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1.
Phys Rev Lett ; 84(2): 294-7, 2000 Jan 10.
Article in English | MEDLINE | ID: mdl-11015894

ABSTRACT

A linear copolymer made of two reciprocally attracting N-monomer blocks collapses to a compact phase through a novel transition, whose exponents are determined with extensive Monte Carlo simulations in two and three dimensions. In the former case, an identification with the statistical geometry of suitable percolation paths allows one to predict that the number of contacts between the blocks grows like N9/16. In the compact phase the blocks are mixed and, in two dimensions, also zipped, in such a way to form a spiral, double chain structure.

3.
Phys Rev Lett ; 62(10): 1067-1070, 1989 Mar 06.
Article in English | MEDLINE | ID: mdl-10039568
4.
Phys Rev Lett ; 63(22): 2537, 1989 Nov 27.
Article in English | MEDLINE | ID: mdl-10040917
5.
Phys Rev Lett ; 59(3): 300-303, 1987 Jul 20.
Article in English | MEDLINE | ID: mdl-10035725
6.
7.
Phys Rev Lett ; 67(20): 2757-2760, 1991 Nov 11.
Article in English | MEDLINE | ID: mdl-10044547
8.
Phys Rev Lett ; 76(26): 4983-4986, 1996 Jun 24.
Article in English | MEDLINE | ID: mdl-10061429
9.
Phys Rev Lett ; 71(7): 1027-1030, 1993 Aug 16.
Article in English | MEDLINE | ID: mdl-10055430
10.
Phys Rev Lett ; 61(13): 1520, 1988 Sep 26.
Article in English | MEDLINE | ID: mdl-10038822
11.
Phys Rev Lett ; 68(4): 488-491, 1992 Jan 27.
Article in English | MEDLINE | ID: mdl-10045909
12.
Phys Rev Lett ; 71(23): 3818-3821, 1993 Dec 06.
Article in English | MEDLINE | ID: mdl-10055081
13.
Phys Rev Lett ; 69(25): 3650-3653, 1992 Dec 21.
Article in English | MEDLINE | ID: mdl-10046878
20.
Article in English | MEDLINE | ID: mdl-11046266

ABSTRACT

In a semi-infinite geometry, a one-dimensional, M-component model of biological evolution realizes microscopically an inhomogeneous branching process for M-->infinity. This implies a size distribution exponent tau(')=7/4 for avalanches starting at a free, "dissipative" end of the evolutionary chain. A bulklike behavior with tau(')=3/2 is restored by "conservative" boundary conditions. These are such as to strictly fix to its critical, bulk value the average number of species directly involved in an evolutionary avalanche by the mutating species located at the chain end. A two-site correlation function exponent tau(')(R)=4 is also calculated exactly in the "dissipative" case, when one of the points is at the border. Together with accurate numerical determinations of the time recurrence exponent tau(')(first), these results show also that, no matter whether dissipation is present or not, boundary avalanches have the same space and time fractal dimensions as those in the bulk, and their distribution exponents obey the basic scaling laws holding there.

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