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Commit Graph

29 Commits

Author SHA1 Message Date
Vera Guelpers
315a42843f changes requested for the pull request 2018-03-02 11:47:38 +00:00
Vera Guelpers
49a0ae73eb Insertion of photon field in seqential conserved current 2018-02-12 09:36:08 +00:00
29e2eddea8 Merge branch 'develop' into feature/hadrons-new-memory-model 2017-12-06 16:49:21 +01:00
62eb1f0e59 FermionOperator virtual destructor needed for polymorphism 2017-12-06 16:48:17 +01:00
Lanny91
44260643f6 First conserved current implementation for Wilson fermions only. Not implemented for Gparity or 5D-vectorised Wilson fermions. 2017-04-25 18:00:24 +01:00
Peter Boyle
fb8d4b2357 Lots of debug on performance Mobius 2016-12-08 17:28:28 +00:00
paboyle
c014574504 A "please implement me" feynman rule. If this were abstract virtual it would
require/force implementation
2016-10-10 23:44:00 +01:00
paboyle
02e983a0cd Momentum space prop and free prop convolution 2016-08-31 00:26:02 +01:00
paboyle
aae8bf31a7 Global edit adding copyright and license info to every source file. 2016-01-02 14:51:32 +00:00
Peter Boyle
a842a6c94d One flavour rational unprec added; untested but does compile.
Moving param structs into a single header for later connection to file I/O using
macromagic.h
2015-08-18 14:40:08 +01:00
Peter Boyle
f0e32f12cf Merge branch 'master' of https://github.com/paboyle/Grid 2015-08-15 23:59:04 +01:00
Peter Boyle
55cfc89459 * Finished the template/policy style introduction of gparity, except the gparity force terms.
So valence sector looks ok.

FermionOperatorImpl.h provides the policy classes.

Expect HMC will introduce a smearing policy and a fermion representation change policy template
param. Will also probably need multi-precision work.

* HMC is running even-odd and non-checkerboarded (checked 4^4 wilson fermion/wilson gauge).

There appears to be a bug in the multi-level integrator -- <e-dH> passes with single level but
not with multi-level.

In any case there looks to be quite a bit to clean up.

This is the "const det" style implementation that is not appropriate  yet for clover since
it assumes that Mee is indept of the gauge fields. Easily fixed in future.
2015-08-15 23:25:49 +01:00
Peter Boyle
ba8c09a58e Reorganising the Fermion interface 2015-08-14 14:16:45 +01:00
Peter Boyle
59d66eb17a Gparity works now even if simd distributed in a Gparity twist direction.
Tested by doubling lattice in t-direction.
2015-08-14 12:57:42 +01:00
Peter Boyle
4dc7c36aa8 Gparity works now even if simd distributed in a Gparity twist direction.
Tested by doubling lattice in t-direction.
2015-08-14 12:57:42 +01:00
Peter Boyle
028e2061e0 Gparity valence test now working.
Interface in FermionOperator will change a lot in future
2015-08-14 00:01:04 +01:00
Peter Boyle
7d3512ab21 Gparity valence test now working.
Interface in FermionOperator will change a lot in future
2015-08-14 00:01:04 +01:00
Peter Boyle
aeb7442d8f Rework/global edit to enforce type templating of fermion operators.
Allows multi-precision work and paves the way for alternate BC's and such like
allowing for example G-parity which is important for K pipi programme.
In particular, can drive an extra flavour index into the fermion fields
using template types.
2015-08-10 20:47:44 +01:00
Peter Boyle
84a66476ab Rework/global edit to enforce type templating of fermion operators.
Allows multi-precision work and paves the way for alternate BC's and such like
allowing for example G-parity which is important for K pipi programme.
In particular, can drive an extra flavour index into the fermion fields
using template types.
2015-08-10 20:47:44 +01:00
Peter Boyle
2994274267 Changes making force term test for DWF pass. 2015-08-01 22:06:07 +09:00
Peter Boyle
2157a6919a Changes making force term test for DWF pass. 2015-08-01 22:06:07 +09:00
Peter Boyle
cc4ca48d13 Two flavour HMC for Wilson/Wilson is conserving energy.
Still to check plaq and <e(-dH)>, but nevertheless this is
progress
2015-07-29 17:53:39 +09:00
Peter Boyle
4fe110bd07 Two flavour HMC for Wilson/Wilson is conserving energy.
Still to check plaq and <e(-dH)>, but nevertheless this is
progress
2015-07-29 17:53:39 +09:00
Peter Boyle
d7e6b65a76 Elemental force term for Wilson dslash added and tests thereof passing.
Now need to construct pseudofermion two flavour, ratio, one flavour, ratio
action fragments.
2015-07-26 10:54:38 +09:00
Peter Boyle
d9d4c5916a Elemental force term for Wilson dslash added and tests thereof passing.
Now need to construct pseudofermion two flavour, ratio, one flavour, ratio
action fragments.
2015-07-26 10:54:38 +09:00
Peter Boyle
9e7035f5dc Conjugate residual algorithm; some more unary functions 2015-06-08 12:04:59 +01:00
Peter Boyle
d6f1ddf99c Conjugate residual algorithm; some more unary functions 2015-06-08 12:04:59 +01:00
Peter Boyle
2583570e17 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
Peter Boyle
3845f267cb 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