{ "items" : [
    { "id" : "http://dbpedia.org/resource/Mermin–Wagner_theorem"
      "properties" : {
        "http://www.w3.org/2000/01/rdf-schema#comment" : [ "In quantum field theory and statistical mechanics, the Mermin–Wagner theorem (also known as Mermin–Wagner–Hohenberg theorem or Coleman theorem) states that continuous symmetries cannot be spontaneously broken at finite temperature in systems with sufficiently short-range interactions in dimensions d ≤ 2."] } } }
