{"id":8457,"date":"2026-08-25T14:28:19","date_gmt":"2026-08-25T19:28:19","guid":{"rendered":"https:\/\/computing.fnal.gov\/lqcd\/?page_id=8457"},"modified":"2026-08-25T14:40:40","modified_gmt":"2026-08-25T19:40:40","slug":"previous-allocations","status":"publish","type":"page","link":"https:\/\/computing.fnal.gov\/lqcd\/previous-allocations\/","title":{"rendered":"Previous Years’ Allocations"},"content":{"rendered":"\n

2025-2026 Allocations<\/h3>\n\n\n\n
Project Name<\/strong><\/td>Description<\/strong><\/td>PI<\/strong><\/td>Type<\/strong>: Cluster<\/strong> <\/td>End Date<\/strong><\/td><\/tr>
affine<\/td>Lattice calculation of (conformal) field theories on curved spacetime<\/td>Nobuyuki Matsumoto<\/td>C: LQ1<\/td>26\/07\/01<\/td><\/tr>
ahisq<\/td>Novel anisotropic pure gauge simulations and the spectrum of anisotropic staggered quarks<\/td>Yannis Trimis<\/td>A: LQ1<\/td>26\/07\/01<\/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\/07\/01<\/td><\/tr>
chargefluct<\/td>Cutoff dependence of higher-order electric-charge fluctuations<\/td>David Clarke<\/td>A: LQ2<\/td>26\/07\/01<\/td><\/tr>
chiqcd<\/td>Lattice calculation of QCD trace anomaly form factors of the hadron energy-momentum tensor using overlap fermions<\/td>Bigeng Wang<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
edmchiqcd<\/td>The nucleon EDM from lattice QCD with overlap fermions at the physical point<\/td>Christian Zimmerman<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
ewbox<\/td>Calculation of the gammaW box<\/td>Fangcheng He<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
fourpluseight<\/td>Symmetric mass generation with domain wall fermions<\/td>Anna Hasenfratz<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
heavylight<\/td>Semileptonic B decays with a vector final state<\/td>Andrew Lytle<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
lhpc<\/td>Nucleon Quark-Gluon structure with Clover-Wilson Fermions and Domain Wall Fermions<\/td>Michael Engelhardt<\/td>A: LQ2<\/td>26\/07\/01<\/td><\/tr>
lp3<\/td>Gluon Parton Distribution of the nucleon from 2+1+1-Flavor Lattice QCD<\/td>William Good<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
mslight<\/td>New ensembles for precision projects by the Fermilab lattice and MILC collaborations<\/td>Alexei Bazavov<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
nplqcd<\/td>Nuclear Physics from the Standard Model<\/td>Phiala Shanahan<\/td>A: LQ2
B: LQ1<\/td>		26\/07\/01<\/td><\/tr>
nptmd<\/td>Computing the gluon Collins-Soper
Kernel for TMD Evolution<\/td>		Yang Fu<\/td>B: LQ2<\/td>26\/07\/01<\/td><\/tr>
pidf<\/td>Pion Valence Quark PDF from Kinematically-Enhanced Interpolators at High Momentum<\/td>Rui Zhang<\/td>A: LQ2<\/td>26\/07\/01<\/td><\/tr>
pion3d<\/td>3D Imaging of the Pion on a Fine Lattice<\/td>Jinchen He<\/td>A: LQ2<\/td>26\/07\/01<\/td><\/tr>
qcdalpha<\/td>The QCD strong coupling alpha_s at the Z-pole<\/td>Julius Kuti<\/td>A: LQ2<\/td>26\/07\/01<\/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\/07\/01<\/td><\/tr>
so4yukawa<\/td>Symmetric mass generation with staggered fermions and scalars<\/td>Julius Kuti<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
su2betafn<\/td>Symmetric mass generation with Four SU(2) Doublet Fermions<\/td>Simon Catterall<\/td>A: LQ1<\/td>26\/07\/01<\/td><\/tr>
taudecay<\/td>Inclusive hadronic decay of the tau lepton<\/td>William Jay<\/td>C: LQ1
C: LQ2<\/td>		26\/07\/01<\/td><\/tr>
tcrenorm<\/td>Tensor renormalization factors for the HISQ action in four-flavor Lattice QCD

