Fixed bug in print_decay_modes where decays with equal BFs were skipped #1041
eduardo-rodriguesci.yml
on: pull_request
pre-commit
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Matrix: checks
Annotations
16 errors
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pre-commit
Process completed with exit code 1.
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Check ubuntu-latest Python 3.8:
tests/dec/test_dec.py#L196
test_particle_property_definitions
AssertionError: assert {'MyK*0': {'m...'width': 0.2}} == {'MyK*0': {'m...'width': 0.2}}
Omitting 3 identical items, use -vv to show
Differing items:
{'MyRho0': {'mass': 0.8, 'width': 147.4}} != {'MyRho0': {'mass': 0.8, 'width': 149.1}}
Full diff:
{
'MyK*0': {
'mass': 0.892,
'width': 0.051,
},
'MyPhi': {
'mass': 1.02,
'width': 0.004,
},
'MyRho0': {
'mass': 0.8,
- 'width': 149.1,
? ^ ^
+ 'width': 147.4,
? ^ ^
},
'rho0': {
'mass': 0.8,
'width': 0.2,
},
}
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Check ubuntu-latest Python 3.8:
tests/dec/test_dec.py#L518
test_custom_model_name
FileNotFoundError: '../data/test_custom_decay_model.dec'!
|
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Check ubuntu-latest Python 3.8:
tests/test_convert.py#L18
test_full_convert
assert {'', '"D0[D]{...,pi+}",', ...} == {'', '"D0[D]{...,pi+}",', ...}
Extra items in the left set:
'Variable rho_770_0_W { "rho_770_0_W" , 147.4 };'
Extra items in the right set:
'Variable rho_770_0_W { "rho_770_0_W" , 149.1 };'
Full diff:
{
'',
'"D0[D]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0[D]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0[P]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0[P]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0{K(1)(1270)-[D;GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{KPi20[FOCUS.Kpi]{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{omega(782){pi+,pi-},K-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{rho(1450)0{pi+,pi-},K-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{rho(770)0{pi+,pi-},K-},pi+}",',
'"D0{K(1)(1400)-{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.0]{pi+,pi-},K-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.1]{pi+,pi-},K-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.prod.1]{pi+,pi-},K-},pi+}",',
'"D0{K(2)*(1430)-{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.KEta]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.KEta]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.Kpi]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.Kpi]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{a(1)(1260)+[D;GSpline.EFF]{rho(770)0{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.pole.0]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.pole.1]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.prod.0]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{rho(770)0{pi+,pi-},pi+},K-}",',
'"D0{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0{rho(770)0{pi+,pi-},KPi10[FOCUS.I32]{K-,pi+}}",',
'"D0{rho(770)0{pi+,pi-},KPi10[FOCUS.Kpi]{K-,pi+}}",',
'*/',
'/* Autogenerated file by AmpGen2GooFit',
'// D0[D]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0[D]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}',
'// D0[P]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0[P]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}',
'// D0{K(1)(1270)-[D;GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{KPi20[FOCUS.Kpi]{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{omega(782){pi+,pi-},K-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{rho(1450)0{pi+,pi-},K-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{rho(770)0{pi+,pi-},K-},pi+}',
'// D0{K(1)(1400)-{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.0]{pi+,pi-},K-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.1]{pi+,pi-},K-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.prod.1]{pi+,pi-},K-},pi+}',
'// D0{K(2)*(1430)-{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.pole.1]{pi+,pi-}}',
'// D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.prod.0]{pi+,pi-}}',
'// D0{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}',
'// D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}
|
|
Check ubuntu-latest Python 3.8
Process completed with exit code 1.
