Search for the lepton-flavour violating decay D0 → e±μ
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A search for the lepton-flavour violating decay lsi1" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si1.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=fc1877ec9ab7d383146f53623195cc45" title="Click to view the MathML source">D0→e±μlass="mathContainer hidden">lass="mathCode">ltimg="si1.gif" overflow="scroll">w>Dw>w>0w>lse">→w>ew>w>±w>w>μw>w>w> is made with a dataset corresponding to an integrated luminosity of lsi2" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si2.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=aeceaccfdc386158ce9873498f288901">lass="imgLazyJSB inlineImage" height="14" width="51" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316000411-si2.gif">lass="mathContainer hidden">lass="mathCode">ltimg="si2.gif" overflow="scroll">3.0width="0.25em">w>fbw>w>1w> of proton–proton collisions at centre-of-mass energies of lsi24" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si24.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=0aeed9fced1f917d344752e5675b6909">lass="imgLazyJSB inlineImage" height="10" width="36" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316000411-si24.gif">lass="mathContainer hidden">lass="mathCode">ltimg="si24.gif" overflow="scroll">7width="0.25em">TeV and lsi26" class="mathmlsrc">le="View the MathML source" class="mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si26.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=e9c1ace21c4d45fb036fe0c92757049a">lass="imgLazyJSB inlineImage" height="10" width="35" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0370269316000411-si26.gif">lass="mathContainer hidden">lass="mathCode">ltimg="si26.gif" overflow="scroll">8width="0.25em">TeV, collected by the LHCb experiment. Candidate lsi5" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si5.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=f0e2cdc444fe36fa3f696d6a2040a4a6" title="Click to view the MathML source">D0lass="mathContainer hidden">lass="mathCode">ltimg="si5.gif" overflow="scroll">w>Dw>w>0w> mesons are selected using the decay lsi27" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si27.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=35be6e726715a8b901212af5c88ce833" title="Click to view the MathML source">D⁎+→D0π+lass="mathContainer hidden">lass="mathCode">ltimg="si27.gif" overflow="scroll">w>Dw>w>+w>lse">→w>Dw>w>0w>w>πw>w>+w> and the lsi1" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si1.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=fc1877ec9ab7d383146f53623195cc45" title="Click to view the MathML source">D0→e±μlass="mathContainer hidden">lass="mathCode">ltimg="si1.gif" overflow="scroll">w>Dw>w>0w>lse">→w>ew>w>±w>w>μw>w>w> branching fraction is measured using the decay mode lsi28" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si28.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=50acf2c2ba49be9507581c6d97f5c66b" title="Click to view the MathML source">D0→Kπ+lass="mathContainer hidden">lass="mathCode">ltimg="si28.gif" overflow="scroll">w>Dw>w>0w>lse">→w>Kw>w>w>w>πw>w>+w> as a normalization channel. No significant excess of lsi1" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si1.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=fc1877ec9ab7d383146f53623195cc45" title="Click to view the MathML source">D0→e±μlass="mathContainer hidden">lass="mathCode">ltimg="si1.gif" overflow="scroll">w>Dw>w>0w>lse">→w>ew>w>±w>w>μw>w>w> candidates over the expected background is seen, and a limit is set on the branching fraction, lsi8" class="mathmlsrc">lass="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316000411&_mathId=si8.gif&_user=111111111&_pii=S0370269316000411&_rdoc=1&_issn=03702693&md5=8fe2e966e026ab3053ca20b522e85073" title="Click to view the MathML source">B(D0→e±μ)<1.3×10−8lass="mathContainer hidden">lass="mathCode">ltimg="si8.gif" overflow="scroll">Blse">(w>Dw>w>0w>lse">→w>ew>w>±w>w>μw>w>w>lse">)<1.3×w>10w>w>8w>, at 90% confidence level. This is an order of magnitude lower than the previous limit and it further constrains the parameter space in some leptoquark models and in supersymmetric models with R-parity violation.

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