Dataset selection#
Here is the list of the datasets we implemented in SIMUnet to fit SMEFT coefficients. For each dataset, we indicate the experiment, the centre of mass energy \(\sqrt{s}\), the final-state channel, the observable(s) used in the fit, the integrated luminosity \(\mathcal{L}\) in inverse femtobarns, and the number of data points \(n_{\rm dat}\), together with the corresponding publication reference. The datasets are organised by physical sectors, namely top, Drell-Yan, W helicity, EW precision observables, Higgs and Diboson.
The user can easily include any of the following datasets to perform a fit with \(\text{SIMUnet}\). This
is done by adding the corresponding Dataset name
with its corresponding configuration keys to the dataset_input
in the runcard,
as shown in the example below:
dataset_inputs:
- {dataset: NMC, frac: 0.75}
- {dataset: ATLASTTBARTOT7TEV, cfac: [QCD], simu_fac: "EFT_NLO"}
- {dataset: CMS_SINGLETOPW_8TEV_TOTAL, simu_fac: "EFT_NLO", use_fixed_predictions: True}
The dataset NMC
is a NNPDF dataset, and it is included as it would be on an NNPDF4.0 runcard.
\(\text{SIMUnet}\) recognises it as a standard dataset with no need for SMEFT modifications.
In contrast, the dataset ATLASTTBARTOT7TEV
includes the additional key simu_fac
,
which instructs \(\text{SIMUnet}\) to calculate theory predictions for this dataset using SMEFT NLO K-factor, as it is clear from its EFT_NLO
value.
The third dataset, CMS_SINGLETOPW_8TEV_TOTAL
, includes two keys: simu_fac
, which has already been discussed, and use_fixed_predictions
. The use_fixed_predictions
key, when set to True,
effectively removes the PDF dependence of the dataset. This approach is appropriate for observables that are either independent of the PDFs (like EWPO or W-helicities in top decays, for example) or are only weakly influenced by them,
and therefore a full computation of FK-tables would be too computationally taxing.
Top sector#
TTBAR#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Channel |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|---|
ATLAS |
7 |
dilepton |
\(\sigma(t\bar{t})\) |
4.6 |
1 |
ATLASTTBARTOT7TEV |
|
ATLAS |
8 |
dilepton |
\(\sigma(t\bar{t})\) |
20.3 |
1 |
ATLASTTBARTOT8TEV |
|
ATLAS |
8 |
dilepton |
\(1/\sigma d\sigma/dm_{t\bar{t}}\) |
20.2 |
5 |
ATLAS_TOPDIFF_DILEPT_8TEV_TTMNORM |
|
ATLAS |
8 |
\(\ell \mathrm{+jets}\) |
\(\sigma(t\bar{t})\) |
20.2 |
1 |
ATLAS_TTBAR_8TEV_LJETS_TOTAL |
|
ATLAS |
8 |
\(\ell \mathrm{+jets}\) |
\(1/\sigma d\sigma/d|y_{t}|\) |
20.3 |
4 |
ATLAS_TTB_DIFF_8TEV_LJ_TRAPNORM |
