Electrical conductivity of a monolayer produced by random sequential adsorption of linear $k$-mers onto a square lattice
Phys. Rev. E 94, 042112 (2016) The electrical conductivity of a monolayer produced by the random sequential adsorption (RSA) of linear $k$-mers onto a square lattice was studied by means of computer simulation. Overlapping with pre-deposited $k$-mers and detachment from the surface were forbidden. T...
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creator | Tarasevich, Yuri Yu Laptev, Valeri V Goltseva, Valeria A Lebovka, Nikolai I |
description | Phys. Rev. E 94, 042112 (2016) The electrical conductivity of a monolayer produced by the random sequential
adsorption (RSA) of linear $k$-mers onto a square lattice was studied by means
of computer simulation. Overlapping with pre-deposited $k$-mers and detachment
from the surface were forbidden. The RSA continued until the saturation jamming
limit, $p_j$. The isotropic and anisotropic depositions for two different
models: of an insulating substrate and conducting $k$-mers (C-model) and of a
conducting substrate and insulating $k$-mers (I-model) were examined. The
Frank-Lobb algorithm was applied to calculate the electrical conductivity in
both the $x$ and $y$ directions for different lengths ($k=1$ -- $128 $) and
concentrations ($p=0$ -- $p_j$) of the $k$-mers. The `intrinsic electrical
conductivity' and concentration dependence of the relative electrical
conductivity $\Sigma (p)$ ($\Sigma=\sigma/ \sigma_m$ for the C-model and
$\Sigma=\sigma_m /\sigma$ for the I-model, where $\sigma_m$ is the electrical
conductivity of substrate) in different directions were analyzed. At large
values of $k$ the $\Sigma (p)$ curves became very similar and they almost
coincided at $k=128$. Moreover, for both models the greater the length of the
$k$-mers the smoother the functions $\Sigma_{xy}(p)$, $\Sigma_{x}(p)$ and
$\Sigma_{y}(p)$. For the C-model, the other interesting findings are: for large
values of $k$ ($k=64, 128$), the values of $\Sigma_{xy}$ and $\Sigma_{y}$
increase rapidly with the initial increase of $p$ from 0 to 0.1; for $k \geq
16$, all the $\Sigma_{xy}(p)$ and $\Sigma_{x}(p)$ curves intersect with each
other at the same iso-conductivity points; for anisotropic deposition, the
percolation concentrations are the same in the $x$ and $y$ directions, whereas,
at the percolation point the greater the length of the $k$-mers the larger the
anisotropy of the electrical conductivity, i.e., the ratio $\sigma_y/\sigma_x$
($>1$). |
doi_str_mv | 10.48550/arxiv.1607.08385 |
format | Article |
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adsorption (RSA) of linear $k$-mers onto a square lattice was studied by means
of computer simulation. Overlapping with pre-deposited $k$-mers and detachment
from the surface were forbidden. The RSA continued until the saturation jamming
limit, $p_j$. The isotropic and anisotropic depositions for two different
models: of an insulating substrate and conducting $k$-mers (C-model) and of a
conducting substrate and insulating $k$-mers (I-model) were examined. The
Frank-Lobb algorithm was applied to calculate the electrical conductivity in
both the $x$ and $y$ directions for different lengths ($k=1$ -- $128 $) and
concentrations ($p=0$ -- $p_j$) of the $k$-mers. The `intrinsic electrical
conductivity' and concentration dependence of the relative electrical
conductivity $\Sigma (p)$ ($\Sigma=\sigma/ \sigma_m$ for the C-model and
$\Sigma=\sigma_m /\sigma$ for the I-model, where $\sigma_m$ is the electrical
conductivity of substrate) in different directions were analyzed. At large
values of $k$ the $\Sigma (p)$ curves became very similar and they almost
