Project Name<\/strong><\/td>Description<\/strong><\/td>Type<\/strong><\/td>PI<\/strong><\/td>| Ends<\/td><\/tr> | | 4fermi<\/td> | Mirror model with reduced staggered fermions<\/td> | A<\/td> | Catterall<\/td> | <\/td><\/tr> | | ahisq<\/td> | Novel anisotropic pure gauge simulations and the spectrum of anisotropic staggered quarks<\/td> | A<\/td> | Bazavov<\/td> | <\/td><\/tr> | | chiqcd<\/td> | Lattice calculation of nucleon energy-momentum tensor form factors using overlap fermions<\/td> | A<\/td> | Wang<\/td> | <\/td><\/tr> | | fourpluseight<\/td> | Gradient flow $\\beta$ function for 6 fundamental flavors<\/td> | A<\/td> | Hasenfratz<\/td> | <\/td><\/tr> | | hadstruc<\/td> | Parton Distribution Functions and Amplitudes…<\/td> | A<\/td> | Richards<\/td> | <\/td><\/tr> | | heavylight<\/td> | Semileptonic B- and D-meson form factors with high precision<\/td> | A<\/td> | Jay<\/td> | <\/td><\/tr> | | lp3<\/td> | Precision Moments of Strange Parton Distribution Functions from Lattice QCD.<\/td> | A<\/td> | Lin<\/td> | <\/td><\/tr> | | mslight<\/td> | New ensembles for precision light-meson decay constants.<\/td> | A<\/td> | Bazavov<\/td> | <\/td><\/tr> | | nplqcd<\/td> | Nuclear Physics from the Standard Model<\/td> | A<\/td> | Shanahan<\/td> | <\/td><\/tr> | | rhqbbar<\/td> | Semi-leptonic B-decays with physical light quarks.<\/td> | A<\/td> | Soni<\/td> | <\/td><\/tr> | | comphiggs<\/td> | Mapping the parameter space of the 4+4 model<\/td> | B<\/td> | Neil<\/td> | 2022-04-01<\/td><\/tr> | | gluonpdf<\/td> | Gluon Parton Distribution of the Pion from Lattice QCD<\/td> | B<\/td> | Lin<\/td> | 2022-07-01<\/td><\/tr> | | hadtensor<\/td> | Computing four-point correlation functions which are related to the structure functions of the pion<\/td> | B<\/td> | Jay<\/td> | 2022-01-01<\/td><\/tr> | | qfenpct<\/td> | Non-perturbative renormalization of critical phi4 theory on S2<\/td> | B<\/td> | Owen<\/td> | 2022-01-01<\/td><\/tr> | | hisqvec<\/td> | Pilot studies of semileptonic decays involving a vector final state<\/td> | C<\/td> | Lytle<\/td> | 2022-07-01<\/td><\/tr> | | hotqcdhisq<\/td> | Hot QCD with HISQ action<\/td> | C<\/td> | Petreczky<\/td> | 2022-04-13<\/td><\/tr> | | largenc<\/td> | Properties of QCD with more than three colors<\/td> | C<\/td> | DeGrand<\/td> | 2022-05-01<\/td><\/tr> | | stggm2dev<\/td> | Staggered Muon g-2<\/td> | C<\/td> | Detar<\/td> | 2021-10-01<\/td><\/tr> | | vaccumdecay<\/td> | A study of metastable vacuum decay, a nonperturbative phenomenon that occurs in real-time<\/td> | C<\/td> | El-Khadra<\/td> | 2021-04-01<\/td><\/tr><\/tbody><\/table>The PY 2021-2022 Type A allocations were for the period from July 1, 2021, through June 30, 2022.<\/figcaption><\/figure>\n\n\n\n <\/p>\n\n\n\n Previous: 2020-2021 Allocations<\/h3>\n\n\n\nThe table below lists the expired type A projects allocated time on the Fermilab USQCD clusters by the Scientific Program Committee. These projects still have opportunistic access to the SLURM batch scheduler and limited storage space.<\/p>\n\n\n\nProject Name<\/strong><\/td>Description<\/strong><\/td>Type<\/strong><\/td>PI<\/strong><\/td><\/tr>| chiqcd<\/td> | Neutrino Nucleon Scattering and Hadronic Tensor<\/td> | A<\/td> | Liu<\/td><\/tr> | | hadstruc<\/td> | Parton Distribution Functions and Amplitudes.<\/td> | A<\/td> | Richards<\/td><\/tr> | | lp3<\/td> | Precision Moments of Strange Parton Distribution Functions from Lattice QCD.<\/td> | A<\/td> | Lin<\/td><\/tr> | | mslight<\/td> | New ensembles for precision light-meson decay constants.<\/td> | A<\/td> | Bazavov<\/td><\/tr> | | nedm<\/td> | Contribution of Theta, cEDM and Weinberg operators to nEDM.<\/td> | A<\/td> | Bhattacharya<\/td><\/tr> | | nme<\/td> | Nucleon Matrix Elements with 2+1 flavor clover fermions,<\/td> | A<\/td> | Gupta<\/td><\/tr> | | rhqbbar<\/td> | Semi-leptonic B-decays with physical light quarks.<\/td> | A<\/td> | Soni<\/td><\/tr> | | vcbok<\/td> | Determination of Vcb from Semi-leptonic Decays B \u2192 D(\u2217)using the Oktay\u2013Kronfeld Action.<\/td> | A<\/td> | Jang<\/td><\/tr><\/tbody><\/table>The 2020-2021 allocations were for the period from July 1, 2020 through June 30, 2021.<\/figcaption><\/figure>\n\n\n\n Note: The project names listed in the table above have to be specified when submitting jobs on the Fermilab USQCD clusters. For any questions or concerns please email us at hpc-admin@fnal.gov<\/a> <\/p>\n\n\n\n<\/p>\n","protected":false},"excerpt":{"rendered":" The table below lists active type A, B, and C projects allocated time on the Fermilab USQCD clusters by the Scientific Program Committee. Please refer to the “USQCD All-Hands Meeting” Indico site for details regarding the allocation process. Current: 2025-2026 Allocations Project Name Description PI Type: Cluster End Date affine Lattice calculation of (conformal) field… More »<\/a><\/p>\n","protected":false},"author":16,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-178","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/178","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/users\/16"}],"replies":[{"embeddable":true,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/comments?post=178"}],"version-history":[{"count":99,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/178\/revisions"}],"predecessor-version":[{"id":7912,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/178\/revisions\/7912"}],"wp:attachment":[{"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/media?parent=178"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}} | | | | |
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