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Grid/lib/Makefile.am

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Reorg of build structure
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# additional include paths necessary to compile the C++ library
AM_CXXFLAGS = -I$(top_srcdir)/
extra_sources=
if BUILD_COMMS_MPI
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extra_sources+=communicator/Grid_communicator_mpi.cc
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endif
Vectors now too and right multiple of matrix with gamma
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if BUILD_COMMS_NONE
Command line args and a general clean up
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extra_sources+=communicator/Grid_communicator_none.cc
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endif
#
# Libraries
#
lib_LIBRARIES = libGrid.a
Partial implementation of the vector types SIMD Implementing SSE4 now A systematic series of tests must be written.
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libGrid_a_SOURCES = \
Grid_init.cc \
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
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stencil/Grid_lebesgue.cc \
Partial implementation of the vector types SIMD Implementing SSE4 now A systematic series of tests must be written.
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stencil/Grid_stencil_common.cc \
algorithms/approx/Zolotarev.cc \
algorithms/approx/Remez.cc \
Domain wall fermions now invert ; have the basis set up for Tanh/Zolo * (Cayley/PartFrac/ContFrac) * (Mobius/Shamir/Wilson) Approx Representation Kernel. All are done with space-time taking part in checkerboarding, Ls uncheckerboarded Have only so far tested the Domain Wall limit of mobius, and at that only checked that it i) Inverts ii) 5dim DW == Ls copies of 4dim D2 iii) MeeInv Mee == 1 iv) Meo+Mee+Moe+Moo == M unprec. v) MpcDagMpc is hermitan vi) Mdag is the adjoint of M between stochastic vectors. That said, the RB schur solve, RB MpcDagMpc solve, Unprec solve all converge and the true residual becomes small; so pretty good tests.
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qcd/SpaceTimeGrid.cc\
qcd/Dirac.cc\
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
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qcd/action/fermion/WilsonKernels.cc\
qcd/action/fermion/WilsonKernelsHand.cc\
Domain wall fermions now invert ; have the basis set up for Tanh/Zolo * (Cayley/PartFrac/ContFrac) * (Mobius/Shamir/Wilson) Approx Representation Kernel. All are done with space-time taking part in checkerboarding, Ls uncheckerboarded Have only so far tested the Domain Wall limit of mobius, and at that only checked that it i) Inverts ii) 5dim DW == Ls copies of 4dim D2 iii) MeeInv Mee == 1 iv) Meo+Mee+Moe+Moo == M unprec. v) MpcDagMpc is hermitan vi) Mdag is the adjoint of M between stochastic vectors. That said, the RB schur solve, RB MpcDagMpc solve, Unprec solve all converge and the true residual becomes small; so pretty good tests.
2015-06-02 16:57:12 +01:00
qcd/action/fermion/WilsonFermion.cc\
qcd/action/fermion/WilsonFermion5D.cc\
qcd/action/fermion/CayleyFermion5D.cc \
qcd/action/fermion/ContinuedFractionFermion5D.cc \
Vectors now too and right multiple of matrix with gamma
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$(extra_sources)
Reorg of build structure
2015-04-18 14:55:00 +01:00
Domain wall fermions now invert ; have the basis set up for Tanh/Zolo * (Cayley/PartFrac/ContFrac) * (Mobius/Shamir/Wilson) Approx Representation Kernel. All are done with space-time taking part in checkerboarding, Ls uncheckerboarded Have only so far tested the Domain Wall limit of mobius, and at that only checked that it i) Inverts ii) 5dim DW == Ls copies of 4dim D2 iii) MeeInv Mee == 1 iv) Meo+Mee+Moe+Moo == M unprec. v) MpcDagMpc is hermitan vi) Mdag is the adjoint of M between stochastic vectors. That said, the RB schur solve, RB MpcDagMpc solve, Unprec solve all converge and the true residual becomes small; so pretty good tests.