coincided at $k=128$. Moreover, for both models the greater the length of the
$k$-mers the smoother the functions $\Sigma_{xy}(p)$, $\Sigma_{x}(p)$ and
$\Sigma_{y}(p)$. For the C-model, the other interesting findings are: for large
values of $k$ ($k=64, 128$), the values of $\Sigma_{xy}$ and $\Sigma_{y}$
increase rapidly with the initial increase of $p$ from 0 to 0.1; for $k \geq
16$, all the $\Sigma_{xy}(p)$ and $\Sigma_{x}(p)$ curves intersect with each
other at the same iso-conductivity points; for anisotropic deposition, the
percolation concentrations are the same in the $x$ and $y$ directions, whereas,
at the percolation point the greater the length of the $k$-mers the larger the
anisotropy of the electrical conductivity, i.e., the ratio $\sigma_y/\sigma_x$
($>1$).</description><identifier>DOI: 10.48550/arxiv.1607.08385</identifier><language>eng</language><subject>Physics - Statistical Mechanics</subject><creationdate>2016-07</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/1607.08385$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.1607.08385$$DView paper in arXiv$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.1103/PhysRevE.94.042112$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink></links><search><creatorcontrib>Tarasevich, Yuri Yu</creatorcontrib><creatorcontrib>Laptev, Valeri V</creatorcontrib><creatorcontrib>Goltseva, Valeria A</creatorcontrib><creatorcontrib>Lebovka, Nikolai I</creatorcontrib><title>Electrical conductivity of a monolayer produced by random sequential adsorption of linear $k$-mers onto a square lattice</title><description>Phys. Rev. E 94, 042112 (2016) The electrical conductivity of a monolayer produced by the random sequential
adsorption (RSA) of linear $k$-mers onto a square lattice was studied by means
of computer simulation. Overlapping with pre-deposited $k$-mers and detachment
from the surface were forbidden. The RSA continued until the saturation jamming
limit, $p_j$. The isotropic and anisotropic depositions for two different
models: of an insulating substrate and conducting $k$-mers (C-model) and of a
conducting substrate and insulating $k$-mers (I-model) were examined. The
Frank-Lobb algorithm was applied to calculate the electrical conductivity in
both the $x$ and $y$ directions for different lengths ($k=1$ -- $128 $) and
concentrations ($p=0$ -- $p_j$) of the $k$-mers. The `intrinsic electrical
conductivity' and concentration dependence of the relative electrical
conductivity $\Sigma (p)$ ($\Sigma=\sigma/ \sigma_m$ for the C-model and
$\Sigma=\sigma_m /\sigma$ for the I-model, where $\sigma_m$ is the electrical
conductivity of substrate) in different directions were analyzed. At large
values of $k$ the $\Sigma (p)$ curves became very similar and they almost
coincided at $k=128$. Moreover, for both models the greater the length of the
$k$-mers the smoother the functions $\Sigma_{xy}(p)$, $\Sigma_{x}(p)$ and
$\Sigma_{y}(p)$. For the C-model, the other interesting findings are: for large
values of $k$ ($k=64, 128$), the values of $\Sigma_{xy}$ and $\Sigma_{y}$
increase rapidly with the initial increase of $p$ from 0 to 0.1; for $k \geq
16$, all the $\Sigma_{xy}(p)$ and $\Sigma_{x}(p)$ curves intersect with each
other at the same iso-conductivity points; for anisotropic deposition, the
percolation concentrations are the same in the $x$ and $y$ directions, whereas,
at the percolation point the greater the length of the $k$-mers the larger the
anisotropy of the electrical conductivity, i.e., the ratio $\sigma_y/\sigma_x$
