cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.102183.v1/t3
title: "Cutflow ggF" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: The efficiency for simulated ggF events to pass each analysis cut.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t4
title: "Cutflow VBF" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: The efficiency for simulated VBF events to pass each analysis cut.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t5
title: "Cutflow VH" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: The efficiency for simulated VH events to pass each analysis cut.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t6
title: "Cutflow ttH" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: The efficiency for simulated ttH events to pass each analysis cut.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t7
title: "Fractional contribution" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: The fractional contribution of each production mode to a given analysis region around the Higgs boson peak, defined as 105 &lt; mJ &lt; 140 GeV. The fraction is given with respect to the total signal yield in the analysis region in question.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t10
title: "Event yields - fiducial" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: Event yields and associated uncertainties after the global likelihood fit in the pT(H) &gt; 450 GeV fiducial region. The total background yield can differ from the sum of the individual components due to rounding.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t8
title: "Acceptance times efficiency - fiducial" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: Signal acceptance times efficiency within the fiducial volume used in the fiducial region.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t9
title: "Acceptance times efficiency - differential" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: Signal acceptance times efficiency for the STXS volumes in the differential measurement. Along with the pTH requirements shown, |yH | &lt; 2 is required. For events with pTH &lt; 300 GeV, the acceptance times efficiency is less than 0.1 × 10−2.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102183.v1/t11
title: "Event yields - differential" of "Constraints on Higgs boson production with large transverse momentum using $H\rightarrow b\bar{b}$ decays in the ATLAS detector"

description: Event yields and associated uncertainties after the global likelihood fit of the differential regions. The total background yield can differ from the sum of the individual components due to rounding. The five STXS volumes are labeled pT0–pT4 corresponding to pTH &lt; 300 GeV, 300 – 450 GeV, 450 – 650 GeV, 650 – 1000 GeV, and &gt; 1000 GeV, respectively. The pT0 event yield is constrained to its SM value within the theoretical and experimental uncertainties and free parameters act independently on the remaining four volumes.
description: CERN-LHC. Constraints of Higgs boson production with transverse momentum up to the TeV scale. The analyzed pp collision data were recorded with the ATLAS detector at the LHC with a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 136 fb^-1. Higgs bosons decaying to bb are reconstructed as single large-radius jets and identified by the experimental signature of two b-hadron decays.

The two cross-section measurement channels:
- Fiducial analysis considers events with a candidate jet with pT &gt; 450 GeV. The signal strength corresponds to events within a fiducial volume which include ggF+VBF+VH+ttH produced events with pT(H) &gt; 450 GeV and |yH| &lt; 2.
- Differential analysis considers events within four bins of candidate jet pT 250-450 GeV, 450-650 GeV, 650-1000 GeV, &gt; 1 TeV. The four signal strengths correspond to events within STXS-like volumes which include ggF+VBF+VH+ttH produced events with |yH| &lt; 2 that are in of the the four pT(H) ranges 300-450 GeV, 450-650 GeV, 650-1000 GeV, and &gt; 1 TeV.
DOI: 10.17182/hepdata.102316.v1/t1
title: "Figure 2.0" of "Antideuteron and anti-helium-3 production in s(NN)**(1/2) = 130-GeV Au + Au collisions."

description: Coalescence parameters $B_2$ and $B_3$ in Au+Au collisions at 130 GeV.
description: The first measurements of light antinucleus production in Au+Au collisions at the Relativistic Heavy-Ion Collider are reported. The observed production rates for $\overline{d}$ and $^3\overline{\mathrm{He}}$ are much larger than in lower energy nucleus-nucleus collisions. A coalescence model analysis of the yields indicates that there is little or no increase in the antinucleon freeze-out volume compared to collisions at CERN SPS energy. These analyses also indicate that the $^3\overline{\mathrm{He}}$ freeze-out volume is smaller than the $\overline{d}$ freeze-out volume.
DOI: 10.17182/hepdata.102316.v1/t2
title: "Table 1.0" of "Antideuteron and anti-helium-3 production in s(NN)**(1/2) = 130-GeV Au + Au collisions."

