-27T23:39:39.185868Z"},"content_sha256":"b37bb56e851afb6e0f2c53fb145db71c3ee43262ecf42e564ff7ba5e97218617","schema_version":"1.0","event_id":"sha256:b37bb56e851afb6e0f2c53fb145db71c3ee43262ecf42e564ff7ba5e97218617"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PXE26547M23Q2X45WC6QAPHY22/bundle.json","state_url":"https://pith.science/pith/PXE26547M23Q2X45WC6QAPHY22/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PXE26547M23Q2X45WC6QAPHY22/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-27T23:39:39Z","links":{"resolver":"https://pith.science/pith/PXE26547M23Q2X45WC6QAPHY22","bundle":"https://pith.science/pith/PXE26547M23Q2X45WC6QAPHY22/bundle.json","state":"https://pith.science/pith/PXE26547M23Q2X45WC6QAPHY22/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PXE26547M23Q2X45WC6QAPHY22/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:PXE26547M23Q2X45WC6QAPHY22","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ddb3dbcf3734bd9aa05db46cf745c4d576812bb3169a8e11417de321850bc022","cross_cats_sorted":["hep-ex","hep-th","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-04-13T15:57:34Z","title_canon_sha256":"2ef6cfc68dda1b30b17084d52c6abb5368a547c16a6cb2e7964dd6dd0c7e476f"},"schema_version":"1.0","source":{"id":"2604.11646","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2604.11646","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"arxiv_version","alias_value":"2604.11646v2","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2604.11646","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"pith_short_12","alias_value":"PXE26547M23Q","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"pith_short_16","alias_value":"PXE26547M23Q2X45","created_at":"2026-06-23T03:13:57Z"},{"alias_kind":"pith_short_8","alias_value":"PXE26547","created_at":"2026-06-23T03:13:57Z"}],"graph_snapshots":[{"event_id":"sha256:b37bb56e851afb6e0f2c53fb145db71c3ee43262ecf42e564ff7ba5e97218617","target":"graph","created_at":"2026-06-23T03:13:57Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"We present the TQ4Q2.0 fragmentation functions for the production of all-heavy (fully heavy) S-wave tetraquarks (T_{4Q}) with scalar (0^{++}), axial-vector (1^{+-}), and tensor (2^{++}) quantum numbers in high-energy hadronic collisions."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"Initial-scale inputs are modeled through updated potential-inspired wave functions, and the NRQCD factorization framework applies at leading power to these tetraquark states."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"The authors construct and publicly release the TQ4Q2.0 fragmentation functions for all-heavy S-wave tetraquarks via NRQCD factorization, extending prior work with nonconstituent contributions and replica-based uncertainties."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"This paper supplies the TQ4Q2.0 fragmentation functions for all-heavy tetraquarks in high-energy hadronic collisions."}],"snapshot_sha256":"7cb8e7b69249211f012a5eb27cadea825f1ac27a20087ce1689c72661a0241d8"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2604.11646/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present the TQ4Q2.0 fragmentation functions for the production of all-heavy (fully heavy) $S$-wave tetraquarks ($T_{4Q}$) with scalar ($0^{++}$), axial-vector ($1^{+-}$), and tensor ($2^{++}$) quantum numbers in high-energy hadronic collisions. This work extends the previous TQ4Q1.1 framework by incorporating nonconstituent heavy-quark contributions and introducing a replica-based uncertainty-quantification strategy derived from multi-scale variations (MHOUs). The construction follows a nonrelativistic QCD factorization approach, combining gluon- and heavy-quark-initiated fragmentation chan","authors_text":"Francesco Giovanni Celiberto","cross_cats":["hep-ex","hep-th","nucl-ex","nucl-th"],"headline":"This paper supplies the TQ4Q2.0 fragmentation functions for all-heavy tetraquarks in high-energy hadronic collisions.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-04-13T15:57:34Z","title":"All-charm tetraquarks at hadron colliders: A high-precision fragmentation perspective"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2604.11646","kind":"arxiv","version":2},"verdict":{"created_at":"2026-05-10T15:10:13.559454Z","id":"84112211-1d6e-4b8e-89c3-178cc5b60766","model_set":{"reader":"grok-4.3"},"one_line_summary":"The authors construct and publicly release the TQ4Q2.0 fragmentation functions for all-heavy S-wave tetraquarks via NRQCD factorization, extending prior work with nonconstituent contributions and replica-based uncertainties.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"This paper supplies the TQ4Q2.0 fragmentation functions for all-heavy tetraquarks in high-energy hadronic collisions.","strongest_claim":"We present the TQ4Q2.0 fragmentation functions for the production of all-heavy (fully heavy) S-wave tetraquarks (T_{4Q}) with scalar (0^{++}), axial-vector (1^{+-}), and tensor (2^{++}) quantum numbers in high-energy hadronic collisions.","weakest_assumption":"Initial-scale inputs are modeled through updated potential-inspired wave functions, and the NRQCD factorization framework applies at leading power to these tetraquark states."}},"verdict_id":"84112211-1d6e-4b8e-89c3-178cc5b60766"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:def41a1beb3bddd652baab5bec532ac644af1e721fa7263c544b5809b9c617c4","target":"record","created_at":"2026-06-23T03:13:57Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"ddb3dbcf3734bd9aa05db46cf745c4d576812bb3169a8e11417de321850bc022","cross_cats_sorted":["hep-ex","hep-th","nucl-ex","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-04-13T15:57:34Z","title_canon_sha256":"2ef6cfc68dda1b30b17084d52c6abb5368a547c16a6cb2e7964dd6dd0c7e476f"},"schema_version":"1.0","source":{"id":"2604.11646","kind":"arxiv","version":2}},"canonical_sha256":"7dc9af779f66b70d5f9db0bd003cf8d6b43f1891cdd2e6f7c80df51735cf1fd9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7dc9af779f66b70d5f9db0bd003cf8d6b43f1891cdd2e6f7c80df51735cf1fd9","first_computed_at":"2026-06-23T03:13:57.214061Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-23T03:13:57.214061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"b+CK0vZ724mnDBdyDkQcxLmbd1EmBWnDFzDQPDmApb4aiQFEktSRSAy2ZNpMqvXFaXQ7Ol0N8aqUfX6vIut6Dg==","signature_status":"signed_v1","signed_at":"2026-06-23T03:13:57.214786Z","signed_message":"canonical_sha256_bytes"},"source_id":"2604.11646","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:def41a1beb3bddd652baab5bec532ac644af1e721fa7263c544b5809b9c617c4","sha256:b37bb56e851afb6e0f2c53fb145db71c3ee43262ecf42e564ff7ba5e97218617"],"state_sha256":"c8335af6398ea404803df2aac91f2c7890d8ce6f6c1eff2363938c95620c77d6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mMGDLVJWTXMgWFe0OcJWlWUTCtj38nnMge967D46YCmdsKIYpHd/ZwvbiX0mb56/4Eb5ySezLzjTzZuZ3u3ZAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-27T23:39:39.188077Z","bundle_sha256":"4b32907fcc88b7a8de3a8c3c71bed26eb4660f8d507d9aca4b00863ea28715d1"}}