[{"quality_controlled":"1","language":[{"iso":"eng"}],"author":[{"full_name":"Thorleifsson, G","first_name":"G","autoren_ansetzung":["Thorleifsson, G","Thorleifsson","G Thorleifsson","Thorleifsson, G","Thorleifsson, G.","G Thorleifsson","G. Thorleifsson"],"last_name":"Thorleifsson"},{"full_name":"Petersson, Bengt","id":"40337","autoren_ansetzung":["Petersson, Bengt","Petersson","Bengt Petersson","Petersson, B","Petersson, B.","B Petersson","B. Petersson"],"last_name":"Petersson","first_name":"Bengt"}],"inspire":"1","first_author":"Thorleifsson, G","arxivID":"hep-lat/9709072","department":[{"_id":"23470456"}],"publication_identifier":{"issn":["0920-5632"]},"volume":"63","title":"Beyond the c=1 barrier in two-dimensional quantum gravity","citation":{"wels":"Thorleifsson, G.; Petersson, B. (1998): Beyond the c=1 barrier in two-dimensional quantum gravity *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*,63: 745-747.","harvard1":"Thorleifsson, G., & Petersson, B., 1998. Beyond the c=1 barrier in two-dimensional quantum gravity. *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*, 63, p 745-747.","aps":" G. Thorleifsson and B. Petersson, Beyond the c=1 barrier in two-dimensional quantum gravity, NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS **63**, 745 (1998).","angewandte-chemie":"G. Thorleifsson, and B. Petersson, “Beyond the c=1 barrier in two-dimensional quantum gravity”, *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*, **1998**, *63*, 745-747.","apa":"Thorleifsson, G., & Petersson, B. (1998). Beyond the c=1 barrier in two-dimensional quantum gravity. *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*, *63*, 745-747. doi:10.1016/S0920-5632(97)00891-8","lncs":" Thorleifsson, G., Petersson, B.: Beyond the c=1 barrier in two-dimensional quantum gravity. NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS. 63, 745-747 (1998).","frontiers":"Thorleifsson, G., and Petersson, B. (1998). Beyond the c=1 barrier in two-dimensional quantum gravity. *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS* 63, 745-747.","chicago":"Thorleifsson, G, and Petersson, Bengt. 1998. “Beyond the c=1 barrier in two-dimensional quantum gravity”, NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS, 63: 745-747.

","ieee":" G. Thorleifsson and B. Petersson, “Beyond the c=1 barrier in two-dimensional quantum gravity”, *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*, vol. 63, 1998, pp. 745-747.","apa_indent":"Thorleifsson, G., & Petersson, B. (1998). Beyond the c=1 barrier in two-dimensional quantum gravity. *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*, *63*, 745-747. doi:10.1016/S0920-5632(97)00891-8

","ama":"Thorleifsson G, Petersson B. Beyond the c=1 barrier in two-dimensional quantum gravity. *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS*. 1998;63:745-747.","bio1":"Thorleifsson G, Petersson B (1998)

Beyond the c=1 barrier in two-dimensional quantum gravity.

NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS 63: 745-747.","dgps":"Thorleifsson, G. & Petersson, B. (1998). Beyond the c=1 barrier in two-dimensional quantum gravity (NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS), *63*, 745-747. ELSEVIER SCIENCE BV. doi:10.1016/S0920-5632(97)00891-8.

","mla":"Thorleifsson, G, and Petersson, Bengt. “Beyond the c=1 barrier in two-dimensional quantum gravity”. *NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS* 63 (1998): 745-747.","default":"Thorleifsson G, Petersson B (1998)

*NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS* 63: 745-747."},"isi":"1","type":"conference","series_title":"NUCLEAR PHYSICS B-PROCEEDINGS SUPPLEMENTS","page":"745-747","id":"1626062","external_id":{"arxiv":["hep-lat/9709072"],"inspire":["448665"],"isi":["000072980200202"]},"date_updated":"2018-07-24T12:58:55Z","_id":"1626062","status":"public","year":"1998","publisher":"ELSEVIER SCIENCE BV","doi":"10.1016/S0920-5632(97)00891-8","date_created":"2010-04-28T13:20:54Z","arxiv":"1","date_submitted":"2011-08-30T07:14:28Z","accept":"1","intvolume":" 63","publication_status":"published","abstract":[{"lang":"eng","text":"We introduce a simple model of touchingrandom surfaces, by adding a chemical potential rho for \"minimal necks\", and study this model numerically coupled to a Gaussian model in d-dimensions (for central charge c = d = 0, 1 and 2). For c less than or equal to 1, this model has a phase transition to branched polymers, for sufficiently large p. For c 2, however, extensive simulations indicate that this transition is replaced by a cross-over behavior on finite lattices - the model is always in the branched polymer phase. This supports recent speculations that, in 2d-gravity, the behavior observe in simulations for c less than or equal to 1, is dominated by finite size effects, which are exponentially enhanced as c --> 1(+)."}]}]