{"work":{"id":"4deaf489-c81b-4322-bb0a-41188b0ad4db","openalex_id":"https://openalex.org/W4299516620","doi":"10.1103/physrevlett","arxiv_id":null,"raw_key":null,"title":"Burdick, and Benjamin L","authors":null,"authors_text":"Mingwu Lu, Nathaniel Q","year":2012,"venue":"HAL (Le Centre pour la Communication Scientifique Directe)","abstract":null,"external_url":"https://doi.org/10.1103/physrevlett","cited_by_count":728,"metadata_source":"openalex","metadata_fetched_at":"2026-08-05T02:28:24.338817+00:00","pith_arxiv_id":null,"created_at":"2026-05-08T17:03:33.499414+00:00","updated_at":"2026-08-05T02:28:24.338817+00:00","title_quality_ok":false,"display_title":"Physical Review Letters 85(10), 2200–2203 (2000)","render_title":"Physical Review Letters 85(10), 2200–2203 (2000)"},"hub":{"state":{"work_id":"4deaf489-c81b-4322-bb0a-41188b0ad4db","tier":"super_hub","tier_reason":"100+ Pith inbound or 10,000+ external citations","pith_inbound_count":278,"external_cited_by_count":728,"distinct_field_count":48,"first_pith_cited_at":"2019-06-19T15:43:07+00:00","last_pith_cited_at":"2026-07-09T06:08:43+00:00","author_build_status":"needed","summary_status":"needed","contexts_status":"needed","graph_status":"needed","ask_index_status":"needed","reader_status":"not_needed","recognition_status":"not_needed","updated_at":"2026-08-22T17:59:23.829162+00:00","tier_text":"super_hub"},"tier":"super_hub","role_counts":[{"context_role":"background","n":86},{"context_role":"method","n":8},{"context_role":"baseline","n":2}],"polarity_counts":[{"context_polarity":"background","n":84},{"context_polarity":"use_method","n":7},{"context_polarity":"baseline","n":2},{"context_polarity":"support","n":2},{"context_polarity":"unclear","n":1}],"runs":{"ask_index":{"job_type":"ask_index","status":"succeeded","result":{"title":"Quantum Fingerprinting","claims":[{"claim_text":"(50) in different ways reveals how various orbitals are correlated with one another within the nuclear state. This type of orbital entanglement, formulated in Fock space, has been shown to be relevant for systems of identical fermions, as it circumvents partitioning ambiguities arising from the anti-symmetrized tensor-product structure of the underlying Hilbert space [284]. Moreover, it is the natural notion of entanglement in the context of classical configuration-interaction methods, such as t","claim_type":"background","confidence":0.85,"evidence_strength":"citation_context"},{"claim_text":"This phenomenon was interpreted as a signature of deconfinement, 31 arising from color screening in the QGP [169]. However, interactions with the medium constituents can strongly modify quarkonium yields and survival probabilities. In this context, open-charm mesons play an important role, as their thermal modifications may affect charmonium absorption through scattering with comoving hadrons [170, 171, 172]. Moreover, the heavy-quark potential, which is central for the theoretical description o","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"},{"claim_text":"In 2021, the same experiment reported the first evidence for a strange charmonium-like pentaquark, 𝑃𝑐𝑠(4459), seen in the𝐽∕𝜓+ Λspectrum from[Ξ − 𝑏 →𝐽∕𝜓+ Λ +𝐾 −]decays [106]. A year later, in 2022, the 𝑃 Λ 𝜓𝑠 (4338)resonance was observed in flavor-untagged[𝐵− →𝐽∕𝜓+𝑝+̄ 𝑝]decays [107]. Additional experimental studies on the𝑃𝑐 sector can be found in Refs. [108, 