description: Invariant yields of $\overline{d}$ and $\overline{p}$. Systematic errors are estimated to be 15%.
description: The first measurements of light antinucleus production in Au+Au collisions at the Relativistic Heavy-Ion Collider are reported. The observed production rates for $\overline{d}$ and $^3\overline{\mathrm{He}}$ are much larger than in lower energy nucleus-nucleus collisions. A coalescence model analysis of the yields indicates that there is little or no increase in the antinucleon freeze-out volume compared to collisions at CERN SPS energy. These analyses also indicate that the $^3\overline{\mathrm{He}}$ freeze-out volume is smaller than the $\overline{d}$ freeze-out volume.
DOI: 10.17182/hepdata.102316.v1/t3
title: "Table 1.1" of "Antideuteron and anti-helium-3 production in s(NN)**(1/2) = 130-GeV Au + Au collisions."

description: Invariant yields of $^3\overline{\mathrm{He}}$ and $\overline{p}$. Systematic errors are estimated to be 15%.
description: The first measurements of light antinucleus production in Au+Au collisions at the Relativistic Heavy-Ion Collider are reported. The observed production rates for $\overline{d}$ and $^3\overline{\mathrm{He}}$ are much larger than in lower energy nucleus-nucleus collisions. A coalescence model analysis of the yields indicates that there is little or no increase in the antinucleon freeze-out volume compared to collisions at CERN SPS energy. These analyses also indicate that the $^3\overline{\mathrm{He}}$ freeze-out volume is smaller than the $\overline{d}$ freeze-out volume.
DOI: 10.17182/hepdata.102317.v1/t2
title: "Figure 2.1" of "Midrapidity phi production in Au+Au collisions at sNN =130 GeV"

description: Transverse mass distriution of $\phi$ for 11-26% centrality in Au+Au collisions at 130 GeV.
description: We present the first measurement of midrapidity vector meson $\phi$ production in Au+Au collisions at RHIC ($\sqrt{s_{_{NN}}}$ = 130 GeV) from from the STAR detector. For the 11% highest multiplicity collisions, the slope parameter from an exponential fit to the transverse mass distribution is $T=379\pm50({\rm stat})\pm45({\rm syst})$ MeV, the yield $dN/dy = 5.73\pm0.37({\rm stat})\pm0.69({\rm syst})$ per event, and the ratio $N_\phi/N_h^-$ is found to be $0.021\pm0.001({\rm stat})\pm0.04({\rm syst})$. The measured ratio $N_\phi/N_h^-$ and $T$ for the $\phi$ meson at midrapidity do not change for the selected multiplicity bins.
DOI: 10.17182/hepdata.102317.v1/t1
title: "Figure 2.0" of "Midrapidity phi production in Au+Au collisions at sNN =130 GeV"

description: Transverse mass distriution of $\phi$ for 0-11% centrality in Au+Au collisions at 130 GeV.
description: We present the first measurement of midrapidity vector meson $\phi$ production in Au+Au collisions at RHIC ($\sqrt{s_{_{NN}}}$ = 130 GeV) from from the STAR detector. For the 11% highest multiplicity collisions, the slope parameter from an exponential fit to the transverse mass distribution is $T=379\pm50({\rm stat})\pm45({\rm syst})$ MeV, the yield $dN/dy = 5.73\pm0.37({\rm stat})\pm0.69({\rm syst})$ per event, and the ratio $N_\phi/N_h^-$ is found to be $0.021\pm0.001({\rm stat})\pm0.04({\rm syst})$. The measured ratio $N_\phi/N_h^-$ and $T$ for the $\phi$ meson at midrapidity do not change for the selected multiplicity bins.
DOI: 10.17182/hepdata.102317.v1/t3
title: "Figure 2.2" of "Midrapidity phi production in Au+Au collisions at sNN =130 GeV"