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# qcd/action/fermion/PartialFractionFermion5D.cc \
Reorg of build structure
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#
# Include files
#
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
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nobase_include_HEADERS=\
./algorithms/approx/bigfloat.h\
./algorithms/approx/bigfloat_double.h\
./algorithms/approx/Chebyshev.h\
./algorithms/approx/Remez.h\
./algorithms/approx/Zolotarev.h\
./algorithms/iterative/ConjugateGradient.h\
./algorithms/iterative/NormalEquations.h\
./algorithms/iterative/SchurRedBlack.h\
./algorithms/LinearOperator.h\
./algorithms/SparseMatrix.h\
./cartesian/Grid_cartesian_base.h\
./cartesian/Grid_cartesian_full.h\
./cartesian/Grid_cartesian_red_black.h\
./communicator/Grid_communicator_base.h\
./cshift/Grid_cshift_common.h\
./cshift/Grid_cshift_mpi.h\
./cshift/Grid_cshift_none.h\
./Grid.h\
./Grid_algorithms.h\
./Grid_aligned_allocator.h\
./Grid_cartesian.h\
./Grid_communicator.h\
./Grid_comparison.h\
./Grid_config.h\
./Grid_cshift.h\
./Grid_extract.h\
./Grid_lattice.h\
./Grid_math.h\
./Grid_simd.h\
./Grid_stencil.h\
./Grid_threads.h\
./lattice/Grid_lattice_arith.h\
./lattice/Grid_lattice_base.h\
./lattice/Grid_lattice_comparison.h\
./lattice/Grid_lattice_conformable.h\
./lattice/Grid_lattice_coordinate.h\
./lattice/Grid_lattice_ET.h\
./lattice/Grid_lattice_local.h\
./lattice/Grid_lattice_overload.h\
./lattice/Grid_lattice_peekpoke.h\
./lattice/Grid_lattice_reality.h\
./lattice/Grid_lattice_reduction.h\
./lattice/Grid_lattice_rng.h\
./lattice/Grid_lattice_trace.h\
./lattice/Grid_lattice_transfer.h\
./lattice/Grid_lattice_transpose.h\
./lattice/Grid_lattice_where.h\
./math/Grid_math_arith.h\
./math/Grid_math_arith_add.h\
./math/Grid_math_arith_mac.h\
./math/Grid_math_arith_mul.h\
./math/Grid_math_arith_scalar.h\
./math/Grid_math_arith_sub.h\
./math/Grid_math_inner.h\
./math/Grid_math_outer.h\
./math/Grid_math_peek.h\
./math/Grid_math_poke.h\
./math/Grid_math_reality.h\
./math/Grid_math_tensors.h\
./math/Grid_math_trace.h\
./math/Grid_math_traits.h\
./math/Grid_math_transpose.h\
./parallelIO/GridNerscIO.h\
./qcd/action/Actions.h\
Domain wall fermions now invert ; have the basis set up for Tanh/Zolo * (Cayley/PartFrac/ContFrac) * (Mobius/Shamir/Wilson) Approx Representation Kernel. All are done with space-time taking part in checkerboarding, Ls uncheckerboarded Have only so far tested the Domain Wall limit of mobius, and at that only checked that it i) Inverts ii) 5dim DW == Ls copies of 4dim D2 iii) MeeInv Mee == 1 iv) Meo+Mee+Moe+Moo == M unprec. v) MpcDagMpc is hermitan vi) Mdag is the adjoint of M between stochastic vectors. That said, the RB schur solve, RB MpcDagMpc solve, Unprec solve all converge and the true residual becomes small; so pretty good tests.
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./qcd/action/fermion/FermionOperator.h\
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
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./qcd/action/fermion/WilsonCompressor.h\
./qcd/action/fermion/WilsonKernels.h\
Domain wall fermions now invert ; have the basis set up for Tanh/Zolo * (Cayley/PartFrac/ContFrac) * (Mobius/Shamir/Wilson) Approx Representation Kernel. All are done with space-time taking part in checkerboarding, Ls uncheckerboarded Have only so far tested the Domain Wall limit of mobius, and at that only checked that it i) Inverts ii) 5dim DW == Ls copies of 4dim D2 iii) MeeInv Mee == 1 iv) Meo+Mee+Moe+Moo == M unprec. v) MpcDagMpc is hermitan vi) Mdag is the adjoint of M between stochastic vectors. That said, the RB schur solve, RB MpcDagMpc solve, Unprec solve all converge and the true residual becomes small; so pretty good tests.
2015-06-02 16:57:12 +01:00
./qcd/action/fermion/WilsonFermion.h\
./qcd/action/fermion/WilsonFermion5D.h\
Large scale change to support 5d fermion formulations. Have 5d replicated wilson with 4d gauge working and matrix regressing to Ls copies of wilson.
2015-05-31 15:09:02 +01:00
./qcd/Dirac.h\
./qcd/QCD.h\
./qcd/TwoSpinor.h\
./simd/Grid_avx.h\
./simd/Grid_avx512.h\
./simd/Grid_qpx.h\
./simd/Grid_sse4.h\
./simd/Grid_vector_types.h\
./simd/Old/Grid_vComplexD.h\
./simd/Old/Grid_vComplexF.h\
./simd/Old/Grid_vInteger.h\
./simd/Old/Grid_vRealD.h\
./simd/Old/Grid_vRealF.h\
./stencil/Grid_lebesgue.h
Reorg of build structure
2015-04-18 14:55:00 +01:00
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