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    {
      "raw_name": "Mironov, A.", 
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          "country": "Russia", 
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        {
          "country": "Russia", 
          "value": "ITEP, Moscow, 117218, Russia"
        }, 
        {
          "country": "Russia", 
          "value": "Lebedev Physics Institute, Moscow, 119991, Russia"
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        {
          "country": "Russia", 
          "value": "National Research Nuclear University MEPhI, Moscow, 115409, Russia"
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      "surname": "Mironov", 
      "given_names": "A.", 
      "full_name": "Mironov, A."
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    {
      "raw_name": "Morozov, A.", 
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          "country": "Russia", 
          "value": "Institute for Information Transmission Problems, Moscow, 127994, Russia"
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        {
          "country": "Russia", 
          "value": "ITEP, Moscow, 117218, Russia"
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        {
          "country": "Russia", 
          "value": "National Research Nuclear University MEPhI, Moscow, 115409, Russia"
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      "surname": "Morozov", 
      "given_names": "A.", 
      "full_name": "Morozov, A."
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    {
      "raw_name": "Zenkevich, Y.", 
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          "country": "Russia", 
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        {
          "country": "Russia", 
          "value": "Institute of Nuclear Research, Moscow, 117312, Russia"
        }, 
        {
          "country": "Russia", 
          "value": "National Research Nuclear University MEPhI, Moscow, 115409, Russia"
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      "surname": "Zenkevich", 
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  "titles": [
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      "source": "Elsevier", 
      "title": "On elementary proof of AGT relations from six dimensions"
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      "source": "Elsevier", 
      "value": "The actual definition of the Nekrasov functions participating in the AGT relations implies a peculiar choice of contours in the LMNS and Dotsenko\u2013Fateev integrals. Once made explicit and applied to the original triply-deformed (6-dimensional) version of these integrals, this approach reduces the AGT relations to symmetry in q1,2,3 , which is just an elementary identity for an appropriate choice of the integration contour (which is, however, a little non-traditional). We illustrate this idea with the simplest example of N=(1,1) U(1) SYM in six dimensions, however all other cases can be evidently considered in a completely similar way."
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