Closed jfeist closed 3 years ago
Merging #11 (25b8446) into main (9c3ba81) will increase coverage by
1.14%
. The diff coverage is100.00%
.
@@ Coverage Diff @@
## main #11 +/- ##
==========================================
+ Coverage 75.02% 76.16% +1.14%
==========================================
Files 10 11 +1
Lines 1105 1179 +74
==========================================
+ Hits 829 898 +69
- Misses 276 281 +5
Impacted Files | Coverage Δ | |
---|---|---|
src/QuantumAlgebra.jl | 100.00% <ø> (ø) |
|
src/alias.jl | 100.00% <100.00%> (ø) |
|
src/convert_to_expression.jl | 84.37% <100.00%> (+0.50%) |
:arrow_up: |
src/operator_defs.jl | 95.97% <100.00%> (+0.27%) |
:arrow_up: |
src/output.jl | 90.64% <100.00%> (+0.49%) |
:arrow_up: |
src/correlations.jl | 67.74% <0.00%> (-1.01%) |
:arrow_down: |
src/vacuum_expvals.jl | 90.14% <0.00%> (-0.63%) |
:arrow_down: |
... and 2 more |
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Using
@anticommuting_fermion_group c d
, you get a group of mutually anticommuting fermionic operators, e.g., to treat itinerant and localized electrons with different operators. Note that two different fermionic operators defined with independent@fermion_ops
calls are assumed to refer to different (quasi-)particle species, and thus commute.Example usage:
The operators within a group are ordered by definition order, not alphabetically as normally:
For comparison, for different
@fermion_ops
:Closes #9.