cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.70761.v1/t2
title: "Table 2" of "Search for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisions"

description: likelihood scan of the (gg$\rightarrow\phi\rightarrow\tau\tau$) - (gg$\rightarrow$bb$\phi\rightarrow\tau\tau$) - plane the with 40000 grid points at each hypothetical higgs mass, m$_\phi$, at $\sqrt{s}$ = 8 TeV testing the $\textbf{asimov dataset of the sum of all backgrounds not including the Standard Model Higgs boson at 125 GeV against a background hypothesis not including the Standard Model Higgs boson at 125 GeV}.
description: A search for neutral Higgs bosons in the minimal supersymmetric extension of the standard model (MSSM) decaying to tau-lepton pairs in pp collisions is performed, using events recorded by the CMS experiment at the LHC. The dataset corresponds to an integrated luminosity of 24.6 fb$^{-1}$, with 4.9 fb$^{-1}$ at 7 TeV and 19.7 fb$^{-1}$ at 8 TeV. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes the case where the Higgs boson is produced in association with a b-quark jet. No excess is observed in the tau-lepton-pair invariant mass spectrum. Exclusion limits are presented in the MSSM parameter space for different benchmark scenarios, $m_\mathrm{h}^\text{max}$, $m_\mathrm{h}^{\text{mod}+}$, $m_\mathrm{h}^{\text{mod}-}$, light-stop, light-stau, $\tau$-phobic, and low-$m_\mathrm{H}$. Upper limits on the cross section times branching fraction for gluon fusion and b-quark associated Higgs boson production are also given.
DOI: 10.17182/hepdata.70761.v1/t3
title: "Table 3" of "Search for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisions"

description: likelihood scan of the (gg$\rightarrow\phi\rightarrow\tau\tau$) - (gg$\rightarrow$bb$\phi\rightarrow\tau\tau$) - plane the with 40000 grid points at each hypothetical higgs mass, m$_\phi$, at $\sqrt{s}$ = 8 TeV testing the observation against a background hypothesis including the Standard Model Higgs boson at 125 GeV.
description: A search for neutral Higgs bosons in the minimal supersymmetric extension of the standard model (MSSM) decaying to tau-lepton pairs in pp collisions is performed, using events recorded by the CMS experiment at the LHC. The dataset corresponds to an integrated luminosity of 24.6 fb$^{-1}$, with 4.9 fb$^{-1}$ at 7 TeV and 19.7 fb$^{-1}$ at 8 TeV. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes the case where the Higgs boson is produced in association with a b-quark jet. No excess is observed in the tau-lepton-pair invariant mass spectrum. Exclusion limits are presented in the MSSM parameter space for different benchmark scenarios, $m_\mathrm{h}^\text{max}$, $m_\mathrm{h}^{\text{mod}+}$, $m_\mathrm{h}^{\text{mod}-}$, light-stop, light-stau, $\tau$-phobic, and low-$m_\mathrm{H}$. Upper limits on the cross section times branching fraction for gluon fusion and b-quark associated Higgs boson production are also given.
DOI: 10.17182/hepdata.70761.v1/t4
title: "Table 4" of "Search for neutral MSSM Higgs bosons decaying to a pair of tau leptons in pp collisions"

description: likelihood scan of the (gg$\rightarrow\phi\rightarrow\tau\tau$) - (gg$\rightarrow$bb$\phi\rightarrow\tau\tau$) - plane the with 40000 grid points at each hypothetical higgs mass, m$_\phi$, at $\sqrt{s}$ = 8 TeV testing an asimov dataset of the sum of all backgrounds including the Standard Model Higgs boson at 125 GeV against a background hypothesis including the Standard Model Higgs boson at 125 GeV.
description: A search for neutral Higgs bosons in the minimal supersymmetric extension of the standard model (MSSM) decaying to tau-lepton pairs in pp collisions is performed, using events recorded by the CMS experiment at the LHC. The dataset corresponds to an integrated luminosity of 24.6 fb$^{-1}$, with 4.9 fb$^{-1}$ at 7 TeV and 19.7 fb$^{-1}$ at 8 TeV. To enhance the sensitivity to neutral MSSM Higgs bosons, the search includes the case where the Higgs boson is produced in association with a b-quark jet. No excess is observed in the tau-lepton-pair invariant mass spectrum. Exclusion limits are presented in the MSSM parameter space for different benchmark scenarios, $m_\mathrm{h}^\text{max}$, $m_\mathrm{h}^{\text{mod}+}$, $m_\mathrm{h}^{\text{mod}-}$, light-stop, light-stau, $\tau$-phobic, and low-$m_\mathrm{H}$. Upper limits on the cross section times branching fraction for gluon fusion and b-quark associated Higgs boson production are also given.
DOI: 10.17182/hepdata.70762.v1/t1
title: "Table 1" of "Dijet production in $\sqrt{s}=7$ TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment"

