Matches in SemOpenAlex for { <https://semopenalex.org/work/W2322203022> ?p ?o ?g. }
- W2322203022 abstract "We investigate the effects of the range of adsorption potential on the equilibrium behavior of a single polymer chain end-attached to a solid surface. The exact analytical theory for ideal lattice chains interacting with a planar surface via a box potential of depth U and width W is presented and compared to continuum model results and to Monte Carlo (MC) simulations using the pruned-enriched Rosenbluth method for self-avoiding chains on a simple cubic lattice. We show that the critical value U(c) corresponding to the adsorption transition scales as W(-1/ν), where the exponent ν=1/2 for ideal chains and ν≈3/5 for self-avoiding walks. Lattice corrections for finite W are incorporated in the analytical prediction of the ideal chain theory U(c)≈(π(2)/24)(W+1/2)(-2) and in the best-fit equation for the MC simulation data U(c)=0.585(W+1/2)(-5/3). Tail, loop, and train distributions at the critical point are evaluated by MC simulations for 1≤W≤10 and compared to analytical results for ideal chains and with scaling theory predictions. The behavior of a self-avoiding chain is remarkably close to that of an ideal chain in several aspects. We demonstrate that the bound fraction θ and the related properties of finite ideal and self-avoiding chains can be presented in a universal reduced form: θ(N,U,W)=θ(NU(c),U/U(c)). By utilizing precise estimations of the critical points we investigate the chain length dependence of the ratio of the normal and lateral components of the gyration radius. Contrary to common expectations this ratio attains a limiting universal value <R(g[perpendicular])(2)>/<R(g[parallel])(2)>=0.320±0.003 only at N~5000. Finite-N corrections for this ratio turn out to be of the opposite sign for W=1 and for W≥2. We also study the N dependence of the apparent crossover exponent φ(eff)(N). Strong corrections to scaling of order N(-0.5) are observed, and the extrapolated value φ=0.483±0.003 is found for all values of W. The strong correction to scaling effects found here explain why for smaller values of N, as used in most previous work, misleadingly large values of φ(eff)(N) were identified as the asymptotic value for the crossover exponent." @default.
- W2322203022 created "2016-06-24" @default.
- W2322203022 creator A5005523800 @default.
- W2322203022 creator A5037753080 @default.
- W2322203022 creator A5058336407 @default.
- W2322203022 creator A5070039682 @default.
- W2322203022 creator A5082708317 @default.
- W2322203022 creator A5084369665 @default.
- W2322203022 date "2013-02-27" @default.
- W2322203022 modified "2023-10-03" @default.
- W2322203022 title "Adsorption of a single polymer chain on a surface: Effects of the potential range" @default.
- W2322203022 cites W1618218131 @default.
- W2322203022 cites W186403072 @default.
- W2322203022 cites W1964610776 @default.
- W2322203022 cites W1966817580 @default.
- W2322203022 cites W1968171976 @default.
- W2322203022 cites W1972738467 @default.
- W2322203022 cites W1986251967 @default.
- W2322203022 cites W1986829471 @default.
- W2322203022 cites W1991021168 @default.
- W2322203022 cites W2000364242 @default.
- W2322203022 cites W2004315869 @default.
- W2322203022 cites W2018805334 @default.
- W2322203022 cites W2020313974 @default.
- W2322203022 cites W2022180470 @default.
- W2322203022 cites W2027190394 @default.
- W2322203022 cites W2027780290 @default.
- W2322203022 cites W2047805511 @default.
- W2322203022 cites W2048072960 @default.
- W2322203022 cites W2054098342 @default.
- W2322203022 cites W2057950366 @default.
- W2322203022 cites W2076027400 @default.
- W2322203022 cites W2078337173 @default.
- W2322203022 cites W2085446411 @default.
- W2322203022 cites W2085548090 @default.
- W2322203022 cites W2087237419 @default.
- W2322203022 cites W2096174895 @default.
- W2322203022 cites W2097246107 @default.
- W2322203022 cites W2099509099 @default.
- W2322203022 cites W2112095542 @default.
- W2322203022 cites W2144463028 @default.
- W2322203022 cites W2158137669 @default.
- W2322203022 cites W2315113407 @default.
- W2322203022 cites W2325253331 @default.
- W2322203022 cites W2335758222 @default.
- W2322203022 cites W3098142529 @default.
- W2322203022 cites W3100722600 @default.
- W2322203022 cites W3102069366 @default.
- W2322203022 cites W3123902762 @default.
- W2322203022 cites W3149520802 @default.
- W2322203022 cites W4234847219 @default.
- W2322203022 cites W2050820300 @default.
- W2322203022 doi "https://doi.org/10.1103/physreve.87.022604" @default.
- W2322203022 hasPubMedId "https://pubmed.ncbi.nlm.nih.gov/23496541" @default.
- W2322203022 hasPublicationYear "2013" @default.
- W2322203022 type Work @default.
- W2322203022 sameAs 2322203022 @default.
- W2322203022 citedByCount "56" @default.
- W2322203022 countsByYear W23222030222013 @default.
- W2322203022 countsByYear W23222030222014 @default.
- W2322203022 countsByYear W23222030222015 @default.
- W2322203022 countsByYear W23222030222016 @default.
- W2322203022 countsByYear W23222030222017 @default.
- W2322203022 countsByYear W23222030222018 @default.
- W2322203022 countsByYear W23222030222019 @default.
- W2322203022 countsByYear W23222030222020 @default.
- W2322203022 countsByYear W23222030222021 @default.
- W2322203022 countsByYear W23222030222022 @default.
- W2322203022 countsByYear W23222030222023 @default.
- W2322203022 crossrefType "journal-article" @default.
- W2322203022 hasAuthorship W2322203022A5005523800 @default.
- W2322203022 hasAuthorship W2322203022A5037753080 @default.
- W2322203022 hasAuthorship W2322203022A5058336407 @default.
- W2322203022 hasAuthorship W2322203022A5070039682 @default.
- W2322203022 hasAuthorship W2322203022A5082708317 @default.
- W2322203022 hasAuthorship W2322203022A5084369665 @default.
- W2322203022 hasConcept C105795698 @default.
- W2322203022 hasConcept C111472728 @default.
- W2322203022 hasConcept C121332964 @default.
- W2322203022 hasConcept C121684516 @default.
- W2322203022 hasConcept C121864883 @default.
- W2322203022 hasConcept C134306372 @default.
- W2322203022 hasConcept C134786449 @default.
- W2322203022 hasConcept C138885662 @default.
- W2322203022 hasConcept C149288129 @default.
- W2322203022 hasConcept C164154869 @default.
- W2322203022 hasConcept C192562407 @default.
- W2322203022 hasConcept C19499675 @default.
- W2322203022 hasConcept C196298200 @default.
- W2322203022 hasConcept C199185054 @default.
- W2322203022 hasConcept C24890656 @default.
- W2322203022 hasConcept C2524010 @default.
- W2322203022 hasConcept C26873012 @default.
- W2322203022 hasConcept C2776639384 @default.
- W2322203022 hasConcept C2780388253 @default.
- W2322203022 hasConcept C2781204021 @default.
- W2322203022 hasConcept C2991992277 @default.
- W2322203022 hasConcept C33923547 @default.
- W2322203022 hasConcept C41008148 @default.
- W2322203022 hasConcept C41895202 @default.