Lattice gravity investigation (not to be confused with older latgrav)<\/td>		Abishek Samlodia

Jack Laiho<\/td>		B: LQ1

C: LQ1<\/td>		26\/07\/01

26\/02\/01<\/td><\/tr>
twistedm<\/td>Twist-3 GPDs from Lattice QCD<\/td>Martha Constantinou<\/td>A: LQ2<\/td>26\/07\/01<\/td><\/tr><\/tbody><\/table>
The PY2025-2026 Type A allocations are for the period from July 1, 2025, through June 30, 2026. Type B and C allocations are typically for 6 months.<\/figcaption><\/figure>\n\n\n\n

2024-2025 Allocations<\/h3>\n\n\n\n
Project Name<\/strong><\/td>Description<\/strong><\/td>Type<\/strong><\/td>PI<\/strong><\/td>Cluster<\/td>Ends<\/td><\/tr>
3dpion<\/td>3D Imaging of the Pion on a Fine Lattice<\/td>A<\/td>Jinchen He \/ Zhang Rui<\/td>LQ2<\/td>25\/07\/01<\/span><\/td><\/tr>
affine<\/td>QFT on Affine Lattices<\/td>C<\/td>George Fleming<\/td>LQ1<\/td>25\/07\/01<\/span><\/span><\/td><\/tr>
ahisq<\/td>Novel anisotropic pure gauge simulations and the spectrum of anisotropic staggered quarks<\/td>A<\/td>Yannis Trimis<\/td>LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
betafn<\/td>The non-perturbative renormalization group beta-function of eight-flavor SU(3) gauge theory<\/td>A<\/td>Curtis Peterson<\/td>LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
chiqcd<\/td>
Lattice calculation of QCD trace anomaly form factors of the hadron  energy-momentum tensor using overlap fermions<\/td>		A<\/td>Bigeng Wang<\/td>LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
fourpluseight<\/td>Gradient flow renormalization scheme<\/td>C<\/td>Anna Hasenfratz<\/td>LQ1<\/td>25\/07\/01<\/span><\/span><\/td><\/tr>
heavylight<\/td>
Semileptonic B decays with a vector final state<\/td>		A<\/td>Andrew Lytle<\/td>LQ1
LQ2<\/td>		25\/07\/01<\/span><\/td><\/tr>
lhpc<\/td>
Nucleon Quark-Gluon Structure with Clover-Wilson Fermions and Domain Wall Fermions<\/td>		A<\/td>Michael
Engelhardt<\/td>		LQ2<\/td>25\/07\/01<\/span><\/td><\/tr>
lp3<\/td>Gluon Parton Distribution of the Nucleon from 2+1+1-Flavor Lattice QCD<\/td>A<\/td>
Huey-Wen Lin<\/td>		LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
mlcross24<\/td>Machine learning to identify phases in pure SU(3) system toward estimating the width of the QCD crossover<\/td>B<\/td>David Clarke<\/td>LQ1<\/td>25\/07\/01<\/span><\/span><\/td><\/tr>
mslight<\/td>New ensembles for precision light-meson decay constants<\/td>A<\/td>Alexei
Bazavov<\/td>		LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
nplqcd<\/td>Nuclear Physics from the Standard Model<\/td>A<\/td>Phiala
Shanahan<\/td>		LQ1
LQ2<\/td>		25\/07\/01<\/span><\/td><\/tr>
nptmd<\/td>Computing the gluon Collins-Soper Kernel for TMD Evolution<\/td>A<\/td>Michael Hagman<\/td>LQ2<\/td>25\/07\/01<\/span><\/td><\/tr>
qcdalpha<\/td>From BSM to \u03b1<\/strong>_s in QCD at the Z-pole<\/td>A<\/td>Julius Kuti<\/td>LQ2<\/td>25\/07\/01<\/span><\/td><\/tr>
stagscale<\/td>Omega Baryon Scale Setting and Hadronic Vacuum Polarization Observables<\/td>A<\/td>Anthony Grebe<\/td>LQ2<\/td>25\/07\/01<\/span><\/td><\/tr>
stagmass<\/td>Studying non-local taste pion masses ultra via coarse MILC ensembles <\/td>C<\/td>Christopher Aubin<\/td>LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
su2betafn<\/td>Novel phases and emerging fixed points in SU(2) gauge systems<\/td>C<\/td>Anna Hasenfratz<\/td>LQ1<\/td>25\/07\/01<\/span><\/td><\/tr>
twistedm<\/td>Twist-3 GPDs from Lattice QCD<\/td>A<\/td>Martha Constantinou<\/td>LQ2<\/td>25\/07\/01<\/span><\/td><\/tr><\/tbody><\/table>
The PY2024-2025 Type A allocations are for the period from July 1, 2024, through June 30, 2025.<\/figcaption><\/figure>\n\n\n\n