description: Transverse mass distriution of $\phi$ for 26-85% centrality in Au+Au collisions at 130 GeV.
description: We present the first measurement of midrapidity vector meson $\phi$ production in Au+Au collisions at RHIC ($\sqrt{s_{_{NN}}}$ = 130 GeV) from from the STAR detector. For the 11% highest multiplicity collisions, the slope parameter from an exponential fit to the transverse mass distribution is $T=379\pm50({\rm stat})\pm45({\rm syst})$ MeV, the yield $dN/dy = 5.73\pm0.37({\rm stat})\pm0.69({\rm syst})$ per event, and the ratio $N_\phi/N_h^-$ is found to be $0.021\pm0.001({\rm stat})\pm0.04({\rm syst})$. The measured ratio $N_\phi/N_h^-$ and $T$ for the $\phi$ meson at midrapidity do not change for the selected multiplicity bins.
DOI: 10.17182/hepdata.102318.v1/t2
title: "Figure 2.1" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of $K_s^0$ as a function of $p_T$ for 11-45% centrality in Au+Au collisions at 130 GeV. Systematic errors of $\pm$0.005 for particle identification and background subtraction and $^{+0}_{-0.005}$ for nonflow effects.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102318.v1/t3
title: "Figure 2.2" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of $\Lambda+\bar{\Lambda}$ as a function of $p_T$ for 0-11% centrality in Au+Au collisions at 130 GeV. Systematic errors of $\pm$0.005 for particle identification and background subtraction and $^{+0}_{-0.005}$ for nonflow effects.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102318.v1/t4
title: "Figure 2.3" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of $\Lambda+\bar{\Lambda}$ as a function of $p_T$ for 11-45% centrality in Au+Au collisions at 130 GeV. Systematic errors of $\pm$0.005 for particle identification and background subtraction and $^{+0}_{-0.005}$ for nonflow effects.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).
DOI: 10.17182/hepdata.102317.v1/t4
title: "Table 1.0" of "Midrapidity phi production in Au+Au collisions at sNN =130 GeV"

description: Slope parameter T, dN/y, $N_\phi/N_h^-$. Systematic uncertainties on T are 12%, on dN/dy are 12%, and on $N_{\phi}/N_{h^-}$ are 22%.
description: We present the first measurement of midrapidity vector meson $\phi$ production in Au+Au collisions at RHIC ($\sqrt{s_{_{NN}}}$ = 130 GeV) from from the STAR detector. For the 11% highest multiplicity collisions, the slope parameter from an exponential fit to the transverse mass distribution is $T=379\pm50({\rm stat})\pm45({\rm syst})$ MeV, the yield $dN/dy = 5.73\pm0.37({\rm stat})\pm0.69({\rm syst})$ per event, and the ratio $N_\phi/N_h^-$ is found to be $0.021\pm0.001({\rm stat})\pm0.04({\rm syst})$. The measured ratio $N_\phi/N_h^-$ and $T$ for the $\phi$ meson at midrapidity do not change for the selected multiplicity bins.
DOI: 10.17182/hepdata.102318.v1/t1
title: "Figure 2.0" of "Azimuthal anisotropy of K0(S) and Lambda + anti-Lambda production at mid-rapidity from Au + Au collisions at s(NN)**(1/2) = 130-GeV."

description: $v_2$ of $K_s^0$ as a function of $p_T$ for 0-11% centrality in Au+Au collisions at 130 GeV. Systematic errors of $\pm$0.005 for particle identification and background subtraction and $^{+0}_{-0.005}$ for nonflow effects.
description: We report STAR results on the azimuthal anisotropy parameter $v_2$ for strange particles $K_s^0$, $\Lambda$, and $\bar{\Lambda}$ at midrapidity in Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 130 GeV at the Relativistic Heavy Ion Collider. The value of $v_2$ as a function of transverse momentum, $p_T$, of the produced particle and collision centrality is presented for both particles up to $p_T\sim3.0$ GeV/$c$. A strong $p_T$ dependence in $v_2$ is observed up to 2.0 GeV/$c$. The $v_2$ measurement is compared with hydrodynamic model calculations. The physics implications of the $p_T$ integrated $v_2$ magnitude as a function of particle mass are also discussed. An erratum of this paper can be found in Phys. Rev. Lett. 127, 089901 (2021).