A study of the decay
pan id="mmlsi1" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316301022&_mathId=si1.gif&_user=111111111&_pii=S0370269316301022&_rdoc=1&_issn=03702693&md5=a27d90cd9ed1c8a9305ee68cb10567d6" title="Click to view the MathML source">Dp>0p>→Kp>−p>πp>+p>μp>+p>μp>−p>pan>pan class="mathContainer hidden">pan class="mathCode"><math altimg="si1.gif" overflow="scroll"><msup><mrow><mi>Dmi>mrow><mrow><mn>0mn>mrow>msup><mo stretchy="false">→mo><msup><mrow><mi>Kmi>mrow><mrow><mo>−mo>mrow>msup><msup><mrow><mi>πmi>mrow><mrow><mo>+mo>mrow>msup><msup><mrow><mi>μmi>mrow><mrow><mo>+mo>mrow>msup><msup><mrow><mi>μmi>mrow><mrow><mo>−mo>mrow>msup>math>pan>pan>pan> is
perfor
med using data collected by the LHCb detector in
proton–
proton collisions at a centre-of-
mass energy of 8 TeV, corres
ponding to an integrated lu
minosity of
pan id="mmlsi2" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316301022&_mathId=si2.gif&_user=111111111&_pii=S0370269316301022&_rdoc=1&_issn=03702693&md5=aa553350039047030cfe0c9c588b103c" title="Click to view the MathML source">2.0 fbp>−1p>pan>pan class="mathContainer hidden">pan class="mathCode"><math altimg="si2.gif" overflow="scroll"><mn>2.0mn><msup><mrow><mtext> fbmtext>mrow><mrow><mo>−mo><mn>1mn>mrow>msup>math>pan>pan>pan>. Decay candidates with
muon
pairs that have an invariant
mass in the range
pan id="mmlsi102" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316301022&_mathId=si102.gif&_user=111111111&_pii=S0370269316301022&_rdoc=1&_issn=03702693&md5=9ca79b3c364a17f07386b953b9201081" title="Click to view the MathML source">675–875 MeV/cp>2p>pan>pan class="mathContainer hidden">pan class="mathCode"><math altimg="si102.gif" overflow="scroll"><mn>675mn><mtext>–mtext><mn>875mn><mtext> MeVmtext><mo stretchy="false">/mo><msup><mrow><mi>cmi>mrow><mrow><mn>2mn>mrow>msup>math>pan>pan>pan> are considered. This region is do
minated by the
pan id="mmlsi11" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316301022&_mathId=si11.gif&_user=111111111&_pii=S0370269316301022&_rdoc=1&_issn=03702693&md5=ed6c8ea4c95c2a6afc807fff99e1cc17" title="Click to view the MathML source">ρp>0p>pan>pan class="mathContainer hidden">pan class="mathCode"><math altimg="si11.gif" overflow="scroll"><msup><mrow><mi>ρmi>mrow><mrow><mn>0mn>mrow>msup>math>pan>pan>pan> and
m>ωm> resonances. The branching fraction in this range is
measured to be
This is the first observation of the decay
pan id="mmlsi1" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0370269316301022&_mathId=si1.gif&_user=111111111&_pii=S0370269316301022&_rdoc=1&_issn=03702693&md5=a27d90cd9ed1c8a9305ee68cb10567d6" title="Click to view the MathML source">Dp>0p>→Kp>−p>πp>+p>μp>+p>μp>−p>pan>pan class="mathContainer hidden">pan class="mathCode"><math altimg="si1.gif" overflow="scroll"><msup><mrow><mi>Dmi>mrow><mrow><mn>0mn>mrow>msup><mo stretchy="false">→mo><msup><mrow><mi>Kmi>mrow><mrow><mo>−mo>mrow>msup><msup><mrow><mi>πmi>mrow><mrow><mo>+mo>mrow>msup><msup><mrow><mi>μmi>mrow><mrow><mo>+mo>mrow>msup><msup><mrow><mi>μmi>mrow><mrow><mo>−mo>mrow>msup>math>pan>pan>pan>. Its branching fraction is consistent with the value ex
pected in the Standard Model.