cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.156184.v1/t4
title: "Figure 8b" of "Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV"

description: The groomed momentum balance distribution of b jets.
description: A measurement of the substructure of bottom quark jets (b jets) in proton-proton (pp) collisions is presented. The measurement uses data collected in pp collisions at $\sqrt{s}$ = 5.02 TeV recorded by the CMS experiment in 2017, corresponding to an integrated luminosity of 301 pb$^{-1}$. The soft-drop-groomed jet radius, $R_{g}$, and momentum balance, $z_{g}$, of b quark jets are presented. These observables can be used to test perturbative quantum chromodynamics predictions that account for mass effects. An algorithm to identify and cluster the charged decay daughters of b hadrons is developed for this analysis, which facilitates the exposure of the gluon radiation pattern of b jets using iterative Cambridge--Aachen declustering. Because the b hadron is partially reconstructed from its charged decay daughters, only charged particles are used for the jet substructure studies. In addition, a jet fragmentation function, $z_{b,ch}$, is measured, which is defined as the distribution of the ratio of the transverse momentum ($p_{T}$) of the partially reconstructed b hadron with respect to the charged-particle component of the jet $p_{T}$. The measured distributions are unfolded to the charged-particle level. The b jet substructure is compared to that of inclusive jets, which are dominated by light-quark and gluon jets, to assess the role of the b quark mass. A strong suppression of emissions at small $R_{g}$ values is observed for b jets when compared to inclusive jets, consistent with the dead-cone effect. The measurements are also compared with theoretical predictions from Monte Carlo event generators. This is the first b jet substructure study that clusters together the b hadron decay daughters.
DOI: 10.17182/hepdata.156184.v1/t5
title: "Figure 9" of "Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV"

description: The jet fragmentation function distribution of b jets.
description: A measurement of the substructure of bottom quark jets (b jets) in proton-proton (pp) collisions is presented. The measurement uses data collected in pp collisions at $\sqrt{s}$ = 5.02 TeV recorded by the CMS experiment in 2017, corresponding to an integrated luminosity of 301 pb$^{-1}$. The soft-drop-groomed jet radius, $R_{g}$, and momentum balance, $z_{g}$, of b quark jets are presented. These observables can be used to test perturbative quantum chromodynamics predictions that account for mass effects. An algorithm to identify and cluster the charged decay daughters of b hadrons is developed for this analysis, which facilitates the exposure of the gluon radiation pattern of b jets using iterative Cambridge--Aachen declustering. Because the b hadron is partially reconstructed from its charged decay daughters, only charged particles are used for the jet substructure studies. In addition, a jet fragmentation function, $z_{b,ch}$, is measured, which is defined as the distribution of the ratio of the transverse momentum ($p_{T}$) of the partially reconstructed b hadron with respect to the charged-particle component of the jet $p_{T}$. The measured distributions are unfolded to the charged-particle level. The b jet substructure is compared to that of inclusive jets, which are dominated by light-quark and gluon jets, to assess the role of the b quark mass. A strong suppression of emissions at small $R_{g}$ values is observed for b jets when compared to inclusive jets, consistent with the dead-cone effect. The measurements are also compared with theoretical predictions from Monte Carlo event generators. This is the first b jet substructure study that clusters together the b hadron decay daughters.
DOI: 10.17182/hepdata.156184.v1/t6
title: "Figure 11a" of "Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV"

description: The b jet to inclusive jet ratio of the groomed jet radius distributions.
description: A measurement of the substructure of bottom quark jets (b jets) in proton-proton (pp) collisions is presented. The measurement uses data collected in pp collisions at $\sqrt{s}$ = 5.02 TeV recorded by the CMS experiment in 2017, corresponding to an integrated luminosity of 301 pb$^{-1}$. The soft-drop-groomed jet radius, $R_{g}$, and momentum balance, $z_{g}$, of b quark jets are presented. These observables can be used to test perturbative quantum chromodynamics predictions that account for mass effects. An algorithm to identify and cluster the charged decay daughters of b hadrons is developed for this analysis, which facilitates the exposure of the gluon radiation pattern of b jets using iterative Cambridge--Aachen declustering. Because the b hadron is partially reconstructed from its charged decay daughters, only charged particles are used for the jet substructure studies. In addition, a jet fragmentation function, $z_{b,ch}$, is measured, which is defined as the distribution of the ratio of the transverse momentum ($p_{T}$) of the partially reconstructed b hadron with respect to the charged-particle component of the jet $p_{T}$. The measured distributions are unfolded to the charged-particle level. The b jet substructure is compared to that of inclusive jets, which are dominated by light-quark and gluon jets, to assess the role of the b quark mass. A strong suppression of emissions at small $R_{g}$ values is observed for b jets when compared to inclusive jets, consistent with the dead-cone effect. The measurements are also compared with theoretical predictions from Monte Carlo event generators. This is the first b jet substructure study that clusters together the b hadron decay daughters.
DOI: 10.17182/hepdata.156184.v1/t7
title: "Figure 11b" of "Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV"

