Randomly Charged Polymers - Polyampholytes

Yacov Kantor


Equilbrium configuration of polyampholyte.
Different colors represent opposite charges.


Spatial configurations of polyampholytes are
very sensitive to the overall excess charge Q.
At low temperature polyampholytes with small
Q are compact, while the polyampholytes with
moderate Q are stretched.

See PRL 96,61(92); PRE49,1383(94);
Europhys.Lett. 27,643(94) PRE51,1299(95)
(with M.Kardar, H.Li)





Tethered Surfaces with Randomness

Yacov Kantor


Ground state of a polymerized memebrane
consisting of monomers of two randomly selected
sizes.


Ground state of a polymerized membrane
with quenched randomness is highly folded.
As the temperature increases the configuration
becomes more flat despite the thermal
fluctuations. Further increase of temperature
leads again to a crumpled state.

See Europhys.Lett. 20,169(94) (with K. Kremer).




Extremal Properties of Random Walks

Yacov Kantor

Probability density that the largest
segment of an N charge sequence +-1
which has reduced charge q=Q/N**(1/2)
has reduced length l=L/N.


For q=0 (neutral segments) probability
density p has square-root singularity
near l=1, essential singularity at l=0
and discontinuous derivative at l=1/2.

See J.Physics A27,L907(95); PRE53,846(95)
(with D. Ertas and S. Wolfling)





Elasticity of Entropy-Dominated Systems

Yacov Kantor

Equilibrium configuration of random
phantom network.


Elastic properties of gels have been studied.

See Phys. Rev. Lett. 85,2533(00);
Europhys. Lett. 52,413(00)
(with O. Farago)





Properties of Knots in Polymers

Yacov Kantor

Knot in a polymer on a cubic lattice.

Size distribution of two- and three-dimensional
knots has been investigated. It was shown that
both entropy and electrostatic interactions favor
"small" knots.

See Phys. Rev. Lett. 88,18810(02);
Europhys. Lett. 60,53(02)
Phys. Rev. E66,31802(02)
(with R. Metzler, A. Hanke, P. G. Dommersnes,
O. Farago, and M. Kardar)





Translocation of a Polymer through a Pore in Membrane

Yacov Kantor

Polymer translocating through a pore.

Translocation time of a long polymer was
investigated a s function of polymer length
and the forces applied to it.

See Phys. Rev. E65,11802(02);
Phys. Rev. E69,21806(03)
(with J. Chuang and M. Kardar)





Polymers Attached to Probes

Yacov Kantor

Distribution of the end-point of a polymer attached to a sphere

In single-molecule mechanical experiments
the probe to which the polymer is attached
influences its behavior.

See Europhys. Lett. 88,48001 (09)
(with R. Bubis and M. Kardar)





Localization of Random Walks near Competing Manifolds

Yacov Kantor

Corner, edge and face have dimensionalities 0, 1 and 2

Adsorbtion of random walk or polymer to
surfaces of competing dimensionalities creates
a complex phase diagram.

See Phys. Rev. E98,022108 (19)
(with R. Halifa Levi and M. Kardar)







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