description: The cross section differential in the forward rapidity gap size, DELTA(C=RAPGAP), for events with at least two jets of pt &gt; 20 GeV found by the anti-kt jet algorithm with R=0.6.
description: CERN-LHC. Measurements of the pseudorapidity gap and xi distributions for dijet production in diffractive events which are defined by large gaps devoid of activity seen in the ATLAS detector, based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV of integrated luminosity of 6.8 nb-1 collected in 2010. The final state consists of two jets found by the anti-kt jet algorithm with transverse momentum greater than 20 GeV and empty regions in the acceptance of the ATLAS detector. The pseudorapidity gap variable, denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.8, in which no final state particles are observed above a (transverse) momentum threshold. The xi variable is calculated using M**2/S and for Single Diffraction DELTA(C=RAPGAP)~=-ln(xi). See PLBXX (2015) YY for more details.

The fiducial region is defined as:
The jet finding uses the anti-kt algorithm with radius R=0.6 or R=0.4 
- all stable particles are used except for muons and neutrinos
- at least 2 jets with ptJet1 &gt; 20 GeV and ptJet2 &gt; 20 GeV
- at least 2 jets with |etaJet1| &lt; 4.4 and |etaJet2| &lt; 4.4

The selection of particles for the gap finding:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV .or. ptParticleCharged &gt; 0.2 GeV
- The gap finding: two gaps are formed defined as the regions without particles
from the edge of the calorimeter at eta=4.8 or eta=-4.8. The larger of the two
is the final gap. 

The selection of particles for the xi calculation:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV 
- The xi value is calculated as Sum [ptParticle*exp(+-etaParticle)/sqrt(S)] where the sum loops over the particles selected above and the exponential function takes the positive (negative) sign if the gap starts at eta = +4.8 (-4.8).

In the tables the individual sources of systematic uncertainty are given in per cent and are described as follows:
dJES = jet energy scale uncertainty
dJER = jet energy resolution uncertainty
dJAR = jet angular resolution uncertainty
dJRE = jet reconstruction efficiency uncertainty
dClustE = cluster energy scale uncertainty
dCST = cell significance threshold uncertainty 
dJCE = jet cleaning efficiency uncertainty
dUnf = unfolding procedure uncertainty
dMod = model uncertainty
dTrig = jet trigger efficiency uncertainty
dtrack = tracking efficiency uncertainty
dlum = luminosity uncertainty
dmat = added material uncertainty.
DOI: 10.17182/hepdata.70762.v1/t2
title: "Table 2" of "Dijet production in $\sqrt{s}=7$ TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment"

description: The cross section differential in the forward rapidity gap size, DELTA(C=RAPGAP), for events with at least two jets of pt &gt; 20 GeV found by the anti-kt jet algorithm with R=0.4.
description: CERN-LHC. Measurements of the pseudorapidity gap and xi distributions for dijet production in diffractive events which are defined by large gaps devoid of activity seen in the ATLAS detector, based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV of integrated luminosity of 6.8 nb-1 collected in 2010. The final state consists of two jets found by the anti-kt jet algorithm with transverse momentum greater than 20 GeV and empty regions in the acceptance of the ATLAS detector. The pseudorapidity gap variable, denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.8, in which no final state particles are observed above a (transverse) momentum threshold. The xi variable is calculated using M**2/S and for Single Diffraction DELTA(C=RAPGAP)~=-ln(xi). See PLBXX (2015) YY for more details.

The fiducial region is defined as:
The jet finding uses the anti-kt algorithm with radius R=0.6 or R=0.4 
- all stable particles are used except for muons and neutrinos
- at least 2 jets with ptJet1 &gt; 20 GeV and ptJet2 &gt; 20 GeV
- at least 2 jets with |etaJet1| &lt; 4.4 and |etaJet2| &lt; 4.4

The selection of particles for the gap finding:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV .or. ptParticleCharged &gt; 0.2 GeV
- The gap finding: two gaps are formed defined as the regions without particles
from the edge of the calorimeter at eta=4.8 or eta=-4.8. The larger of the two
is the final gap. 

