cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.52862.v1/t3
title: "Table 3" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 3-jet Dalitz X4 distribution.
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t4
title: "Table 4" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 4-jet Dalitz X3 distribution.
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t5
title: "Table 5" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 4-jet Dalitz X4 distribution.
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t7
title: "Table 7" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 5-jet Dalitz X4 distribution.
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t10
title: "Table 10" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 4-jet angular distribution in COS(THETA(3)).
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t11
title: "Table 11" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 4-jet angular distribution in CHI(3).
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t12
title: "Table 12" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 5-jet angular distribution in COS(THETA(3)).
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t13
title: "Table 13" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 5-jet angular distribution in CHI(3).
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t14
title: "Table 14" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Single-jet mass fraction distributions in 3-jet events.
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t6
title: "Table 6" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 5-jet Dalitz X3 distribution.
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t8
title: "Table 8" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 3-jet angular distribution in COS(THETA(3)).
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.
DOI: 10.17182/hepdata.52862.v1/t9
title: "Table 9" of "Further Properties of High-Mass Multijet Events at the Fermilab Proton-Antiproton Collider"

description: Inclusive 3-jet angular distribution in CHI(3).
description: Fermilab-Tevatron. Properties of high-mass multijet events produced in proton-antiproton collisions at centre-of-mass energy of 1.8 TeV.. This paper gives the following distributions of 3-, 4- and 5- jet data where the final states jets, numbered 3, 4 and 5 are such that the jet energies areordered as E3 & gt; E4 & gt; E5.. 1 - Inclusive multijet mass distributions.. 2 - Distibutions in the Dalitiz variables X3 and X4 defined as XJ = EJ/(3-jet Mass). For thisthe 4-jet systems are reduced to 3-jet systems by combining the two jets with the lowest 2-jet mass. In a similar way 5-jet systems are firstreduced to 4-jet systems by first combining the two jets with lowest 2-jet mass , and then likewise into 3-jet systems.. 3 - Distributions of COS(THETA(3)) of the angle of the leading jet scattering angle.. 4 - Distributions in CHI(3), the angle between the 3-jet plane and the plane containing the leading-jet and the average beam direction in the 3-jet resty-frame.. 5 - The single jet-mass fractions F3, F4 and F5 where FJ=M(J)/M(3JET).. 6 - Two body energy sharing variables XA (=EA/(EA+EB))and XB(=EB/(EA+EB)) in the multijet rets-frame where A and B are the two systems combined together in 4-jet and 5-jet events and EA & gt; EB. XC and XD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The normalized masses FA=MA/M(n-jet) and FB=MB/M(n-jet).FC and FD are the corresponding variables in the reduction of 5-jet to 4-jet events.. The two body angular variable COS(CHI(AB)) defined in the n-jet rest frameas the angle between the plane containing the (AB) system and the average beam direction and the plane containing A and B. COS(CHI(CD)) is the corresponding variable in the reduction of 5-jet to 4-jet events.. All data have been read from the plots.