|
ATLAS |
8 |
\(\ell \mathrm{+jets}\) |
\(1/\sigma d\sigma/d|y_{t\bar{t}}|\) |
20.3 |
4 |
ATLAS_TTB_DIFF_8TEV_LJ_TTRAPNORM |
|
ATLAS |
13 |
dilepton |
\(\sigma(t\bar{t})\) |
36.1 |
1 |
ATLAS_TTBAR_13TEV_DILEPTON_TOTAL |
|
ATLAS |
13 |
hadronic |
\(\sigma(t\bar{t})\) |
36.1 |
1 |
ATLAS_TTBAR_13TEV_HADRONIC_TOTAL |
|
ATLAS |
13 |
hadronic |
\(1/\sigma d^2\sigma/d|y_{t\bar{t}}|dm_{t\bar{t}}\) |
36.1 |
10 |
ATLAS_TTBAR_13TEV_HADRONIC_2D_TTM_ABSYTTNORM |
|
ATLAS |
13 |
\(\ell \mathrm{+jets}\) |
\(\sigma(t\bar{t})\) |
139 |
1 |
ATLAS_TTBAR_13TEV_LJETS_TOTAL |
|
ATLAS |
13 |
\(\ell \mathrm{+jets}\) |
\(1/\sigma d\sigma/dm_{t\bar{t}}\) |
36 |
8 |
ATLAS_TTBAR_13TEV_TTMNORM |
|
CMS |
5 |
combination |
\(\sigma(t\bar{t})\) |
0.027 |
1 |
CMSTTBARTOT5TEV |
|
CMS |
7 |
combination |
\(\sigma(t\bar{t})\) |
5.0 |
1 |
CMSTTBARTOT7TEV |
|
CMS |
8 |
combination |
\(\sigma(t\bar{t})\) |
19.7 |
1 |
CMSTTBARTOT8TEV |
|
CMS |
8 |
dilepton |
\(1/\sigma d^2\sigma/dy_{t\bar{t}}dm_{t\bar{t}}\) |
19.7 |
16 |
CMS_TTBAR_2D_DIFF_MTT_TTRAP_NORM |
|
CMS |
8 |
\(\ell \mathrm{+jets}\) |
\(1/\sigma d\sigma/dy_{t\bar{t}}\) |
19.7 |
9 |
CMSTOPDIFF8TEVTTRAPNORM |
|
CMS |
13 |
dilepton |
\(\sigma(t\bar{t})\) |
43 |
1 |
CMSTTBARTOT13TEV |
|
CMS |
13 |
dilepton |
\(1/\sigma d\sigma/dy_{t\bar{t}}\) |
35.9 |
5 |
CMS_TTB_DIFF_13TEV_2016_2L_TTMNORM |
|
CMS |
13 |
\(\ell \mathrm{+jets}\) |
\(\sigma(t\bar{t})\) |
137 |
1 |
CMS_TTBAR_13TEV_LJETS_TOTAL |
|
CMS |
13 |
\(\ell \mathrm{+jets}\) |
\(1/\sigma d\sigma/dm_{t\bar{t}}\) |
137 |
14 |
CMS_TTBAR_13TEV_TTMNORM |
TTBAR Asymmetry#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Channel |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|---|
ATLAS |
8 |
dilepton |
\(A_C\) |
20.3 |
1 |
ATLAS_TTBAR_8TEV_ASY |
|
ATLAS |
13 |
\(\ell \mathrm{+jets}\) |
\(A_C\) |
139 |
5 |
ATLAS_TTBAR_13TEV_ASY_2022 |
|
CMS |
8 |
dilepton |
\(A_C\) |
19.5 |
3 |
CMS_TTBAR_8TEV_ASY |
|
CMS |
13 |
\(\ell \mathrm{+jets}\) |
\(A_C\) |
138 |
3 |
CMS_TTBAR_13TEV_ASY |
|
ATLAS and CMS |
8 |
\(\ell \mathrm{+jets}\) |
\(A_C\) |
20 |
6 |
ATLAS_CMS_TTBAR_8TEV_ASY |
TTZ#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
ATLAS |
8 |
\(\sigma(t\bar{t}Z)\) |
20.3 |
1 |
ATLAS_TTBARZ_8TEV_TOTAL |
|
ATLAS |
13 |
\(\sigma(t\bar{t}Z)\) |
36.1 |
1 |
ATLAS_TTBARZ_13TEV_TOTAL |
|
ATLAS |
13 |
\(1/\sigma d\sigma(t\bar{t}Z)/dp_T^Z\) |
139 |
6 |
ATLAS_TTBARZ_13TEV_PTZNORM |
|
CMS |
8 |
\(\sigma(t\bar{t}Z)\) |
19.5 |
1 |
CMS_TTBARZ_8TEV_TOTAL |
|
CMS |
13 |
\(\sigma(t\bar{t}Z)\) |
35.9 |
1 |
CMS_TTBARZ_13TEV_TOTAL |
|
CMS |
13 |
\(1/\sigma d\sigma(t\bar{t}Z)/dp_T^Z\) |
