Changelog¶
This document describes the main changes in CTHyb.
Version 2.1¶
Contributors¶
- Hugo U. R. Strand, new functionality, two-particle Green’s function sampling in imaginary time and frequency, and sampling by operator insertion.
- Igor Krivenko, occupation number constraints in the trace, two-particle Green’s function sampling with NFFT and mixed basis frequency*(legendre)^2.
- Lewin Boehnke, (indirect contribution) through the first mixed basis sampling implementation in an early version of
cthyb
. - Nils Wentzell, nfft_buf_t, cmake, and install.
Testers¶
Manuel Zingl, Daniel Mantadakis, and Jonathan Karp.
Changes in installation and cmake files¶
- Headers are now installed to
${CMAKE_INSTALL_PREFIX}/include/triqs_cthyb
. - The c++ namespace is now a single namespace called
triqs_cthyb
. - The python module is named
triqs_cthyb
.
Solver Interface¶
The type of gf_struct has changed from a dict to a list of pairs
{ 'up' : [0, 1], 'dn' : [0, 1] } --> [ ('up', [0,1]), ('dn', [0,1]) ]
measure_g_l has been renamed to measure_G_l
measure_g_tau has been renamed to measure_G_tau
Truncation of the local Hilbert space in total density using
loc_n_min
andloc_n_max
Two particle Greens function sampling with a whole set of measurements see
measure_G2_*
Two particle susceptibilities sampling by insertion using measure_O_tau
Tunable parameters for the determinant regularization see det_* parameters
Solver object can be stored and loaded directly to/from h5 archive
Tail fit functionality is rewritten for the Triqs 2.0 change in how tail coefficients are handled
Changes in behavior¶
move_double
is now enabled by default.The sampled single particle Greens function is modified when tail fitting is enabled.
The
gf_struct
should be a list of list of block index and a list of target space indices, e.g.gf_struct = [['up', [0, 1]], ['down', [0, 1]]]
.When passing a dictionary a warning is printed.
Dependencies¶
- The NFFT3 library by default, to compile without the library use the cmake flag
-DMeasureG2=OFF
.