cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.110691.v2/t288
title: "Advanced $\mathrm{S_{T}}$ full table" of "Inclusive nonresonant multilepton probes of new phenomena at $\sqrt{s}$ = 13 TeV"

description: The SR distributions of the Advanced $\mathrm{S_{T}}$ table for the combined 2016-2018 data set. The detailed description of the bin numbers can be found in Tables 3-6 in the paper. The lower panel shows the ratio of observed events to the total expected background prediction. The gray band on the ratio represents the sum of statistical and systematic uncertainties in the SM background predictions. The expected SM background distributions and the uncertainties are shown before fitting the data under the background-only hypothesis. For illustration, an example signal hypothesis for the production of the scalar leptoquark coupled to a top quark and a muon for $\mathrm{m_{S}}$ = 1.4 TeV, before the fit, is also overlaid.
description: An inclusive search for nonresonant signatures of beyond the standard model (SM) phenomena in events with three or more charged leptons, including hadronically decaying $\tau$ leptons, is presented. The analysis is based on a data sample corresponding to an integrated luminosity of 138 $\mathrm{fb}^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV, collected by the CMS experiment at the LHC in 2016--2018. Events are categorized based on the lepton and b-tagged jet multiplicities and various kinematic variables. Three scenarios of physics beyond the SM are probed, and signal-specific boosted decision trees are used for enhancing sensitivity. No significant deviations from the background expectations are observed. Lower limits are set at 95% confidence level on the mass of type-III seesaw heavy fermions in the range 845--1065 GeV for various decay branching fraction combinations to SM leptons. Doublet and singlet vector-like $\tau$ lepton extensions of the SM are excluded for masses below 1045 GeV and in the mass range 125--150 GeV, respectively. Scalar leptoquarks decaying exclusively to a top quark and a lepton are excluded below 1.12--1.42 TeV, depending on the lepton flavor. For the type-III seesaw as well as the vector-like doublet model, these constraints are the most stringent to date. For the vector-like singlet model, these are the first constraints from the LHC experiments. Detailed results are also presented to facilitate alternative theoretical interpretations.
DOI: 10.25549/vercoutere-ouc110611043
title: A bridge

description: Road to a bridge through the mountains. Header includes the words: A Bridge
DOI: 10.17182/hepdata.110699.v1/t1
title: "Figure1pp200" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physical Review C87, 054907 (2013)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in p+p at $\sqrt{s_{NN}}$= 200 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t2
title: "Figure1pp624" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physics Letters B94, 106 (1980)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in p+p at $\sqrt{s_{NN}}$= 62.4 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t3
title: "Figure1pp63" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Nucl. Part. Phys. 23, A1 (1997) and Sov. J. Nucl. Phys. 51, 836 (1990)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in p+p at $\sqrt{s_{NN}}$= 63 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t4
title: "Figure1pp63_1" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Nucl. Part. Phys. 23, A1 (1997)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in p+p at $\sqrt{s_{NN}}$= 63 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t5
title: "Figure1pp63_2" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Sov. J. Nucl. Phys. 51, 836 (1990)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in p+p at $\sqrt{s_{NN}}$= 63 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t6
title: "Figure1AuAu624" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Au+Au at $\sqrt{s_{NN}}$= 62.4 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t7
title: "Figure1AuAu39" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Au+Au at $\sqrt{s_{NN}}$= 39.0 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t10
title: "Figure1AuAu200HighpT" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physical Review Letters 109, 152302 (2012)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Au+Au at $\sqrt{s_{NN}}$= 200 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t11
title: "Figure1CuCu200" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physical Review C98, 054902 (2018)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Cu+Cu at $\sqrt{s_{NN}}$= 200 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t12
title: "Figure1PbPb2760" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physics Letters B754 235 (2016)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Pb+Pb at $\sqrt{s_{NN}}$= 2760 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t13
title: "Figure 2" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Number of binary collisions N_{coll} vs. Charged particle multiplicity in Au+Au at various cm energies.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t14
title: "Figure 2-1" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Charged particle multiplicity vs. centrality in Au+Au at various cm energies.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t8
title: "Figure1AuAu200LowpT1" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physical Review C91, 064904 (2015)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Au+Au at $\sqrt{s_{NN}}$= 200 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.17182/hepdata.110699.v1/t9
title: "Figure1AuAu200LowpT2" of "Beam-energy and centrality dependence of direct-photon emission from ultra-relativistic heavy-ion collisions"

description: Direct photon spectra(Physical Review Letters 104, 132301 (2010)) normalized by $(dN_{ch}/d\eta)^{1.25}$ for in Au+Au at $\sqrt{s_{NN}}$= 200 GeV.
description: BNL-RHIC. The PHENIX collaboration presents first measurements of low-momentum (0.4&lt; $p_T$ &lt;3 GeV/$c$) direct-photon yields from Au+Au collisions at $\sqrt{s_{NN}}$=39 and 62.4 GeV. For both beam energies the direct-photon yields are substantially enhanced with respect to expectations from prompt processes, similar to the yields observed in Au+Au collisions at $\sqrt{s_{NN}}$=200. Analyzing the photon yield as a function of the experimental observable $dN_{ch}/d\eta$ reveals that the low-momentum (&gt;1 GeV/$c$) direct-photon yield $dN^{dir}_{\gamma}/d\eta$ is a smooth function of $dN_{ch}/d\eta$ and can be well described as proportional to $(dN_{ch}/d\eta)^\alpha$ with $\alpha\approx1.25$. This scaling behavior holds for a wide range of beam energies at the Relativistic Heavy Ion Collider and the Large Hadron Collider, for centrality selected samples, as well as for different, A+A collision systems. At a given beam energy the scaling also holds for high $p_T$(&gt;5 GeV/$c$) but when results from different collision energies are compared, an additional $\sqrt{s_{NN}}$-dependent multiplicative factor is needed to describe the integrated-direct-photon yield.
DOI: 10.25549/vercoutere-ouc110611087
title: Colorful streaks II

description: Streaks of red, orange, green, navy blue, gray,and tan; denser streaks in the center; swirls of streaks around the center. Notes written by OT: The patient painted an estimated 100 of the same meticculous style to the point of compulsion. When I gave him a full sheet of paper it didn't take long for him to figure out that by folding it in half he had the same size he always used. Published in a text book