77.5 |
3 |
CMS_TTBARZ_13TEV_PTZNORM |
TTW#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
ATLAS |
8 |
\(\sigma(t\bar{t}W)\) |
20.3 |
1 |
ATLAS_TTBARW_8TEV_TOTAL |
|
ATLAS |
13 |
\(\sigma(t\bar{t}W)\) |
36.1 |
1 |
ATLAS_TTBARW_13TEV_TOTAL |
|
CMS |
8 |
\(\sigma(t\bar{t}W)\) |
19.5 |
1 |
CMS_TTBARW_8TEV_TOTAL |
|
CMS |
13 |
\(\sigma(t\bar{t}W)\) |
35.9 |
1 |
CMS_TTBARW_13TEV_TOTAL |
TTGamma#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
ATLAS |
8 |
\(\sigma(t\bar{t}\gamma)\) |
20.2 |
1 |
ATLAS_TTBARGAMMA_8TEV_TOTAL |
|
CMS |
8 |
\(\sigma(t\bar{t}\gamma)\) |
19.7 |
1 |
CMS_TTBARGAMMA_8TEV_TOTAL |
4 Heavy quarks#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Channel |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|---|
ATLAS |
13 |
multi-lepton |
\(\sigma_{\text{tot}}(t\bar{t}t\bar{t})\) |
139 |
1 |
ATLAS_4TOP_13TEV_MULTILEP_TOTAL |
|
ATLAS |
13 |
single-lepton |
\(\sigma_{\text{tot}}(t\bar{t}t\bar{t})\) |
139 |
1 |
ATLAS_4TOP_13TEV_SLEP_TOTAL |
|
ATLAS |
13 |
\(\ell \mathrm{+jets}\) |
\(\sigma_{\text{tot}}(t\bar{t}b\bar{b})\) |
36.1 |
1 |
ATLAS_TTBB_13TEV_LJETS_TOTAL |
|
CMS |
13 |
multi-lepton |
\(\sigma_{\text{tot}}(t\bar{t}t\bar{t})\) |
137 |
1 |
CMS_4TOP_13TEV_MULTILEP_TOTAL |
|
CMS |
13 |
single-lepton |
\(\sigma_{\text{tot}}(t\bar{t}t\bar{t})\) |
35.8 |
1 |
CMS_4TOP_13TEV_SLEP_TOTAL |
|
CMS |
13 |
all-jet |
\(\sigma_{\text{tot}}(t\bar{t}b\bar{b})\) |
35.9 |
1 |
CMS_TTBB_13TEV_ALLJET_TOTAL |
|
CMS |
13 |
dilepton |
\(\sigma_{\text{tot}}(t\bar{t}b\bar{b})\) |
35.9 |
1 |
CMS_TTBB_13TEV_DILEPTON_TOTAL |
|
CMS |
13 |
\(\ell \mathrm{+jets}\) |
\(\sigma_{\text{tot}}(t\bar{t}b\bar{b})\) |
35.9 |
1 |
CMS_TTBB_13TEV_LJETS_TOTAL |
T#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Channel |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|---|
ATLAS |
7 |
t-channel |
\(\sigma_\text{tot}(t)\) |
4.59 |
1 |
ATLAS_SINGLETOP_TCH_7TEV_T |
|
ATLAS |
7 |
t-channel |
\(\sigma_\text{tot}(\bar{t})\) |
4.59 |
1 |
ATLAS_SINGLETOP_TCH_7TEV_TB |
|
ATLAS |
7 |
t-channel |
\(1/\sigma d\sigma(tq)/dy_t\) |
4.59 |
3 |
ATLAS_SINGLETOP_TCH_DIFF_7TEV_T_RAP_NORM |
|
ATLAS |
7 |
t-channel |
\(1/\sigma d\sigma(\bar{t}q)/dy_{\bar{t}}\) |
4.59 |
3 |
ATLAS_SINGLETOP_TCH_DIFF_7TEV_TBAR_RAP_NORM |
|
ATLAS |
8 |
t-channel |
\(\sigma_\text{tot}(t)\) |
20.2 |
1 |
ATLAS_SINGLETOP_TCH_8TEV_T |
|
ATLAS |
8 |
t-channel |
\(\sigma_{\text{tot}}(\bar{t})\) |
20.2 |
1 |
ATLAS_SINGLETOP_TCH_8TEV_TB |
|
ATLAS |
8 |
t-channel |
\(1/\sigma d\sigma(tq)/dy_t\) |
20.2 |
1 |
ATLAS_SINGLETOP_TCH_DIFF_8TEV_T_RAP_NORM |
