{"id":178,"date":"2021-02-23T14:45:46","date_gmt":"2021-02-23T20:45:46","guid":{"rendered":"http:\/\/computing.fnal.gov\/lqcd\/?page_id=178"},"modified":"2026-08-25T14:39:46","modified_gmt":"2026-08-25T19:39:46","slug":"allocations","status":"publish","type":"page","link":"https:\/\/computing.fnal.gov\/lqcd\/allocations\/","title":{"rendered":"Allocations"},"content":{"rendered":"\n

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<\/a>” Indico site for details regarding the allocation process.<\/p>\n\n\n\n

2026-2027 Allocations<\/h2>\n\n\n\n

Class A<\/h3>\n\n\n\n
Project Name<\/th>Description<\/th>PI<\/th>Cluster<\/th><\/tr><\/thead>
ahisq<\/td>Lattice generation with anisotropic Highly Improved Staggered Quarks (aHISQ)<\/td>Yannis Trimis<\/td>LQ1<\/td><\/tr>
chargefluct<\/td>Cutoff dependence of higher-order electric-charge fluctuations<\/td>Alexei Bazovov<\/td>LQ2<\/td><\/tr>
csglu27<\/td>Computing the gluon Collins-Soper Kernel with Coulomb-Gauge Operators<\/td>Arthur Avkhadiev<\/td>LQ1
& LQ2<\/td><\/tr>
fourpluseight<\/td>Symmetric mass generation: SU(3) with N_f=8 staggered fermions<\/td>Anna Hasenfratz<\/td>LQ1<\/td><\/tr>
gluonp0<\/td>A Systematic Study of the Renormalization of Gluon PDF and GPD Operators<\/td>Raza Sufian<\/td>LQ2<\/td><\/tr>
lhpc<\/td>Nucleon Quark-Gluon structure with Clover-Wilson Fermions and Domain Wall Fermions<\/td>Michael Engelhardt<\/td>LQ2<\/td><\/tr>
mlgff<\/td>Gravitational form factors of the pion: towards the continuum limit with ML acceleration<\/td>Daniel Hackett<\/td>LQ2<\/td><\/tr>
mslight<\/td>New ensembles for precision projects by the Fermilab lattice and MILC collaborations<\/td>Leon Hostetler<\/td>LQ1<\/td><\/tr>
nclff<\/td>Nucleon Electromagnetic Form Factors at Large Momentum Transfer with Feynman-Hellman Method<\/td>Rui Zhang<\/td>LQ2<\/td><\/tr>
nf10stag<\/td>Conformal fixed point of SU(3) with Nf = 10 flavors using Rooted staggered fermions and PV improved action<\/td>Nathan Mackey<\/td>LQ1<\/td><\/tr>
nf4alphas<\/td>Non-perturbative determination of the strong coupling constant from gradient flow<\/td>Curtis Peterson<\/td>LQ1
& LQ2<\/td><\/tr>
nplqcd<\/td>Nuclear Physics from the Standard Model<\/td>Anthony Grebe<\/td>LQ1
& LQ2<\/td><\/tr>
qcdalpha<\/td>The QCD strong coupling alpha_s at the Z-pole<\/td>Julius Kuti<\/td>LQ2<\/td><\/tr>
stgmugm2<\/td>Conformal fixed point of SU(3) with Nf = 10 flavors using Rooted staggered fermions and PV improved action<\/td>Shaun Lahert<\/td>LQ2<\/td><\/tr>
su2betafn<\/td>Symmetric mass generation with Four SU(2) Doublet Fermions<\/td>Simon Catterall<\/td>LQ1<\/td><\/tr>
taudecay<\/td>Inclusive hadronic decay of the tau lepton<\/td>Matteo Saccardi<\/td>LQ2<\/td><\/tr>
tcrenorm<\/td>Tensor renormalization factors for the HISQ action in four-flavor Lattice QCD<\/td>Abishek Samlodia<\/td>LQ1<\/td><\/tr>
twistedm<\/td>Twist-3 GPDs from Lattice QCD<\/td>Martha Constantinou<\/td>LQ2<\/td><\/tr><\/tbody><\/table>
The PY2026-2027 Type A allocations are for the period from July 1, 2026 through June 30, 2027.<\/figcaption><\/figure>\n\n\n\n

Class B and C<\/h3>\n\n\n\n
Project Name<\/th>Description<\/th>PI<\/th>Type:
Cluster<\/th>		End Date<\/th><\/tr><\/thead>
affine<\/td>Lattice calculation of (conformal) field theories on curved spacetime<\/td>Nobuyuki Matsumoto<\/td>C: LQ2<\/td>26\/08\/12<\/td><\/tr>
betafn<\/td>Test of the Quantum EXpressions lattice field theory framework with Grid backend for offloading work onto CPU and GPU accelerators<\/td>Curtis Peterson<\/td>C: LQ1
C: LQ2<\/td>		26\/08\/04<\/td><\/tr>
gnn<\/td>Performance Scaling of Graph Neural Networks on Lattices<\/td>Huey-Wen Lin<\/td>C: LQ1<\/td>27\/01\/01<\/td><\/tr>
heavylight<\/td>Semileptonic B decays with a vector final state<\/td>Andrew Lytle<\/td>C: LQ2<\/td>26\/08\/20<\/td><\/tr>
lqftml<\/td>Test of Agentic AI infrastructure for data retrieval and workflow script development<\/td>Daniel Hackett<\/span><\/td>C: LQ2<\/td>26\/09\/23<\/td><\/tr>
nptmd<\/td>Computing the gluon Collins-Soper Kernel for TMD Evolution<\/td>Yang Fu<\/td>B: LQ2<\/td>26\/08\/04<\/td><\/tr>
qed3<\/td>Coarse lattice studies of QED3 in Radial Quantization with Overlap Fermions<\/td>Nobuyuki Matsumoto<\/td>B: LQ2<\/span><\/td>26\/11\/21<\/td><\/tr>
quai<\/td>Develop and benchmark efficient quantum gate sets for simulating SU(N) lattice gauge theories using qudits<\/td>Peter Vander Griend<\/td>C: LQ1
C: LQ2<\/td>		26\/11\/05<\/span>
26\/11\/05<\/span><\/td><\/tr>
taudecay<\/td>Inclusive hadronic decay of the tau lepton<\/td>Matteo Saccardi<\/td>C: LQ1<\/td>26\/08\/05<\/td><\/tr>
tensorcgt<\/td>Tensor-network simulation of chiral gauge theories<\/td>Hersh Singh<\/td>C: LQ1
C: LQ2<\/td>		27\/01\/17<\/span>
27\/01\/17<\/td><\/tr><\/tbody><\/table>
Type B and C allocations are typically for 6 months and can start at any time during the year.<\/figcaption><\/figure>\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. 2026-2027 Allocations Class A Project Name Description PI Cluster ahisq Lattice generation with anisotropic Highly Improved Staggered… 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":169,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/178\/revisions"}],"predecessor-version":[{"id":8499,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/178\/revisions\/8499"}],"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}]}}