|
|
Check ubuntu-latest Python 3.10:
tests/dec/test_dec.py#L196
test_particle_property_definitions
AssertionError: assert {'MyK*0': {'m...'width': 0.2}} == {'MyK*0': {'m...'width': 0.2}}
Omitting 3 identical items, use -vv to show
Differing items:
{'MyRho0': {'mass': 0.8, 'width': 147.4}} != {'MyRho0': {'mass': 0.8, 'width': 149.1}}
Full diff:
{
'MyK*0': {
'mass': 0.892,
'width': 0.051,
},
'MyPhi': {
'mass': 1.02,
'width': 0.004,
},
'MyRho0': {
'mass': 0.8,
- 'width': 149.1,
? ^ ^
+ 'width': 147.4,
? ^ ^
},
'rho0': {
'mass': 0.8,
'width': 0.2,
},
}
|
|
Check ubuntu-latest Python 3.10:
tests/dec/test_dec.py#L518
test_custom_model_name
FileNotFoundError: '../data/test_custom_decay_model.dec'!
|
|
Check ubuntu-latest Python 3.10:
tests/test_convert.py#L18
test_full_convert
assert {'', '"D0[D]{...,pi+}",', ...} == {'', '"D0[D]{...,pi+}",', ...}
Extra items in the left set:
'Variable rho_770_0_W { "rho_770_0_W" , 147.4 };'
Extra items in the right set:
'Variable rho_770_0_W { "rho_770_0_W" , 149.1 };'
Full diff:
{
'',
'"D0[D]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0[D]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0[P]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0[P]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0{K(1)(1270)-[D;GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{KPi20[FOCUS.Kpi]{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{omega(782){pi+,pi-},K-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{rho(1450)0{pi+,pi-},K-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{rho(770)0{pi+,pi-},K-},pi+}",',
'"D0{K(1)(1400)-{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.0]{pi+,pi-},K-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.1]{pi+,pi-},K-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.prod.1]{pi+,pi-},K-},pi+}",',
'"D0{K(2)*(1430)-{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.KEta]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.KEta]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.Kpi]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.Kpi]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{a(1)(1260)+[D;GSpline.EFF]{rho(770)0{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.pole.0]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.pole.1]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.prod.0]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{rho(770)0{pi+,pi-},pi+},K-}",',
'"D0{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0{rho(770)0{pi+,pi-},KPi10[FOCUS.I32]{K-,pi+}}",',
'"D0{rho(770)0{pi+,pi-},KPi10[FOCUS.Kpi]{K-,pi+}}",',
'*/',
'/* Autogenerated file by AmpGen2GooFit',
'// D0[D]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0[D]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}',
'// D0[P]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0[P]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}',
'// D0{K(1)(1270)-[D;GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{KPi20[FOCUS.Kpi]{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{omega(782){pi+,pi-},K-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{rho(1450)0{pi+,pi-},K-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{rho(770)0{pi+,pi-},K-},pi+}',
'// D0{K(1)(1400)-{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.0]{pi+,pi-},K-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.1]{pi+,pi-},K-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.prod.1]{pi+,pi-},K-},pi+}',
'// D0{K(2)*(1430)-{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.pole.1]{pi+,pi-}}',
'// D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.prod.0]{pi+,pi-}}',
'// D0{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}',
'// D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}
|
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Check ubuntu-latest Python 3.10
Process completed with exit code 1.
|
|
Check windows-latest Python 3.8
Process completed with exit code 1.
|
|
Check macos-13 Python 3.9
Process completed with exit code 1.
|
|
Check windows-latest Python 3.11
Process completed with exit code 1.
|
|
Check ubuntu-latest Python 3.12:
tests/dec/test_dec.py#L196
test_particle_property_definitions
AssertionError: assert {'MyK*0': {'m...'width': 0.2}} == {'MyK*0': {'m...'width': 0.2}}
Omitting 3 identical items, use -vv to show
Differing items:
{'MyRho0': {'mass': 0.8, 'width': 147.4}} != {'MyRho0': {'mass': 0.8, 'width': 149.1}}
Full diff:
{
'MyK*0': {
'mass': 0.892,
'width': 0.051,
},
'MyPhi': {
'mass': 1.02,
'width': 0.004,
},
'MyRho0': {
'mass': 0.8,
- 'width': 149.1,
? ^ ^
+ 'width': 147.4,
? ^ ^
},
'rho0': {
'mass': 0.8,
'width': 0.2,
},
}
|
|
Check ubuntu-latest Python 3.12:
tests/dec/test_dec.py#L518
test_custom_model_name
FileNotFoundError: '../data/test_custom_decay_model.dec'!