109]. Despite significant advances in identifying mass spectra and decay modes of exotic baryons, the underlying mechanisms responsible for ","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"}],"why_cited":"Pith tracks Quantum Fingerprinting because it crossed a citation-hub threshold. Current citing contexts most often use it as background evidence (3 contexts).","role_counts":[{"n":3,"context_role":"background"}]},"error":null,"updated_at":"2026-05-14T19:36:22.479135+00:00"},"author_expand":{"job_type":"author_expand","status":"succeeded","result":{"authors_linked":[{"id":"fbeae6cf-f1aa-414c-8871-7056f33c24cc","orcid":null,"display_name":"Zhang"}]},"error":null,"updated_at":"2026-05-14T19:36:22.588074+00:00"},"context_extract":{"job_type":"context_extract","status":"succeeded","result":{"enqueued_papers":25},"error":null,"updated_at":"2026-05-14T18:29:30.189373+00:00"},"graph_features":{"job_type":"graph_features","status":"succeeded","result":{"co_cited":[{"title":"Pattern Recognition 127 (2022), 108611","work_id":"238df2e4-a3e5-46f3-860e-3ae2b0094b97","shared_citers":22},{"title":"H., Jedamzik, K., & Pogosian, L","work_id":"aa5a5821-cbcf-44c7-b743-a852432392bd","shared_citers":17},{"title":"Available: https://link.aps.org/doi/10.1103/PhysRevA","work_id":"7622cbba-e948-42e0-8cd2-290ad3793bc2","shared_citers":15},{"title":"M.et al.Tunability of the topological nodal-line semimetal phase in ZrSiX-type materials (X = S, Se, Te).Physical Review B95, 161101 (2017)","work_id":"0e1cfea8-2230-4913-91c7-a8ac9eb1a51d","shared_citers":12},{"title":"Nuclear ab initio calculations of 6He β -decay for beyond the Standard Model studies","work_id":"f5512874-0e46-48e3-86b0-58f135f8e424","shared_citers":9},{"title":"Lewis, W","work_id":"bf7f3f64-80c5-4847-8cb1-3a6dbe2cdf14","shared_citers":7},{"title":"Tenenbaum, Vin de Silva, and John C","work_id":"656f6b47-9c8d-489d-af8f-5d0f17981423","shared_citers":6},{"title":"URLhttps://doi.org/10.48550/arXiv","work_id":"5c2060c6-427c-4321-be22-49ccae439d80","shared_citers":6},{"title":"Electromagnetic effects and weak form factors","work_id":"452a5ae5-edd9-4748-acb9-24dae2cec95e","shared_citers":5},{"title":"High precision analytical description of the allowed beta spectrum shape","work_id":"c7a35325-19cf-4f42-9c2f-173687729ec9","shared_citers":5},{"title":"Quantum Computing in the NISQ era and beyond","work_id":"db02914e-62e0-4457-a74e-836513460506","shared_citers":5},{"title":"SIAM Journal on Computing26(5), 1484–1509 (1997) https: //doi.org/10.1137/s0097539795293172","work_id":"8c114c19-82cb-47cf-98f7-484a0ef818f7","shared_citers":5},{"title":"G., Yuan, W., Macri, L","work_id":"ec2ceb71-84c6-42f9-8595-7d02bd369ca8","shared_citers":4},{"title":"Hasenbusch, Dynamic critical exponent z of the three-dimensional ising universality class: Monte carlo simulations of the improved blume-capel model, Phys","work_id":"c78d9447-3703-41df-964c-28f4f69acd5a","shared_citers":4},{"title":"Horodecki, P","work_id":"c6753c9b-4b5d-4aef-83f8-c568b2ee340a","shared_citers":4},{"title":"In: Samuel J","work_id":"1e2e43d5-a734-41b6-a5cc-6e1c0d46b56a","shared_citers":4},{"title":"Lorentz Invariance and the Kinematic Structure of V ertex Functions","work_id":"ececf8d2-c38b-4cca-9905-51d364a7f169","shared_citers":4},{"title":"M., Crawford, T","work_id":"dacf65ad-e19b-4a01-96f6-621ad3f94b3a","shared_citers":4},{"title":"Petreczky