The selection of particles for the xi calculation:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV 
- The xi value is calculated as Sum [ptParticle*exp(+-etaParticle)/sqrt(S)] where the sum loops over the particles selected above and the exponential function takes the positive (negative) sign if the gap starts at eta = +4.8 (-4.8).

In the tables the individual sources of systematic uncertainty are given in per cent and are described as follows:
dJES = jet energy scale uncertainty
dJER = jet energy resolution uncertainty
dJAR = jet angular resolution uncertainty
dJRE = jet reconstruction efficiency uncertainty
dClustE = cluster energy scale uncertainty
dCST = cell significance threshold uncertainty 
dJCE = jet cleaning efficiency uncertainty
dUnf = unfolding procedure uncertainty
dMod = model uncertainty
dTrig = jet trigger efficiency uncertainty
dtrack = tracking efficiency uncertainty
dlum = luminosity uncertainty
dmat = added material uncertainty.
DOI: 10.17182/hepdata.70762.v1/t3
title: "Table 3" of "Dijet production in $\sqrt{s}=7$ TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment"

description: The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt &gt; 20 GeV found by the anti-kt jet algorithm with R=0.6.
description: CERN-LHC. Measurements of the pseudorapidity gap and xi distributions for dijet production in diffractive events which are defined by large gaps devoid of activity seen in the ATLAS detector, based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV of integrated luminosity of 6.8 nb-1 collected in 2010. The final state consists of two jets found by the anti-kt jet algorithm with transverse momentum greater than 20 GeV and empty regions in the acceptance of the ATLAS detector. The pseudorapidity gap variable, denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.8, in which no final state particles are observed above a (transverse) momentum threshold. The xi variable is calculated using M**2/S and for Single Diffraction DELTA(C=RAPGAP)~=-ln(xi). See PLBXX (2015) YY for more details.

The fiducial region is defined as:
The jet finding uses the anti-kt algorithm with radius R=0.6 or R=0.4 
- all stable particles are used except for muons and neutrinos
- at least 2 jets with ptJet1 &gt; 20 GeV and ptJet2 &gt; 20 GeV
- at least 2 jets with |etaJet1| &lt; 4.4 and |etaJet2| &lt; 4.4

The selection of particles for the gap finding:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV .or. ptParticleCharged &gt; 0.2 GeV
- The gap finding: two gaps are formed defined as the regions without particles
from the edge of the calorimeter at eta=4.8 or eta=-4.8. The larger of the two
is the final gap. 

The selection of particles for the xi calculation:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV 
- The xi value is calculated as Sum [ptParticle*exp(+-etaParticle)/sqrt(S)] where the sum loops over the particles selected above and the exponential function takes the positive (negative) sign if the gap starts at eta = +4.8 (-4.8).

In the tables the individual sources of systematic uncertainty are given in per cent and are described as follows:
dJES = jet energy scale uncertainty
dJER = jet energy resolution uncertainty
dJAR = jet angular resolution uncertainty
dJRE = jet reconstruction efficiency uncertainty
dClustE = cluster energy scale uncertainty
dCST = cell significance threshold uncertainty 
dJCE = jet cleaning efficiency uncertainty
dUnf = unfolding procedure uncertainty
dMod = model uncertainty
dTrig = jet trigger efficiency uncertainty
dtrack = tracking efficiency uncertainty
dlum = luminosity uncertainty
dmat = added material uncertainty.
DOI: 10.17182/hepdata.70762.v1/t4
title: "Table 4" of "Dijet production in $\sqrt{s}=7$ TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment"

description: The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt &gt; 20 GeV found by the anti-kt jet algorithm with R=0.4.
description: CERN-LHC. Measurements of the pseudorapidity gap and xi distributions for dijet production in diffractive events which are defined by large gaps devoid of activity seen in the ATLAS detector, based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV of integrated luminosity of 6.8 nb-1 collected in 2010. The final state consists of two jets found by the anti-kt jet algorithm with transverse momentum greater than 20 GeV and empty regions in the acceptance of the ATLAS detector. The pseudorapidity gap variable, denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.8, in which no final state particles are observed above a (transverse) momentum threshold. The xi variable is calculated using M**2/S and for Single Diffraction DELTA(C=RAPGAP)~=-ln(xi). See PLBXX (2015) YY for more details.