|
|
Check ubuntu-latest Python 3.12:
tests/test_convert.py#L18
test_full_convert
assert {'', '"D0[D]{...,pi+}",', ...} == {'', '"D0[D]{...,pi+}",', ...}
Extra items in the left set:
'Variable rho_770_0_W { "rho_770_0_W" , 147.4 };'
Extra items in the right set:
'Variable rho_770_0_W { "rho_770_0_W" , 149.1 };'
Full diff:
{
'',
'"D0[D]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0[D]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0[P]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0[P]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0{K(1)(1270)-[D;GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{KPi20[FOCUS.Kpi]{K-,pi+},pi-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{omega(782){pi+,pi-},K-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{rho(1450)0{pi+,pi-},K-},pi+}",',
'"D0{K(1)(1270)-[GSpline.EFF]{rho(770)0{pi+,pi-},K-},pi+}",',
'"D0{K(1)(1400)-{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.0]{pi+,pi-},K-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.1]{pi+,pi-},K-},pi+}",',
'"D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.prod.1]{pi+,pi-},K-},pi+}",',
'"D0{K(2)*(1430)-{K*(892)~0{K-,pi+},pi-},pi+}",',
'"D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}",',
'"D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.KEta]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.KEta]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.Kpi]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}",',
'"D0{KPi00[FOCUS.Kpi]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}",',
'"D0{a(1)(1260)+[D;GSpline.EFF]{rho(770)0{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.pole.0]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.pole.1]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{PiPi2[kMatrix.prod.0]{pi+,pi-},pi+},K-}",',
'"D0{a(1)(1260)+[GSpline.EFF]{rho(770)0{pi+,pi-},pi+},K-}",',
'"D0{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}",',
'"D0{rho(770)0{pi+,pi-},KPi10[FOCUS.I32]{K-,pi+}}",',
'"D0{rho(770)0{pi+,pi-},KPi10[FOCUS.Kpi]{K-,pi+}}",',
'*/',
'/* Autogenerated file by AmpGen2GooFit',
'// D0[D]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0[D]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}',
'// D0[P]{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0[P]{rho(1450)0{pi+,pi-},K*(892)~0{K-,pi+}}',
'// D0{K(1)(1270)-[D;GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{KPi20[FOCUS.Kpi]{K-,pi+},pi-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{omega(782){pi+,pi-},K-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{rho(1450)0{pi+,pi-},K-},pi+}',
'// D0{K(1)(1270)-[GSpline.EFF]{rho(770)0{pi+,pi-},K-},pi+}',
'// D0{K(1)(1400)-{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.0]{pi+,pi-},K-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.pole.1]{pi+,pi-},K-},pi+}',
'// D0{K(1460)-[GSpline.EFF]{PiPi3[kMatrix.prod.1]{pi+,pi-},K-},pi+}',
'// D0{K(2)*(1430)-{K*(892)~0{K-,pi+},pi-},pi+}',
'// D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.pole.1]{pi+,pi-}}',
'// D0{K*(892)~0{K-,pi+},PiPi1[kMatrix.prod.0]{pi+,pi-}}',
'// D0{K*(892)~0{K-,pi+},rho(770)0{pi+,pi-}}',
'// D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.pole.1]{pi+,pi-}}',
'// D0{KPi00[FOCUS.I32]{K-,pi+},PiPi0[kMatrix.prod.0]{pi+,pi-}}
|
|
Check ubuntu-latest Python 3.12
Process completed with exit code 1.
|