description: The b jet to inclusive jet ratio of the groomed momentum balance distributions.
description: A measurement of the substructure of bottom quark jets (b jets) in proton-proton (pp) collisions is presented. The measurement uses data collected in pp collisions at $\sqrt{s}$ = 5.02 TeV recorded by the CMS experiment in 2017, corresponding to an integrated luminosity of 301 pb$^{-1}$. The soft-drop-groomed jet radius, $R_{g}$, and momentum balance, $z_{g}$, of b quark jets are presented. These observables can be used to test perturbative quantum chromodynamics predictions that account for mass effects. An algorithm to identify and cluster the charged decay daughters of b hadrons is developed for this analysis, which facilitates the exposure of the gluon radiation pattern of b jets using iterative Cambridge--Aachen declustering. Because the b hadron is partially reconstructed from its charged decay daughters, only charged particles are used for the jet substructure studies. In addition, a jet fragmentation function, $z_{b,ch}$, is measured, which is defined as the distribution of the ratio of the transverse momentum ($p_{T}$) of the partially reconstructed b hadron with respect to the charged-particle component of the jet $p_{T}$. The measured distributions are unfolded to the charged-particle level. The b jet substructure is compared to that of inclusive jets, which are dominated by light-quark and gluon jets, to assess the role of the b quark mass. A strong suppression of emissions at small $R_{g}$ values is observed for b jets when compared to inclusive jets, consistent with the dead-cone effect. The measurements are also compared with theoretical predictions from Monte Carlo event generators. This is the first b jet substructure study that clusters together the b hadron decay daughters.
DOI: 10.57761/z41d-n606
title: CMS_Surg_2020-2025
DOI: 10.5061/dryad.jdfn2z38s
title: Habitat fragmentation and logging affects the occurrence of the lesser mouse deer in tropical forest reserves

description: Due to rapid urbanization, logging, and agricultural expansion, forest
 fragmentation is negatively affecting native wildlife populations
 throughout the tropics. This study examined the effects of landscape and
 habitat characteristics on the lesser mouse deer, Tragulus kanchil,
 populations in Peninsular Malaysia. A total of 315 camera traps were
 deployed in eight forest reserves. This study provides critical ecological
 information for managing and conserving understudied populations of T.
 kanchil. We found that the detection of T. kanchil was attributed to
 forest fragmentation. Forest patches had the detection of T. kanchil four
 times greater than continuous forests. The detection of T. kanchil was
 nearly three times higher in the peat swamp forest compared to the lowland
 dipterocarp forests. Surprisingly, the detection of T. kanchil was almost
 twice lower in the unlogged forests compared to logged forests. The
 detection of T. kanchil increased with the presence of trees, particularly
 those with DBH of 5 cm to 45 cm, canopy cover, number of saplings and
 palms, number of dead fallen trees, and distance from nearest roads.
 However, detection decreased with a greater number of trees with a DBH
 greater than 45 cm and higher elevation. We recommend that conservation
 stakeholders take the necessary steps to support the conservation of mouse
 deer species and its natural habitats regardless of whether these forests
 are fragmented or continuous. These steps include eradicating poaching,
 habitat degradation, and further deforestation.
description: Camera trapping was conducted between March 2013 and April 2018.
 Thirty cameras (Bushnell Trophy Cam and Bushnell Trophy Cam HD) were used
 in the survey. The cameras operated 24 hours per day and were left for two
 weeks to maximize the number of detections and obtain sufficient data for
 analysis (Nichols & Karanth, 2002). The infrared feature of the
 Bushnell Trophy Cam consists of a sensor triggered by motion and heat. The
 camera was set to capture three images per second, with a 1- or 10-second
 interval between. The cameras were fixed on trees at the height of 30 cm
 to 50 cm above the ground at angles facing the animal trails. The images
 captured were sorted down to species level, with species other than
 <i>T. kanchil</i> excluded from the analysis (Figure 2).
  Overexposure and unclear images that led to unidentified species were
 also excluded (Sasidhran <i>et al</i>., 2016). Mousedeer
 detection in the camera traps was represented by the number of
 photographic images recorded at each of the 315 sites.
DOI: 10.5061/dryad.mcvdncjzq
title: Data and code from: Light might suppress both types of sound-evoked anti-predator flight in moths