|
ATLAS |
8 |
t-channel |
\(1/\sigma d\sigma(\bar{t}q)/dy_{\bar{t}}\) |
20.2 |
3 |
ATLAS_SINGLETOP_TCH_DIFF_8TEV_TBAR_RAP_NORM |
|
ATLAS |
8 |
s-channel |
\(\sigma_{\text{tot}}(t + \bar{t})\) |
20.3 |
1 |
ATLAS_SINGLETOP_SCH_8TEV_TOTAL |
|
ATLAS |
13 |
t-channel |
\(\sigma_\text{tot}(t)\) |
3.2 |
1 |
ATLAS_SINGLETOP_TCH_13TEV_T |
|
ATLAS |
13 |
t-channel |
\(\sigma_{\text{tot}}(\bar{t})\) |
3.2 |
1 |
ATLAS_SINGLETOP_TCH_13TEV_TB |
|
ATLAS |
13 |
s-channel |
\(\sigma_\text{tot}(t+\bar{t})\) |
139 |
1 |
ATLAS_SINGLETOP_SCH_13TEV_TOTAL |
|
CMS |
7 |
t-channel |
\(\sigma_\text{tot}(t) + \sigma_{\text{tot}}(\bar{t})\) |
1.17, 1.56 |
1 |
CMS_SINGLETOP_TCH_TOT_7TEV |
|
CMS |
8 |
t-channel |
\(\sigma_\text{tot}(t)\) |
19.7 |
1 |
CMS_SINGLETOP_TCH_8TEV_T |
|
CMS |
8 |
t-channel |
\(\sigma_{\text{tot}}(\bar{t})\) |
19.7 |
1 |
CMS_SINGLETOP_TCH_8TEV_TB |
|
CMS |
8 |
s-channel |
\(\sigma_\text{tot}(t+\bar{t})\) |
19.7 |
1 |
CMS_SINGLETOP_SCH_8TEV_TOTAL |
|
CMS |
13 |
t-channel |
\(\sigma_\text{tot}(t)\) |
2.2 |
1 |
CMS_SINGLETOP_TCH_13TEV_T |
|
CMS |
13 |
t-channel |
\(\sigma_{\text{tot}}(\bar{t})\) |
2.2 |
1 |
CMS_SINGLETOP_TCH_13TEV_TB |
|
CMS |
13 |
t-channel |
\(1/\sigma d\sigma/d|y^{(t)}|\) |
35.9 |
4 |
CMS_SINGLETOP_TCH_13TEV_YTNORM |
TW#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Channel |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|---|
ATLAS |
8 |
dilepton |
\(\sigma_{\text{tot}}(tW)\) |
20.3 |
1 |
ATLAS_SINGLETOPW_8TEV_TOTAL |
|
ATLAS |
8 |
single-lepton |
\(\sigma_{\text{tot}}(tW)\) |
20.2 |
1 |
ATLAS_SINGLETOPW_8TEV_SLEP_TOTAL |
|
ATLAS |
13 |
dilepton |
\(\sigma_{\text{tot}}(tW)\) |
3.2 |
1 |
ATLAS_SINGLETOPW_13TEV_TOTAL |
|
CMS |
8 |
dilepton |
\(\sigma_{\text{tot}}(tW)\) |
12.2 |
1 |
CMS_SINGLETOPW_8TEV_TOTAL |
|
CMS |
13 |
dilepton |
\(\sigma_{\text{tot}}(tW)\) |
35.9 |
1 |
CMS_SINGLETOPW_13TEV_TOTAL |
|
CMS |
13 |
single-lepton |
\(\sigma_{\text{tot}}(tW)\) |
36 |
1 |
CMS_SINGLETOPW_13TEV_SLEP_TOTAL |
TZ#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Channel |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|---|
ATLAS |
13 |
dilepton |
\(\sigma_{\text{fid}}(tZj)\) |
139 |
1 |
ATLAS_SINGLETOPZ_13TEV_TOTAL |
|
CMS |
13 |
dilepton |
\(\sigma_{\text{fid}}(tZj)\) |
77.4 |
1 |
CMS_SINGLETOPZ_13TEV_TOTAL |
|
CMS |
13 |
dilepton |
\(d\sigma_{\text{fid}}(tZj)/dp_T^t\) |
138 |
3 |
CMS_SINGLETOPZ_13TEV_PTT |
Drell-Yan#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
ATLAS |
8 |
\(d^2\sigma/dm_{\ell\ell}d|y_{\ell\ell}|\) |
20.3 |
48 |
ATLASDY2D8TEV |
Reference (Table 3) |
ATLAS |
7 |
