2004
DOI: 10.1016/j.physleta.2004.06.063
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Scaling of star polymers: high order results

Abstract: We extend existing renormalization group calculations for the exponents describing scaling of star polymers and polymer networks constituted by chains of different species (the so-called copolymer star exponents). Our four loop results find application in the description of various phenomena involving self-avoiding and random walks that interact.

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Cited by 10 publications
(11 citation statements)
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“…Here, ν RW = 1/2 and ν SAW are the mean square end-to-end distance exponents for the random and self-avoiding walks, correspondingly, and d is space dimension. The exponents η f 1 f 2 have been calculated within field-theoretical renormalization group approach [9,[32][33][34] and are currently know in the fourth order of the ε = 4 − d expansion [35]. Below, we list them together with the ε-expansion for the exponent ν SAW [36] in the corresponding order: Substituting expressions (1.6)-(1.11) into the scaling relations (1.5) one can evaluate loop exponents c i at any value of d. It is well known, however, that ε-expansions of the field theory are asymptotic at best and proper resummation technique is required to get a reliable numerical information on their basis [37,38].…”
Section: -3mentioning
confidence: 99%
“…Here, ν RW = 1/2 and ν SAW are the mean square end-to-end distance exponents for the random and self-avoiding walks, correspondingly, and d is space dimension. The exponents η f 1 f 2 have been calculated within field-theoretical renormalization group approach [9,[32][33][34] and are currently know in the fourth order of the ε = 4 − d expansion [35]. Below, we list them together with the ε-expansion for the exponent ν SAW [36] in the corresponding order: Substituting expressions (1.6)-(1.11) into the scaling relations (1.5) one can evaluate loop exponents c i at any value of d. It is well known, however, that ε-expansions of the field theory are asymptotic at best and proper resummation technique is required to get a reliable numerical information on their basis [37,38].…”
Section: -3mentioning
confidence: 99%
“…Here, ν RW and ν SAW are the mean square end-to-end distance exponents for the random and self-avoiding walks, correspondingly, and d is space dimension. The exponents η f1f2 have been calculated within field-theoretical renormalization group approach [10,21] and are currently know in the fourth order of the ε = 4−d expansion [22]. Below, we list them together with the ε-expansion for the exponent ν SAW [23] in the corresponding order: Where ζ(x) is Riemann zeta-function.…”
Section: Poland-scheraga Model: Scaling Relations and ε-Expansionmentioning
confidence: 99%
“…Therefore the scaling properties of a heterogeneous polymer network made of interacting SAWs and RWs can be reformulated in terms scaling exponents of co-polymer stars made of two interacting sets of SAWs (η S f1f2 ), of RWs (η G f1f2 ) or of a set of SAWs that interacts with RWs (η U f1f2 ) [24]. Field-theoretical renormalization group calculations of the above copolymer star exponents resulted in ε = 4 − d expansions which have been obtained successively within ε 3 [21] and ε 4 [23] accuracy.…”
Section: V1 V1 V3 V3mentioning
confidence: 99%