and J","work_id":"bad00e9e-5a71-4ae3-b3f2-8aef76f60efa","shared_citers":4},{"title":"Przybylska, A","work_id":"9de06f05-6495-4577-8e82-a375f06e87b9","shared_citers":4},{"title":"Relativistic continuous matrix product states for quantum fields without cutoff.Phys","work_id":"32ff0a4d-a56d-4db2-a8d6-5ad8ca0dcec8","shared_citers":4},{"title":"94, 029901 (2022)].arXiv:1705.00141,doi:10.1103/RevModPhys.90.015004","work_id":"5ffae003-6528-459e-bfef-302998e553a8","shared_citers":3},{"title":"Aaij, et al., Observation of a J/ψΛResonance Consistent with a Strange Pentaquark Candidate in B-→J/ψΛp¯Decays, Phys","work_id":"e8e48350-e8bc-46dc-b2db-27f689c5d1ae","shared_citers":3},{"title":"Aaij, et al., Observation of a narrow pentaquark state,Pc(4312)+, and of two-peak structure of thePc(4450)+, Phys","work_id":"ad98d413-58ae-43ad-80f9-2ad3d318698d","shared_citers":3}],"time_series":[{"n":1,"year":2025},{"n":97,"year":2026}],"dependency_candidates":[]},"error":null,"updated_at":"2026-05-14T18:29:34.397712+00:00"},"identity_refresh":{"job_type":"identity_refresh","status":"succeeded","result":{"items":[{"title":"Qwen3 Technical Report","outcome":"unchanged","work_id":"25a4e30c-1232-48e7-9925-02fa12ba7c9e","resolver":"local_arxiv","confidence":0.98,"old_work_id":"25a4e30c-1232-48e7-9925-02fa12ba7c9e"}],"counts":{"fixed":0,"merged":0,"unchanged":1,"quarantined":0,"needs_external_resolution":0},"errors":[],"attempted":1},"error":null,"updated_at":"2026-05-14T18:30:04.587381+00:00"},"role_polarity":{"job_type":"role_polarity","status":"succeeded","result":{"title":"Quantum Fingerprinting","claims":[{"claim_text":"(50) in different ways reveals how various orbitals are correlated with one another within the nuclear state. This type of orbital entanglement, formulated in Fock space, has been shown to be relevant for systems of identical fermions, as it circumvents partitioning ambiguities arising from the anti-symmetrized tensor-product structure of the underlying Hilbert space [284]. Moreover, it is the natural notion of entanglement in the context of classical configuration-interaction methods, such as t","claim_type":"background","confidence":0.85,"evidence_strength":"citation_context"},{"claim_text":"This phenomenon was interpreted as a signature of deconfinement, 31 arising from color screening in the QGP [169]. However, interactions with the medium constituents can strongly modify quarkonium yields and survival probabilities. In this context, open-charm mesons play an important role, as their thermal modifications may affect charmonium absorption through scattering with comoving hadrons [170, 171, 172]. Moreover, the heavy-quark potential, which is central for the theoretical description o","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"},{"claim_text":"In 2021, the same experiment reported the first evidence for a strange charmonium-like pentaquark, 𝑃𝑐𝑠(4459), seen in the𝐽∕𝜓+ Λspectrum from[Ξ − 𝑏 →𝐽∕𝜓+ Λ +𝐾 −]decays [106]. A year later, in 2022, the 𝑃 Λ 𝜓𝑠 (4338)resonance was observed in flavor-untagged[𝐵− →𝐽∕𝜓+𝑝+̄ 𝑝]decays [107]. Additional experimental studies on the𝑃𝑐 sector can be found in Refs. [108, 109]. Despite significant advances in identifying mass spectra and decay modes of exotic baryons, the underlying mechanisms responsible for ","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"}],"why_cited":"Pith tracks Quantum