You Can\u27t Take it With You Dramaturgical Website

The presenters are enrolled in TheatreUNI’s Dramaturgy course where they study drama through a theoretical lens to create analytical criticism and research contextual support for TheatreUNI’s current productions. They have compiled research into a dramaturgical website focused on topics relating to the text of Kaufman and Hart’s Pulitzer Prize winning play You Can’t Take it With You. We will be presenting our final website designed for TheatreUNI patrons, and discussing each of the topics that we individually researched. Our research covers the following topics through the lens of the 1930’s: Great Depression, entertainment industry, music, fashion, immigration, the Russian Revolution, Rasputin, and the Romonovs, the public’s views of the IRS, the FBI, use of fireworks, comedic styles, and racism present in the original text and how TheatreUNI is overcoming it

Search for supersymmetry with a compressed mass spectrum in events with a soft τ\tau lepton, a highly energetic jet, and large missing transverse momentum in proton-proton collisions at s=\sqrt{s}= 13 TeV

The first search for supersymmetry in events with an experimental signature of one soft, hadronically decaying $\tau$ lepton, one energetic jet from initial-state radiation, and large transverse momentum imbalance is presented. These event signatures are consistent with direct or indirect production of scalar $\tau$ leptons ($\tilde{\tau}$) in supersymmetric models that exhibit coannihilation between the $\tilde{\tau}$ and the lightest neutralino ($\tilde{\chi}^0_1$), and that could generate the observed relic density of dark matter. The data correspond to an integrated luminosity of 77.2 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=$ 13 TeV collected with the CMS detector at the LHC in 2016 and 2017. The results are interpreted in a supersymmetric scenario with a small mass difference ($\Delta m$) between the chargino ($\tilde{\chi}^\pm_1$) or next-to-lightest neutralino ($\tilde{\chi}^0_2$), and the $\tilde{\chi}^0_1$. The mass of the $\tilde{\tau}$ is assumed to be the average of the $\tilde{\chi}^\pm_1$ and $\tilde{\chi}^0_1$ masses. The data are consistent with standard model background predictions. Upper limits at 95% confidence level are set on the sum of the $\tilde{\chi}^\pm_1$, $\tilde{\chi}^0_2$, and $\tilde{\tau}$ production cross sections for $\Delta m(\tilde{\chi}^\pm_1, \tilde{\chi}^0_1) =$ 50 GeV, resulting in a lower limit of 290 GeV on the mass of the $\tilde{\chi}^\pm_1$, which is the most stringent to date and surpasses the bounds from the LEP experiments

Työministeriön tilastoja 1991, Maaliskuu

Suomen virallinen tilasto (SVT