2020
DOI: 10.1021/acs.macromol.9b02370
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Near-Θ Polymers in a Cylindrical Space

Abstract: The advent of single-molecule manipulations has renewed our interest in understanding chain molecules in confined spaces. The conformation and dynamics of these molecules depend on the degree of confinement and self-avoidance. A distinguishing feature of weakly self-avoiding polymers (e.g., DNA) in a cylindrical space is the emergence of the so-called extended de Gennes regime. On the other hand, an earlier study indicates that slit confinement enhances the self-avoidance of a Θ-polymer, for which the two-body… Show more

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Cited by 3 publications
(6 citation statements)
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“…In two dimensions (2D), the correlation length exponent is ν normalΘ 2 normalD = 4 / 7 , which is different from that of the RW. Since the higher-order virial terms cannot be ignored in 2D, the Θ point of a polymer chain in 2D is defined under a more subtle condition than B 2 = 0 in 3D. As a result, the Θ point of a 2D polymer, in practice, has numerically been attained by tuning the relevant parameters (see the Methods section). Historically, studies on geometrical fractal objects in 2D, in particular, the Θ chain in 2D and its exotic exponent ν normalΘ 2 normalD = 4 / 7 0.571 , culminated in the 1980s.…”
Section: Introductionmentioning
confidence: 99%
“…In two dimensions (2D), the correlation length exponent is ν normalΘ 2 normalD = 4 / 7 , which is different from that of the RW. Since the higher-order virial terms cannot be ignored in 2D, the Θ point of a polymer chain in 2D is defined under a more subtle condition than B 2 = 0 in 3D. As a result, the Θ point of a 2D polymer, in practice, has numerically been attained by tuning the relevant parameters (see the Methods section). Historically, studies on geometrical fractal objects in 2D, in particular, the Θ chain in 2D and its exotic exponent ν normalΘ 2 normalD = 4 / 7 0.571 , culminated in the 1980s.…”
Section: Introductionmentioning
confidence: 99%
“…(ii) The configurations of the Θ chain differ from those of SAW (Figure B) in that some monomers are buried inside the domain, whereas others are exposed to the periphery constituting the external perimeter. Θ chains in dilute phase obey , characterized by the fractal dimension of percolating clusters ; ,,,,,, however, Figure D indicates that the external perimeter of the Θ chain is still self-avoiding, such that . …”
Section: Resultsmentioning
confidence: 99%
“…gm m e e g / c X Y X Y (28) For the correlation between two L-arm vertices of the watermelon geometry, the magnetic charges at X and Y are due to a vortex and anti-vortex pair with L/2 dislocations m X = −m Y = L/2, and the electric charges at X and Y are given as e X = e Y = 1 − g, and hence the scaling dimension x L = −(gm X m Y + e X e Y /g)/2 is expressed in terms of g and L 14 = x L g g g 8…”
Section: Contact Exponentmentioning
confidence: 99%
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“…Note that near θ-temperature and in the low molecular weight limit, large deviations from Gaussian chain properties have been reported, and the R g 2 deviates from the ideal chain behavior could have the square root correction format , or the logarithmic correction . For the logarithmic correction model, B = 37/363, −37/363 and 1.9/(44π) are reported by mean-field theory methods .…”
Section: Resultsmentioning
confidence: 99%