($>1$).</description><subject>Physics - Statistical Mechanics</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNqFjrEOgkAQRK-xMOoHWLkFLYhRlN5o_AB7sh5LsvG4xb3DyN-Lxt5qipk3ecYsN3m2K4siX6O--Jlt9vkhy8ttWUzN6-TIRmWLDqz4ureRnxwHkAYQWvHicCCFTmXsqIbbAIq-lhYCPXrykUcS6yDaRRb_4Rx7QoXknqQtaQDxUcaz8OhRCRzGyJbmZtKgC7T45cyszqfr8ZJ-HatOuUUdqo9r9XXd_l-8ASg-S_Y</recordid><startdate>20160728</startdate><enddate>20160728</enddate><creator>Tarasevich, Yuri Yu</creator><creator>Laptev, Valeri V</creator><creator>Goltseva, Valeria A</creator><creator>Lebovka, Nikolai I</creator><scope>GOX</scope></search><sort><creationdate>20160728</creationdate><title>Electrical conductivity of a monolayer produced by random sequential adsorption of linear $k$-mers onto a square lattice</title><author>Tarasevich, Yuri Yu ; Laptev, Valeri V ; Goltseva, Valeria A ; Lebovka, Nikolai I</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_1607_083853</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Physics - Statistical Mechanics</topic><toplevel>online_resources</toplevel><creatorcontrib>Tarasevich, Yuri Yu</creatorcontrib><creatorcontrib>Laptev, Valeri V</creatorcontrib><creatorcontrib>Goltseva, Valeria A</creatorcontrib><creatorcontrib>Lebovka, Nikolai I</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Tarasevich, Yuri Yu</au><au>Laptev, Valeri V</au><au>Goltseva, Valeria A</au><au>Lebovka, Nikolai I</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Electrical conductivity of a monolayer produced by random sequential adsorption of linear $k$-mers onto a square lattice</atitle><date>2016-07-28</date><risdate>2016</risdate><abstract>Phys. Rev. E 94, 042112 (2016) The electrical conductivity of a monolayer produced by the random sequential
adsorption (RSA) of linear $k$-mers onto a square lattice was studied by means
of computer simulation. Overlapping with pre-deposited $k$-mers and detachment
from the surface were forbidden. The RSA continued until the saturation jamming
limit, $p_j$. The isotropic and anisotropic depositions for two different
models: of an insulating substrate and conducting $k$-mers (C-model) and of a
conducting substrate and insulating $k$-mers (I-model) were examined. The
Frank-Lobb algorithm was applied to calculate the electrical conductivity in
both the $x$ and $y$ directions for different lengths ($k=1$ -- $128 $) and
concentrations ($p=0$ -- $p_j$) of the $k$-mers. The `intrinsic electrical
conductivity' and concentration dependence of the relative electrical
conductivity $\Sigma (p)$ ($\Sigma=\sigma/ \sigma_m$ for the C-model and
$\Sigma=\sigma_m /\sigma$ for the I-model, where $\sigma_m$ is the electrical
conductivity of substrate) in different directions were analyzed. At large
values of $k$ the $\Sigma (p)$ curves became very similar and they almost
coincided at $k=128$. Moreover, for both models the greater the length of the
$k$-mers the smoother the functions $\Sigma_{xy}(p)$, $\Sigma_{x}(p)$ and
$\Sigma_{y}(p)$. For the C-model, the other interesting findings are: for large
values of $k$ ($k=64, 128$), the values of $\Sigma_{xy}$ and $\Sigma_{y}$
increase rapidly with the initial increase of $p$ from 0 to 0.1; for $k \geq
16$, all the $\Sigma_{xy}(p)$ and $\Sigma_{x}(p)$ curves intersect with each
other at the same iso-conductivity points; for anisotropic deposition, the
percolation concentrations are the same in the $x$ and $y$ directions, whereas,
at the percolation point the greater the length of the $k$-mers the larger the
anisotropy of the electrical conductivity, i.e., the ratio $\sigma_y/\sigma_x$
($>1$).</abstract><doi>10.48550/arxiv.1607.08385</doi><oa>free_for_read</oa></addata></record> |
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title | Electrical conductivity of a monolayer produced by random sequential adsorption of linear $k$-mers onto a square lattice |
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