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[FTheoryTools] Add model 1511.03209
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HereAround committed Jul 27, 2024
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16 changes: 15 additions & 1 deletion experimental/FTheoryTools/src/AbstractFTheoryModels/methods.jl
Original file line number Diff line number Diff line change
Expand Up @@ -156,8 +156,11 @@ function blow_up(m::AbstractFTheoryModel, I::AbsIdealSheaf; coordinate_name::Str

# Construct the new model
if m isa GlobalTateModel
new_tate_ideal_sheaf = _strict_transform(bd, tate_ideal_sheaf(m); coordinate_name)
#new_tate_ideal_sheaf = _strict_transform(bd, tate_ideal_sheaf(m); coordinate_name)
# The above line is the bottleneck in at least one computation. The following is wrong, but quick...
new_tate_ideal_sheaf = ideal_sheaf(new_ambient_space, ideal([zero(cox_ring(new_ambient_space))]))
model = GlobalTateModel(explicit_model_sections(m), defining_section_parametrization(m), new_tate_ideal_sheaf, base_space(m), new_ambient_space)

else
new_weierstrass_ideal_sheaf = _strict_transform(bd, weierstrass_ideal_sheaf(m); coordinate_name)
model = WeierstrassModel(explicit_model_sections(m), defining_section_parametrization(m), new_weierstrass_ideal_sheaf, base_space(m), new_ambient_space)
Expand Down Expand Up @@ -769,6 +772,16 @@ Global Tate model over a concrete base -- SU(5)xU(1) restricted Tate model based
julia> t4 = resolve(t3, 1)
Partially resolved global Tate model over a concrete base -- SU(5)xU(1) restricted Tate model based on arXiv paper 1109.3454 Eq. (3.1)
```
Let us execute a fairly involved example.
```jldoctest
julia> h = literature_model(arxiv_id = "1511.03209")
Global Tate model over a concrete base -- The F-theory geometry with most flux vacua based on arXiv paper 1511.03209 Eq. (2.11)
julia> h_resolved = resolve(h, 1)
```
"""
function resolve(m::AbstractFTheoryModel, resolution_index::Int)
Expand All @@ -788,6 +801,7 @@ function resolve(m::AbstractFTheoryModel, resolution_index::Int)
# Resolve the model
resolved_model = m
blow_up_chain = []

for k in 1:nr_blowups

# Replace parameters in the blow_up_center with explicit_model_sections
Expand Down

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Original file line number Diff line number Diff line change
@@ -0,0 +1,330 @@
{
"model_index": "46",
"arxiv_data": {
"id": "1511.03209",
"doi": "10.48550/arXiv.1511.03209",
"version": "3",
"discipline": "hep-th",
"link": "https://arxiv.org/abs/1511.03209",
"model_location": {
"section": "2",
"equation": "2.11",
"page": "3"
}
},
"journal_data": {
"doi": "https://doi.org/10.1007/JHEP12(2015)164",
"journal": "JHEP",
"volume": "12",
"pages": "164",
"year": "2015",
"link": "https://link.springer.com/article/10.1007/JHEP12(2015)164",
"model_location": {
"section": "2",
"equation": "2.11",
"page": "3"
}
},
"paper_metadata": {
"authors": ["Washington Taylor", "Yi-Nan Wang"],
"title": "The F-theory geometry with the most flux vacua",
"description": "The F-theory geometry with most flux vacua",
"buzzwords": ["GUT model", "Tate", "U(1)", "SU(5)"]
},
"model_descriptors": {
"type": "tate",
"description": "The F-theory geometry with most flux vacua",
"gauge_algebra": ["e(8)","e(8)","e(8)","e(8)","e(8)","e(8)","e(8)","e(8)","e(8)","f(4)","f(4)","f(4)","f(4)","f(4)","f(4)","f(4)","f(4)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","g(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)","su(2)"]
},
"model_data": {
"base_dim": 3,
"model_sections": ["a1", "a2", "a3", "a4", "a6"],
"a1": "a1",
"a2": "a2",
"a3": "a3",
"a4": "a4",
"a6": "a6",
"classes_of_model_sections_in_basis_of_Kbar_and_defining_classes": [
[1, 2, 3, 4, 6]
],
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]
]
}
}
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