Search for Second-Generation Leptoquark Pairs in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>p</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover></mml:mrow></mml:mrow><mml:mi mathvariant="italic">p</mml:mi></mml:math>Collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>√</mml:mi><mml:mi mathvariant="italic">s</mml:mi><mml:mspace/><mml:mo>=</mml:mo><mml:mspace/><mml:mn>1.8</mml:mn><mml:mn/><mml:mi/><mml:mi>TeV</mml:mi></mml:math>
Annotatsiya
We have searched for second-generation leptoquark (LQ) pairs in the $\ensuremath{\mu}\ensuremath{\mu}+\mathrm{jets}$ channel using $94\ifmmode\pm\else\textpm\fi{}5{\mathrm{pb}}^{\ensuremath{-}1}$ of $\overline{p}p$ collider data collected by the D0 experiment at the Fermilab Tevatron during 1993--1996. No evidence for a signal is observed. These results are combined with those from the $\ensuremath{\mu}\ensuremath{\nu}+\mathrm{jets}$ and $\ensuremath{\nu}\ensuremath{\nu}+\mathrm{jets}$ channels to obtain $95%$ confidence level (C.L.) upper limits on the LQ pair production cross section as a function of mass and $\ensuremath{\beta}$, the branching fraction of a LQ decay into a charged lepton and a quark. Lower limits of $200(180)\mathrm{GeV}{/c}^{2}$ for $\ensuremath{\beta}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}1(\frac{1}{2})$ are set at the $95%$ C.L. on the mass of scalar LQ. Mass limits are also set on vector leptoquarks as a function of $\ensuremath{\beta}$.