actually include symmetry analysis tests in runtest.jl

- rename *stopgap test-file to *manual.

add Random to test/Project.toml

Author: thchr

test/Project.toml

@@ -2,4 +2,5 @@
 Crystalline = "ae5e2be0-a263-11e9-351e-f94dad1eb351"
 DeepDiffs = "ab62b9b5-e342-54a8-a765-a90f495de1a6"
 LinearAlgebra = "37e2e46d-f89d-539d-b4ee-838fcccc9c8e"
+Random = "9a3f8284-a2c9-5f02-9a11-845980a1fd5c"
 Test = "8dfed614-e22c-5e08-85e1-65c5234f0b40"

test/runtests.jl

@@ -8,8 +8,8 @@ include("berry.jl")                # berry curvature and chern numbers
 include("spectrum.jl")             # spectrum evaluation
 include("show.jl")                 # show/display methods
 include("gradients.jl")            # hopping and momentum gradients
-#include("symmetry_analysis.jl")    # each tb model is symmetry compatible w/ its constituent EBRs (not yet working)
-include("symmetry_analysis_stopgap.jl") # paired-down version of above (interim; see PR #89)
+include("symmetry_analysis.jl")    # each tb model is symmetry compatible w/ its constituent EBRs
+include("symmetry_analysis_manual.jl") # paired-down, manual version of above, testing individual cases
 
 @testset "AbstractArray interface" begin
     brs = calc_bandreps(16, Val(2))

test/symmetry_analysis.jl

@@ -11,7 +11,7 @@ using Crystalline: free
     sgnum = 17                         # plane group p6mm
     brs = calc_bandreps(sgnum, Val(2)) # band representations
     cbr = @composite brs[5]            # (2b|A₁) EBR
-    tbm = tb_hamiltonian(cbr)          # tight-binding model (nearest neigbors)
+    tbm = tb_hamiltonian(cbr)          # tight-binding model (nearest neighbors)
     ptbm = tbm([0, 1])                 # zero self-energy, nonzero nearest-neighbor hopping
     ns = collect_compatible(ptbm)
     @test only(ns) == SymmetryVector(cbr) == SymmetryVector(CompositeBandRep(ptbm))