cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.64506.v1/t9
title: "Table 9" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The measured E+ E- --&gt; KS KL cross section as a function of the centre-of-mass energy.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t15
title: "Table 15" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; KS KS K+ K-) and the J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t16
title: "Table 16" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; K*(892) KS PI) * BR(K*(892) --&gt; KS PI) and the J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t17
title: "Table 17" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; K2*(1430) KS PI) * BR(K2*(1430) --&gt; KS PI) and the J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t18
title: "Table 18" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; K*(892)+ K*(892)-) * (BR(K*(892) --&gt; KS PI))**2 and the 90% C.L. J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t19
title: "Table 19" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; K2*(1430) K*(892)) * BR(K2*(1430) --&gt; KS PI) * BR(K*(892) --&gt; KS PI) and the 90% C.L. J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t20
title: "Table 20" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; KS KS PHI(1020)) * BR(PHI --&gt; K+ K-) and the J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.26023/5aqh-7gg7-tz0g
title: MITTEN-CI: CopterSonde 3 Offshore Vertical Profiles. Version 1.0

description: Vertical profiles of temperature, relative humidity and winds measured by the InterMet CopterSonde3 that was deployed from a location on the eastern shore of Lake Michigan at the intake facility of the Wyoming, Michigan City Water Plant (northwest of Holland, Michigan) during the Maritime to Inland Transitions Towards ENvironments for Convection Initiation (MITTEN-CI) campaign. Profiles were taken from a point approximately 300m offshore and from about 190 to 800 m ASL.
DOI: 10.17182/hepdata.64506.v1/t21
title: "Table 21" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; F2PRIME(1525) PHI(1020)) * BR(PHI --&gt; K+ K-} * BR(F2PRIME(1525) --&gt; KS KS) and the J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64506.v1/t22
title: "Table 22" of "Cross sections for the reactions $e^+ e^-\to K_S^0 K_L^0$, $K_S^0 K_L^0 \pi^+\pi^-$, $K_S^0 K_S^0 \pi^+\pi^-$, and $K_S^0 K_S^0 K^+K^-$ from events with initial-state radiation"

description: The product WIDTH(E+ E- --&gt; J/PSI) * BR(J/PSI --&gt; F2PRIME(1525) K+ K-) * BR(F2PRIME(1525) --&gt; KS KS) and the J/PSI branching fraction.
description: SLAC-PEP2. We study the processes E+ E- --&gt; KS KL GAMMA, KS KL PI+ PI- GAMMA, KS KS PI+ PI- GAMMA, and KS KS K+ K- GAMMA, where the photon is radiated from the initial state, providing cross section measurements for the hadronic states over a continuum of center-of-mass energies. The results are based on 469 inverse femtobarns of data collected with the BaBar detector at SLAC. We observe the PHI(1020) resonance in the KS KL final state and measure the product of its electronic width and branching fraction with about 3% uncertainty. We present a measurement of the E+ E- --&gt; KS KL cross section in the energy range from 1.06 to 2.2 GeV and observe the production of a resonance at 1.67 GeV. We present the first measurements of the E+ E- --&gt; KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- cross sections, and study the intermediate resonance structures. We obtain the first observations of J/PSI decay to the KS KL PI+ PI-, KS KS PI+ PI-, and KS KS K+ K- final states.
DOI: 10.17182/hepdata.64507.v1/t1
title: "Table 1" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: The stransverse mass distribution in the multi-jet CR-C1N2.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t2
title: "Table 2" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Mt(tau1)+Mt(tau2) distribution in the multi-jet CR C1C1.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t3
title: "Table 3" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Effective mass distribution in the multi-jet CR DS-highMass.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t4
title: "Table 4" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Effective mass distribution in the multi-jet CR DS-lowMass.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t5
title: "Table 5" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Distribution of Met in the W+jets control region with 20.3/fb.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t6
title: "Table 6" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Distribution of Meff in the W+jets control region with 20.3/fb.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.
DOI: 10.17182/hepdata.64507.v1/t7
title: "Table 7" of "Search for the direct production of charginos, neutralinos and staus in final states with at least two hadronically decaying taus and missing transverse momentum in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector"

description: Distribution of Mt2 in the W+jets control region with 20.3/fb.
description: CERN-LHC. Results of a search for the electroweak associated production of charginos and next-to-lightest neutralinos, pairs of charginos or pairs of tau sleptons are presented. These processes are characterised by final states with at least two hadronically decaying tau leptons, missing transverse momentum and low jet activity. The analysis is based on an integrated luminosity of 20.3 fb-1 of proton-proton collisions at sqrt(s) = 8 TeV recorded with the ATLAS experiment at the Large Hadron Collider. No significant excess is observed with respect to the predictions from Standard Model processes. Limits are set at 95% confidence level on the masses of the lighter chargino and next-to-lightest neutralino for various hypotheses for the lightest neutralino mass in simplified models. In the scenario of direct production of chargino pairs, with each chargino decaying into the lightest neutralino via an intermediate tau slepton, chargino masses up to 345 GeV are excluded for a massless lightest neutralino. For associated production of mass-degenerate charginos and next-to-lightest neutralinos, both decaying into the lightest neutralino via an intermediate tau slepton, masses up to 410 GeV are excluded for a massless lightest neutralino.