Fingerprinting because it crossed a citation-hub threshold. Current citing contexts most often use it as background evidence (3 contexts).","role_counts":[{"n":3,"context_role":"background"}]},"error":null,"updated_at":"2026-05-14T19:36:22.483363+00:00"},"summary_claims":{"job_type":"summary_claims","status":"succeeded","result":{"title":"Quantum Fingerprinting","claims":[{"claim_text":"This phenomenon was interpreted as a signature of deconfinement, 31 arising from color screening in the QGP [169]. However, interactions with the medium constituents can strongly modify quarkonium yields and survival probabilities. In this context, open-charm mesons play an important role, as their thermal modifications may affect charmonium absorption through scattering with comoving hadrons [170, 171, 172]. Moreover, the heavy-quark potential, which is central for the theoretical description o","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"},{"claim_text":"In 2021, the same experiment reported the first evidence for a strange charmonium-like pentaquark, 𝑃𝑐𝑠(4459), seen in the𝐽∕𝜓+ Λspectrum from[Ξ − 𝑏 →𝐽∕𝜓+ Λ +𝐾 −]decays [106]. A year later, in 2022, the 𝑃 Λ 𝜓𝑠 (4338)resonance was observed in flavor-untagged[𝐵− →𝐽∕𝜓+𝑝+̄ 𝑝]decays [107]. Additional experimental studies on the𝑃𝑐 sector can be found in Refs. [108, 109]. Despite significant advances in identifying mass spectra and decay modes of exotic baryons, the underlying mechanisms responsible for ","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"}],"why_cited":"Pith tracks Quantum Fingerprinting because it crossed a citation-hub threshold. Current citing contexts most often use it as background evidence (2 contexts).","role_counts":[{"n":2,"context_role":"background"}]},"error":null,"updated_at":"2026-05-14T18:29:34.403670+00:00"}},"summary":{"title":"Quantum Fingerprinting","claims":[{"claim_text":"This phenomenon was interpreted as a signature of deconfinement, 31 arising from color screening in the QGP [169]. However, interactions with the medium constituents can strongly modify quarkonium yields and survival probabilities. In this context, open-charm mesons play an important role, as their thermal modifications may affect charmonium absorption through scattering with comoving hadrons [170, 171, 172]. Moreover, the heavy-quark potential, which is central for the theoretical description o","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"},{"claim_text":"In 2021, the same experiment reported the first evidence for a strange charmonium-like pentaquark, 𝑃𝑐𝑠(4459), seen in the𝐽∕𝜓+ Λspectrum from[Ξ − 𝑏 →𝐽∕𝜓+ Λ +𝐾 −]decays [106]. A year later, in 2022, the 𝑃 Λ 𝜓𝑠 (4338)resonance was observed in flavor-untagged[𝐵− →𝐽∕𝜓+𝑝+̄ 𝑝]decays [107]. Additional experimental studies on the𝑃𝑐 sector can be found in Refs. [108, 109]. Despite significant advances in identifying mass spectra and decay modes of exotic baryons, the underlying mechanisms responsible for ","claim_type":"background","confidence":0.8,"evidence_strength":"citation_context"}],"why_cited":"Pith tracks Quantum Fingerprinting because it crossed a citation-hub threshold. Current citing contexts most often use it as background evidence (2 contexts).","role_counts":[{"n":2,"context_role":"background"}]},"graph":{"co_cited":[{"title":"Pattern Recognition 127 (2022), 