The fiducial region is defined as:
The jet finding uses the anti-kt algorithm with radius R=0.6 or R=0.4 
- all stable particles are used except for muons and neutrinos
- at least 2 jets with ptJet1 &gt; 20 GeV and ptJet2 &gt; 20 GeV
- at least 2 jets with |etaJet1| &lt; 4.4 and |etaJet2| &lt; 4.4

The selection of particles for the gap finding:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV .or. ptParticleCharged &gt; 0.2 GeV
- The gap finding: two gaps are formed defined as the regions without particles
from the edge of the calorimeter at eta=4.8 or eta=-4.8. The larger of the two
is the final gap. 

The selection of particles for the xi calculation:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV 
- The xi value is calculated as Sum [ptParticle*exp(+-etaParticle)/sqrt(S)] where the sum loops over the particles selected above and the exponential function takes the positive (negative) sign if the gap starts at eta = +4.8 (-4.8).

In the tables the individual sources of systematic uncertainty are given in per cent and are described as follows:
dJES = jet energy scale uncertainty
dJER = jet energy resolution uncertainty
dJAR = jet angular resolution uncertainty
dJRE = jet reconstruction efficiency uncertainty
dClustE = cluster energy scale uncertainty
dCST = cell significance threshold uncertainty 
dJCE = jet cleaning efficiency uncertainty
dUnf = unfolding procedure uncertainty
dMod = model uncertainty
dTrig = jet trigger efficiency uncertainty
dtrack = tracking efficiency uncertainty
dlum = luminosity uncertainty
dmat = added material uncertainty.
DOI: 10.17182/hepdata.70762.v1/t5
title: "Table 5" of "Dijet production in $\sqrt{s}=7$ TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment"

description: The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt &gt; 20 GeV found by the anti-kt jet algorithm with R=0.6 and after requiring that the pseudorapidity gap &gt; 2.
description: CERN-LHC. Measurements of the pseudorapidity gap and xi distributions for dijet production in diffractive events which are defined by large gaps devoid of activity seen in the ATLAS detector, based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV of integrated luminosity of 6.8 nb-1 collected in 2010. The final state consists of two jets found by the anti-kt jet algorithm with transverse momentum greater than 20 GeV and empty regions in the acceptance of the ATLAS detector. The pseudorapidity gap variable, denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.8, in which no final state particles are observed above a (transverse) momentum threshold. The xi variable is calculated using M**2/S and for Single Diffraction DELTA(C=RAPGAP)~=-ln(xi). See PLBXX (2015) YY for more details.

The fiducial region is defined as:
The jet finding uses the anti-kt algorithm with radius R=0.6 or R=0.4 
- all stable particles are used except for muons and neutrinos
- at least 2 jets with ptJet1 &gt; 20 GeV and ptJet2 &gt; 20 GeV
- at least 2 jets with |etaJet1| &lt; 4.4 and |etaJet2| &lt; 4.4

The selection of particles for the gap finding:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV .or. ptParticleCharged &gt; 0.2 GeV
- The gap finding: two gaps are formed defined as the regions without particles
from the edge of the calorimeter at eta=4.8 or eta=-4.8. The larger of the two
is the final gap. 

The selection of particles for the xi calculation:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV 
- The xi value is calculated as Sum [ptParticle*exp(+-etaParticle)/sqrt(S)] where the sum loops over the particles selected above and the exponential function takes the positive (negative) sign if the gap starts at eta = +4.8 (-4.8).

In the tables the individual sources of systematic uncertainty are given in per cent and are described as follows:
dJES = jet energy scale uncertainty
dJER = jet energy resolution uncertainty
dJAR = jet angular resolution uncertainty
dJRE = jet reconstruction efficiency uncertainty
dClustE = cluster energy scale uncertainty
dCST = cell significance threshold uncertainty 
dJCE = jet cleaning efficiency uncertainty
dUnf = unfolding procedure uncertainty
dMod = model uncertainty
dTrig = jet trigger efficiency uncertainty
dtrack = tracking efficiency uncertainty
dlum = luminosity uncertainty
dmat = added material uncertainty.
DOI: 10.17182/hepdata.70762.v1/t6
title: "Table 6" of "Dijet production in $\sqrt{s}=7$ TeV $pp$ collisions with large rapidity gaps at the ATLAS experiment"

