8 research outputs found

    Reading Too Much into \u3cem\u3eReeder-Simco\u3c/em\u3e?

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    This Note argues that a careful analysis of the Supreme Court\u27s opinion in Volvo Trucks North America, Inc. v. Reeder-Simco GMC, Inc. demonstrates that, despite the expansive dicta appearing in part IV of that opinion, the Court did not intend to reshape the course of its Robinson-Patman Act jurisprudence in any significant way. The Court\u27s opinion operated well within the confines of established Robinson-Patman Act doctrine, even if its searching review of the evidence presented at trial represented a rare foray into the arena of factual error correction. After Reeder-Simco, however, many commentators emphasized the dicta in part IV of the opinion and argued that Reeder-Simco portended the end of a pillar of Robinson-Patman Act doctrine, the Morton Salt Inference. In light of the expansive interpretations that many commentators adopted after Reeder-Simco, this Note surveys citations to the opinion to determine whether such broad readings of the case have taken hold in the lower courts as well. The results show that courts have generally read the opinion narrowly and continue to apply the Morton Salt Inference in secondary-line Robinson-Patman Act cases

    Keeping the Door Ajar for Foreign Plaintiffs in Global Cartel Cases after \u3cem\u3eEmpagran\u3c/em\u3e

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    In many ways, the Supreme Court\u27s opinion of F. Hoffmann-LaRoche Ltd. V. Empagran S.A. raised more questions than it answered. Growing out of the massive international vitamins cartel uncovered in the 1990s, Empagran presented a scenario in which all parties were foreign and all conduct occurred abroad. Although it is well established by now that the Sherman Act applies to foreign conduct that was meant to produce and did in fact produce some substantial effect in the United States, Empagran presented the Court with the first truly foreign antitrust case. It involved not only foreign conduct, but also foreign plaintiffs complaining of injuries suffered abroad at the hands of foreign defendants. The case therefore appeared to present thorny questions about the proper construction of the Foreign Trade Antitrust Improvements Act of 1982 ( FTAIA ) and the extent of the Sherman Act\u27s extraterritorial application

    Keeping the Door Ajar for Foreign Plaintiffs in Global Cartel Cases after \u3cem\u3eEmpagran\u3c/em\u3e

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    In many ways, the Supreme Court\u27s opinion of F. Hoffmann-LaRoche Ltd. V. Empagran S.A. raised more questions than it answered. Growing out of the massive international vitamins cartel uncovered in the 1990s, Empagran presented a scenario in which all parties were foreign and all conduct occurred abroad. Although it is well established by now that the Sherman Act applies to foreign conduct that was meant to produce and did in fact produce some substantial effect in the United States, Empagran presented the Court with the first truly foreign antitrust case. It involved not only foreign conduct, but also foreign plaintiffs complaining of injuries suffered abroad at the hands of foreign defendants. The case therefore appeared to present thorny questions about the proper construction of the Foreign Trade Antitrust Improvements Act of 1982 ( FTAIA ) and the extent of the Sherman Act\u27s extraterritorial application

    ATLAS Run 1 searches for direct pair production of third-generation squarks at the Large Hadron Collider

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    The Grooved Pegboard Test as a Validity Indicator—a Study on Psychogenic Interference as a Confound in Performance Validity Research

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    Measurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H??????? and H???ZZ*???4??? Decay Channels at s\sqrt{s}=8??????TeV with the ATLAS Detector

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    Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3~fb1^{-1} of pppp collisions produced by the Large Hadron Collider at a center-of-mass energy of s=8\sqrt{s} = 8 TeV and recorded by the ATLAS detector. Cross sections are obtained from measured HγγH \rightarrow \gamma \gamma and HZZ4H \rightarrow ZZ ^{*}\rightarrow 4\ell event yields, which are combined accounting for detector efficiencies, fiducial acceptances and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be σppH=33.0±5.3(stat)±1.6(sys)pb\sigma_{pp \to H} = 33.0 \pm 5.3 \, ({\rm stat}) \pm 1.6 \, ({\rm sys}) \mathrm{pb}. The measurements are compared to state-of-the-art predictions.Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3  fb-1 of pp collisions produced by the Large Hadron Collider at a center-of-mass energy of s=8  TeV and recorded by the ATLAS detector. Cross sections are obtained from measured H→γγ and H→ZZ*→4ℓ event yields, which are combined accounting for detector efficiencies, fiducial acceptances, and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be σpp→H=33.0±5.3 (stat)±1.6 (syst)  pb. The measurements are compared to state-of-the-art predictions.Measurements of the total and differential cross sections of Higgs boson production are performed using 20.3 fb1^{-1} of pppp collisions produced by the Large Hadron Collider at a center-of-mass energy of s=8\sqrt{s} = 8 TeV and recorded by the ATLAS detector. Cross sections are obtained from measured HγγH \rightarrow \gamma \gamma and HZZ4H \rightarrow ZZ ^{*}\rightarrow 4\ell event yields, which are combined accounting for detector efficiencies, fiducial acceptances and branching fractions. Differential cross sections are reported as a function of Higgs boson transverse momentum, Higgs boson rapidity, number of jets in the event, and transverse momentum of the leading jet. The total production cross section is determined to be σppH=33.0±5.3(stat)±1.6(sys)pb\sigma_{pp \to H} = 33.0 \pm 5.3 \, ({\rm stat}) \pm 1.6 \, ({\rm sys}) \mathrm{pb}. The measurements are compared to state-of-the-art predictions
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