2023-2024 Allocations<\/h3>\n\n\n\n
Project Name<\/strong><\/td>Description<\/strong><\/td>Type<\/strong><\/td>PI<\/strong><\/td>Cluster<\/td>Ends<\/td><\/tr>
ahisq<\/td>Novel anisotropic pure gauge simulations and the spectrum of anisotropic staggered quarks<\/td>A<\/td>Yannis Trimis <\/td>LQ1<\/td><\/td><\/tr>
chiqcd<\/td>Lattice calculation of nucleon energy-momentum tensor form factors using overlap fermions<\/td>A<\/td>Bigeng Wang<\/td>LQ1<\/td><\/td><\/tr>
fourpluseight<\/td>Gradient flow renormalization scheme<\/td>A<\/td>Anna Hasenfratz<\/td>LQ1<\/td><\/td><\/tr>
hadtensor<\/td>A Lattice Calculation of the Hadron Tensor of the Pion<\/td>A<\/td>William Jay<\/td>LQ1<\/td><\/td><\/tr>
heavylight<\/td>Semileptonic B decays with a vector final state<\/td>A<\/td>Andrew Lytle<\/td>LQ1<\/td><\/td><\/tr>
latgrav<\/td>Dynamical (unquenched) fermions coupled to geometry<\/td>C<\/td>John W Laiho<\/td>LQ1<\/td><\/td><\/tr>
lhpc<\/td>Nucleon Quark-Gluon Structure with Clover-Wilson Fermions and Domain Wall Fermions<\/td>A<\/td>Michael Engelhardt<\/td>LQ2<\/td><\/td><\/tr>
lgg<\/td>Asymptotic safety hypothesis for gravity using a lattice regularization.<\/td>C<\/td>Judah Unmuth-Yockey<\/td>LQ1<\/td><\/td><\/tr>
lp3<\/td>Constraining the Bjorken-x Dependence of the Strange Distribution of the Proton Using Lattice Inputs<\/td>A<\/td>Huey-wen Lin<\/td>LQ1<\/td><\/td><\/tr>
mslight<\/td>New ensembles for precision light-meson decay constants.<\/td>A<\/td>Steven Gottlieb<\/td>LQ1<\/td><\/td><\/tr>
nplqcd<\/td>Nuclear Physics from the Standard Model<\/td>A<\/td>Phiala Shanahan<\/td>LQ2<\/td><\/td><\/tr>
nptmd<\/td>Computing the Collins-Soper Kernel for TMD Evolution at the Physical Quark Masses<\/td>A<\/td>Michael Wagman<\/td>LQ1<\/td><\/td><\/tr>
qcdalpha<\/td>From BSM to \u03b1 in QCD at the Z-pole: 2023-2024<\/td>A<\/td>Julius Kuti<\/td>LQ2<\/td><\/td><\/tr>
stgmugm2<\/td>Muon g \u2212 2 Hadronic Vacuum Polarization from four flavors of sea quarks using the HISQ Action<\/td>A<\/td>Michael Lynch<\/td>LQ1,LQ2<\/td><\/td><\/tr>
stagscale<\/td>Scale setting studies on the MILC HISQ ensembles<\/td>A<\/td>Alexei Bazavov<\/td>LQ1<\/td><\/td><\/tr>
su2betafn<\/td>Novel phases and emerging fixed points in SU(2) gauge systems<\/td>A<\/td>Anna Hasenfratz<\/td>LQ1<\/td><\/td><\/tr>
twistedm<\/td>Twist-3 GPDs from Lattice QCD<\/td>A<\/td>Martha Constantinou<\/td>LQ2<\/td><\/td><\/tr><\/tbody><\/table>
The PY 2023-2024 Type A allocations are for the period from July 1, 2023, through June 30, 2024.<\/figcaption><\/figure>\n\n\n\n