description: The cross section differential in the fraction of the proton four-momentum carried by the Pomeron, LOG10(C=XI), for events with at least two jets of pt &gt; 20 GeV found by the anti-kt jet algorithm with R=0.4 and after requiring that the pseudorapidity gap &gt; 2.
description: CERN-LHC. Measurements of the pseudorapidity gap and xi distributions for dijet production in diffractive events which are defined by large gaps devoid of activity seen in the ATLAS detector, based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV of integrated luminosity of 6.8 nb-1 collected in 2010. The final state consists of two jets found by the anti-kt jet algorithm with transverse momentum greater than 20 GeV and empty regions in the acceptance of the ATLAS detector. The pseudorapidity gap variable, denoted here as DELTA(C=RAPGAP), is defined as the larger of the pseudorapidity regions extending to the limits of the ATLAS detector sensitivity at eta=+-4.8, in which no final state particles are observed above a (transverse) momentum threshold. The xi variable is calculated using M**2/S and for Single Diffraction DELTA(C=RAPGAP)~=-ln(xi). See PLBXX (2015) YY for more details.

The fiducial region is defined as:
The jet finding uses the anti-kt algorithm with radius R=0.6 or R=0.4 
- all stable particles are used except for muons and neutrinos
- at least 2 jets with ptJet1 &gt; 20 GeV and ptJet2 &gt; 20 GeV
- at least 2 jets with |etaJet1| &lt; 4.4 and |etaJet2| &lt; 4.4

The selection of particles for the gap finding:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV .or. ptParticleCharged &gt; 0.2 GeV
- The gap finding: two gaps are formed defined as the regions without particles
from the edge of the calorimeter at eta=4.8 or eta=-4.8. The larger of the two
is the final gap. 

The selection of particles for the xi calculation:
- |etaParticle| &lt; 4.8
- pParticleNeutral &gt; 0.2 GeV
- pParticleCharged &gt; 0.5 GeV 
- The xi value is calculated as Sum [ptParticle*exp(+-etaParticle)/sqrt(S)] where the sum loops over the particles selected above and the exponential function takes the positive (negative) sign if the gap starts at eta = +4.8 (-4.8).

In the tables the individual sources of systematic uncertainty are given in per cent and are described as follows:
dJES = jet energy scale uncertainty
dJER = jet energy resolution uncertainty
dJAR = jet angular resolution uncertainty
dJRE = jet reconstruction efficiency uncertainty
dClustE = cluster energy scale uncertainty
dCST = cell significance threshold uncertainty 
dJCE = jet cleaning efficiency uncertainty
dUnf = unfolding procedure uncertainty
dMod = model uncertainty
dTrig = jet trigger efficiency uncertainty
dtrack = tracking efficiency uncertainty
dlum = luminosity uncertainty
dmat = added material uncertainty.
DOI: 10.17182/hepdata.70773.v1/t1
title: "Table 1" of "K-minus-p interactions from 594 to 820 mev/c"

description: No description provided.
description: THE FOLLOWING COMMENTS ARE TAKEN FROM THE PI N COMPILATION OF R.L. KELLY. THEY ARE THAT COMPILATION'S COMPLETE SET OF COMMENTS FOR PAPERS RELATED TO THE SAME EXPERIMENT (DESIGNATED BERTANZA69) AS THE CURRENT PAPER. (THE IDENTIFIER PRECEDING THE REFERENCE AND COMMENT FOR EACH PAPER IS FOR CROSS-REFERENCING WITHIN THESE COMMENTS ONLY AND DOES NOT NECESSARILY AGREE WITH THE SHORT CODE USED ELSEWHERE IN THE PRESENT COMPILATION.) /// BERTANZA69 [L. BERTANZA,PR 177,2036(1969)] -- K- P AND PI- P EXPOSURE TAKEN IN COLUMBIA-BNL 30-INCH HBC AT THE AGS. PI- P DCS DATA AT 708,725,741,768,AND 802 MEV/C. /// BERTANZA68 [L. BERTANZA,PREPRINT(POSSIBLY CERN-8990),1968.] -- DATA READ FROM GRAPH. PREPRINT VERSION OF BERTANZA69 WITH LARGER GRAPHS. /// BERLEY65 [D. BERLEY,PRL 15,641(1965)] -- FIRST PUBLICATION OF K- P TO LAMBDA ETA RESULTS FROM THIS EXPOSURE. /// BERLEY66 [D. BERLEY,PRL 16,162(1966)] -- ERRATA FOR BERLEY65.. DATA ARE UNNORMALIZED OR NORMALIZED TO OTHER DATA.
The PI- P data is given for comparison in the paper (note added by MRW 19.1.2016).