description: Urbanization exposes wild animals to increased levels of light, affecting
 particularly nocturnal animals. Artificial light at night might shift the
 balance of predator-prey interactions, for example of nocturnal
 echolocating bats and eared moths. Moths exposed to light show less
 last-ditch manoeuvres in response to attacking close-by bats. In contrast,
 the extent to which negative phonotaxis, moths’ first line of defence
 against distant bats, is affected by light is unclear. Here, we aimed to
 quantify the overall effect of light on both types of sound-evoked
 anti-predator flight, last-ditch manoeuvres and negative phonotaxis. We
 caught moths at two light traps, which were alternately equipped with
 loudspeakers that presented ultrasonic playbacks to simulate hunting bats.
 The light field was omnidirectional to attract moths equally from all
 directions. In contrast, the sound field was directional and thus,
 depending on the moth’s approach direction, elicited either only negative
 phonotaxis, or negative phonotaxis and last-ditch manoeuvres. We did not
 observe an effect of sound playback on the number of caught moths,
 suggesting that light might suppress both types of anti-predator flight,
 as either type would have caused a decline in the number of caught moths.
 As control, we confirmed that our playback was able to elicit evasive
 flight in moths in a dark flight room. Showing no effect of a treatment,
 however, is difficult. We discuss potential alternative explanations for
 our results, and call for further studies to investigate how light
 interferes with animal behaviour.
DOI: 10.17182/hepdata.33614.v1/t1
title: "Table 1" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t2
title: "Table 2" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t3
title: "Table 3" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t4
title: "Table 4" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t5
title: "Table 5" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t8
title: "Table 8" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t10
title: "Table 10" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t11
title: "Table 11" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t12
title: "Table 12" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t13
title: "Table 13" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t14
title: "Table 14" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t6
title: "Table 6" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t7
title: "Table 7" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t9
title: "Table 9" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.5061/dryad.5hqbzkh46
title: A meta‐analysis of insularity effects on herbivory and plant defences

description: Aim: Plants on islands are often subjected to lower levels of herbivory
 relative to those at mainland sites. As a consequence, island plants are
 predicted to exhibit lower levels of physical and chemical defences, which
 renders them more susceptible to introduced herbivores. Yet, instances of
 high pressure by superabundant herbivores native to islands have been
 reported in many insular systems, which presumably would result in
 heightened plant defences. To date, no quantitative review has been
 conducted to determine how common these contrasting patterns are and their
 implications for the evolution of plant defences. Location: Islands
 worldwide Taxon: Plants, insects, mammals Methods: We conducted a
 meta-analysis of insularity effects on herbivory and plant defences by
 including studies that conducted island-mainland comparisons of the same
 plant species in both environments (90% of cases), or insular endemics vs.
 mainland congeners (10% of cases). We tested for differences between
 mammalian and invertebrate herbivory as well as between plant chemical and
 physical defences by specifying comparisons based on the type of herbivore
 included in the study. Results: Mammalian herbivory was significantly
 higher on islands than on mainlands. In contrast, no significant effect
 was observed on invertebrate herbivory. In addition, we found no
 significant difference in either plant physical or chemical defences
 between insular and mainland plants, though physical defences tended to be
 higher for plants on islands. Main conclusions: All analysed mammal
 studies focused on species introduced to islands, suggesting greater
 susceptibility of insular plants to exotic mammals, whereas the lack of
 effects in the case of invertebrate herbivory suggests no difference in
 susceptibility to molluscs and insects between insular and mainland
 plants. Interestingly, plant trait patterns suggest a trend for increased
 physical defences by insular plants, possibly due to heightened pressure
 by exotic mammalian herbivores on islands, whereas chemical defences
 appear uncorrelated to differences in herbivory. These findings call for
 further experimental and observational studies measuring defences and
 herbivory for multiple sympatric plant species occurring at both mainland
 and island sites within a system, or comparing insular endemics to
 congeneric mainland species.
DOI: 10.17182/hepdata.33614.v1/t15
title: "Table 15" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t16
title: "Table 16" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t17
title: "Table 17" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.
DOI: 10.17182/hepdata.33614.v1/t18
title: "Table 18" of "A detailed study of the nucleon structure functions in deep elastic muon scattering in iron"

description: No description provided.
description: PLAB=120 TO 280 GEV/C. FINAL EMC DATA ON STRUCTURE FUNCTIONS OF NUCLEON USING IRON TARGET. RANGES ARE:- 0.04 & lt; X & lt; 0.7 AND 3.5 & lt; Q**2 & lt; 220. NO CORRECTION FOR FERMI MOTION HAS BEEN INCLUDED. A VALUE OF R=0 WAS ASSUMED. THEIR MEASURED (GLOBAL) VALUE OF R IS 0.026 +- 0.037 +- 0.174.