2022-2023 Allocations<\/h3>\n\n\n\n
Project Name<\/strong><\/td>Description<\/strong><\/td>Type<\/strong><\/td>PI<\/strong><\/td>Ends<\/td><\/tr>
ahisq<\/td>Novel anisotropic pure gauge simulations and the spectrum of anisotropic staggered quarks<\/td>A<\/td>Alexei Bazavov<\/td><\/td><\/tr>
axial<\/td>The Nucleon Axial-Vector Form Factor at the Physical Point with the HISQ Ensembles<\/td>A<\/td>Andreas Kronfeld<\/td><\/td><\/tr>
chiqcd<\/td>Lattice calculation of nucleon energy-momentum tensor form factors using overlap fermions<\/td>A<\/td>Bigeng Wang<\/td><\/td><\/tr>
hadtensor<\/td>A Lattice Calculation of the Hadron Tensor of the Pion<\/td>A<\/td>William Jay<\/td><\/td><\/tr>
heavylight<\/td>Semileptonic B decays with a vector final state<\/td>A<\/td>Andrew Lytle<\/td><\/td><\/tr>
lp3<\/td>Constraining the Bjorken-x Dependence of the Strange Distribution of the Proton Using Lattice Inputs<\/td>A<\/td>Huey-wen Lin<\/td><\/td><\/tr>
mslight<\/td>New ensembles for precision light-meson decay constants.<\/td>A<\/td>Carleton DeTar<\/td><\/td><\/tr>
nptmd<\/td>Computing the Collins-Soper Kernel for TMD Evolution at the Physical Quark Masses<\/td>A<\/td>Michael Wagman<\/td><\/td><\/tr>
stgmugm2<\/td>Storage only allocation<\/td>A<\/td>Carleton Detar<\/td><\/td><\/tr>
gluonpdf<\/td>Gluon Parton Distribution of the Pion from Lattice QCD<\/td>B?<\/td>Huey-wen Lin<\/td>2022-07-01<\/td><\/tr>
qfenpct<\/td>Non-perturbative renormalization of critical phi4 theory on S2<\/td>B<\/td>Evan Owen<\/td>2023-01-01<\/td><\/tr><\/tbody><\/table>
The PY 2022-2023 Type A allocations were for the period from July 1, 2022, through June 30, 2023.<\/figcaption><\/figure>\n\n\n\n

2021-2022 Allocations<\/h3>\n\n\n\n
Project 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","protected":false},"excerpt":{"rendered":"

2025-2026 Allocations Project Name Description PI Type: Cluster End Date affine Lattice calculation of (conformal) field theories on curved spacetime Nobuyuki Matsumoto C: LQ1 26\/07\/01 ahisq Novel anisotropic pure gauge simulations and the spectrum of anisotropic staggered quarks Yannis Trimis A: LQ1 26\/07\/01 betafn Test of the Quantum EXpressions lattice field theory framework with Grid… More »<\/a><\/p>\n","protected":false},"author":67,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-8457","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/8457","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\/67"}],"replies":[{"embeddable":true,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/comments?post=8457"}],"version-history":[{"count":7,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/8457\/revisions"}],"predecessor-version":[{"id":8502,"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/pages\/8457\/revisions\/8502"}],"wp:attachment":[{"href":"https:\/\/computing.fnal.gov\/lqcd\/wp-json\/wp\/v2\/media?parent=8457"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}