108611","work_id":"238df2e4-a3e5-46f3-860e-3ae2b0094b97","shared_citers":22},{"title":"H., Jedamzik, K., & Pogosian, L","work_id":"aa5a5821-cbcf-44c7-b743-a852432392bd","shared_citers":17},{"title":"Available: https://link.aps.org/doi/10.1103/PhysRevA","work_id":"7622cbba-e948-42e0-8cd2-290ad3793bc2","shared_citers":15},{"title":"M.et al.Tunability of the topological nodal-line semimetal phase in ZrSiX-type materials (X = S, Se, Te).Physical Review B95, 161101 (2017)","work_id":"0e1cfea8-2230-4913-91c7-a8ac9eb1a51d","shared_citers":12},{"title":"Nuclear ab initio calculations of 6He β -decay for beyond the Standard Model studies","work_id":"f5512874-0e46-48e3-86b0-58f135f8e424","shared_citers":9},{"title":"Lewis, W","work_id":"bf7f3f64-80c5-4847-8cb1-3a6dbe2cdf14","shared_citers":7},{"title":"Tenenbaum, Vin de Silva, and John C","work_id":"656f6b47-9c8d-489d-af8f-5d0f17981423","shared_citers":6},{"title":"URLhttps://doi.org/10.48550/arXiv","work_id":"5c2060c6-427c-4321-be22-49ccae439d80","shared_citers":6},{"title":"Electromagnetic effects and weak form factors","work_id":"452a5ae5-edd9-4748-acb9-24dae2cec95e","shared_citers":5},{"title":"High precision analytical description of the allowed beta spectrum shape","work_id":"c7a35325-19cf-4f42-9c2f-173687729ec9","shared_citers":5},{"title":"Quantum Computing in the NISQ era and beyond","work_id":"db02914e-62e0-4457-a74e-836513460506","shared_citers":5},{"title":"SIAM Journal on Computing26(5), 1484–1509 (1997) https: //doi.org/10.1137/s0097539795293172","work_id":"8c114c19-82cb-47cf-98f7-484a0ef818f7","shared_citers":5},{"title":"G., Yuan, W., Macri, L","work_id":"ec2ceb71-84c6-42f9-8595-7d02bd369ca8","shared_citers":4},{"title":"Hasenbusch, Dynamic critical exponent z of the three-dimensional ising universality class: Monte carlo simulations of the improved blume-capel model, Phys","work_id":"c78d9447-3703-41df-964c-28f4f69acd5a","shared_citers":4},{"title":"Horodecki, P","work_id":"c6753c9b-4b5d-4aef-83f8-c568b2ee340a","shared_citers":4},{"title":"In: Samuel J","work_id":"1e2e43d5-a734-41b6-a5cc-6e1c0d46b56a","shared_citers":4},{"title":"Lorentz Invariance and the Kinematic Structure of V ertex Functions","work_id":"ececf8d2-c38b-4cca-9905-51d364a7f169","shared_citers":4},{"title":"M., Crawford, T","work_id":"dacf65ad-e19b-4a01-96f6-621ad3f94b3a","shared_citers":4},{"title":"Petreczky and J","work_id":"bad00e9e-5a71-4ae3-b3f2-8aef76f60efa","shared_citers":4},{"title":"Przybylska, A","work_id":"9de06f05-6495-4577-8e82-a375f06e87b9","shared_citers":4},{"title":"Relativistic continuous matrix product states for quantum fields without cutoff.Phys","work_id":"32ff0a4d-a56d-4db2-a8d6-5ad8ca0dcec8","shared_citers":4},{"title":"94, 029901 (2022)].arXiv:1705.00141,doi:10.1103/RevModPhys.90.015004","work_id":"5ffae003-6528-459e-bfef-302998e553a8","shared_citers":3},{"title":"Aaij, et al., Observation of a J/ψΛResonance Consistent with a Strange Pentaquark Candidate in B-→J/ψΛp¯Decays, Phys","work_id":"e8e48350-e8bc-46dc-b2db-27f689c5d1ae","shared_citers":3},{"title":"Aaij, et al., Observation of a narrow pentaquark state,Pc(4312)+, and of two-peak structure of thePc(4450)+, Phys","work_id":"ad98d413-58ae-43ad-80f9-2ad3d318698d","shared_citers":3}],"time_series":[{"n":1,"year":2025},{"n":97,"year":2026}],"dependency_candidates":[]},"authors":[{"id":"fbeae6cf-f1aa-414c-8871-7056f33c24cc","orcid":null,"display_name":"Zhang","source":"manual","import_confidence":0.72}]}}