\(d\sigma_{Z/\gamma^{*}}/dM_{ll}\) |
4.9 |
13 |
ATLASZHIGHMASS49FB |
|
CMS |
7 |
\(d\sigma_{Z/\gamma^{*}}/dy\) |
4.5 |
132 |
CMSDY2D11 |
|
CMS |
8 |
\(d\sigma_{Z/\gamma^{*}}/dy\) |
19.7 |
41 |
CMSDY1D12 |
|
CMS |
13 |
\(d\sigma/dM_{\ell\ell}\) |
5.1 |
43 |
CMS_HMDY_13TEV |
W helicity#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
ATLAS and CMS |
8 |
\(F_0, F_L\) |
20 |
2 |
ATLAS_CMS_WHEL_8TEV |
|
ATLAS |
13 |
\(F_0, F_L\) |
139 |
2 |
ATLAS_WHEL_13TEV |
Electroweak Precision Observables#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
LEP |
0.250 |
Z observables |
19 |
LEP_ZDATA |
Reference (Tables 2.13, 3.6, 4.3, 5.8, and 5.10) |
|
LEP |
0.196 |
\(\mathcal{B}(W \rightarrow e^{-} \bar{v}_e),\) \(\mathcal{B}(W \rightarrow \mu^{-} \bar{v}_{\mu}),\) \(\mathcal{B}(W \rightarrow \tau^{-} \bar{v}_{\tau})\) |
3 |
3 |
LEP_BRW |
Reference (Table E.6) |
LEP |
0.189 |
\(\sigma(e^+ e^- \rightarrow e^+ e^-)\) |
3 |
21 |
LEP_BHABHA |
Reference (Table 3.11 and 3.12) |
LEP |
0.209 |
\(\hat{\alpha}^{(5)}_{\rm}(M_Z)\) |
3 |
1 |
LEP_ALPHAEW |
Reference (Equation 10.11) |
Higgs#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
ATLAS and CMS |
7 and 8 |
\(\mu_{H \rightarrow \mu^+ \mu^-}\) |
5 and 20 |
22 |
ATLAS_CMS_SSinc_RunI |
Reference (Table 13) |
CMS |
13 |
\(\mu_{H}\) |
35.9 |
24 |
CMS_SSINC_RUNII |
|
ATLAS |
13 |
\(\mu_{H}\) |
80 |
25 |
ATLAS_STXS_RUNII |
|
ATLAS |
13 |
\(\mu_{H \rightarrow Z \gamma}\) |
139 |
1 |
ATLAS_SSINC_RUNII_ZGAM |
|
ATLAS |
13 |
\(\mu_{H \rightarrow \mu^+ \mu^-}\) |
139 |
1 |
ATLAS_SSINC_RUNII_MUMU |
Diboson#
Exp. |
\(\bf{\sqrt{s}} \textbf{(TeV)}\) |
Observable |
\(\mathcal{L} (\text{fb}^{-1})\) |
\(\mathbf{n_{\rm dat}}\) |
Dataset name |
Ref. |
---|---|---|---|---|---|---|
LEP |
0.182 |
\(d \sigma _{WW} / d cos(\theta _W)\) |
0.164 |
10 |
LEP_EEWW_182GEV |
Reference (Table 5.6, line 1) |
LEP |
0.189 |
\(d \sigma _{WW} / d cos(\theta _W)\) |
0.588 |
10 |
LEP_EEWW_189GEV |
Reference (Table 5.6, line 2) |
LEP |
0.198 |
\(d \sigma _{WW} / d cos(\theta _W)\) |
0.605 |
10 |
LEP_EEWW_198GEV |
Reference (Table 5.6, line 3) |
LEP |
0.206 |
\(d \sigma _{WW} / d cos(\theta _W)\) |
0.631 |
10 |
LEP_EEWW_206GEV |
Reference (Table 5.6, line 4) |
ATLAS |
13 |
\(d \sigma _{W^+W^-}/d m_{e \mu}\) |
36.1 |
13 |
ATLAS_WW_13TeV_2016_MEMU |
|
ATLAS |
13 |
\(d \sigma _{WZ} / d m_{T}\) |
36.1 |
6 |
ATLAS_WZ_13TeV_2016_MTWZ |
|
ATLAS |
13 |
\(d \sigma(Zjj)/d \Delta \phi_{jj}\) |
139 |
12 |
ATLAS_Zjj_13TeV_2016 |
Reference (Table 8) |
CMS |
13 |
\(d \sigma _{WZ} / d p_{T}\) |
35.9 |
11 |
CMS_WZ_13TeV_2016_PTZ |