in the distributional sense for some 62&_mathId=si41.gif&_user=111111111&_pii=S0022039616302662&_rdoc=1&_issn=00220396&md5=894843b84bd2c879dc74cd36d9e1ad48" title="Click to view the MathML source">k≥0, where 62&_mathId=si6.gif&_user=111111111&_pii=S0022039616302662&_rdoc=1&_issn=00220396&md5=ecce76a6e1a415ef2e631248b422a822" title="Click to view the MathML source">δ0 is the Dirac mass at the origin. We prove the existence of singular solutions in the subcritical case: 62&_mathId=si7.gif&_user=111111111&_pii=S0022039616302662&_rdoc=1&_issn=00220396&md5=2e22c12f11b5abbe7e5d5c614633b2c0">62-si7.gif"> and prove that either the solution u has removable singularity at the origin or satisfies 62&_mathId=si8.gif&_user=111111111&_pii=S0022039616302662&_rdoc=1&_issn=00220396&md5=d27636cb478504b030eb89ff4d0e5db8" title="Click to view the MathML source">lim|x|→0+u(x)|x|N−2=CN which is a positive constant. In the supercritical case: 62&_mathId=si9.gif&_user=111111111&_pii=S0022039616302662&_rdoc=1&_issn=00220396&md5=70146721e42f9535f8941e9ba640062a">62-si9.gif"> we prove that 62&_mathId=si10.gif&_user=111111111&_pii=S0022039616302662&_rdoc=1&_issn=00220396&md5=510479bb49b7722168cf1be59081acdc" title="Click to view the MathML source">k=0.