Spectrum of the M 5 -traveling waves
In this paper, we study the essential spectrum of the operator obtained by linearizing at traveling waves that occur in the one-dimensional version of the M 5 -model for mesenchymal cell movement inside a directed tissue made up of highly aligned fibers. We show that traveling waves are spectrally u...
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Veröffentlicht in: | Mathematical modelling of natural phenomena 2020-12, Vol.15, p.66 |
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description | In this paper, we study the essential spectrum of the operator obtained by linearizing at traveling waves that occur in the one-dimensional version of the M
5
-model for mesenchymal cell movement inside a directed tissue made up of highly aligned fibers. We show that traveling waves are spectrally unstable in
L
2
(ℝ; ℂ
3
) as the essential spectrum includes the imaginary axis. Tools in the proof include exponential dichotomies and Fredholm properties. We prove that a weighted space
L
w
2
(ℝ; ℂ
3
) with the same function for the tree variables of the linearized operator is no suitable to shift the essential spectrum to the left of the imaginary axis. We find a pair of appropriate weight functions whereby on the weighted space
L
wα
2
(ℝ; ℂ
2
) ×
L
wε
2
(ℝ; ℂ) the essential spectrum lies on {
Reλ |
doi_str_mv | 10.1051/mmnp/2020039 |
format | Article |
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5
-model for mesenchymal cell movement inside a directed tissue made up of highly aligned fibers. We show that traveling waves are spectrally unstable in
L
2
(ℝ; ℂ
3
) as the essential spectrum includes the imaginary axis. Tools in the proof include exponential dichotomies and Fredholm properties. We prove that a weighted space
L
w
2
(ℝ; ℂ
3
) with the same function for the tree variables of the linearized operator is no suitable to shift the essential spectrum to the left of the imaginary axis. We find a pair of appropriate weight functions whereby on the weighted space
L
wα
2
(ℝ; ℂ
2
) ×
L
wε
2
(ℝ; ℂ) the essential spectrum lies on {
Reλ
<0}, outside the imaginary axis.</description><identifier>ISSN: 0973-5348</identifier><identifier>EISSN: 1760-6101</identifier><identifier>DOI: 10.1051/mmnp/2020039</identifier><language>eng</language><ispartof>Mathematical modelling of natural phenomena, 2020-12, Vol.15, p.66</ispartof><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c122t-fef084be1b5a66c5c7386c2b4d2c97e57f7ae31fa52260e4309b5f54c0b3219f3</cites><orcidid>0000-0001-9153-657X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Cruz-García, Salvador</creatorcontrib><title>Spectrum of the M 5 -traveling waves</title><title>Mathematical modelling of natural phenomena</title><description>In this paper, we study the essential spectrum of the operator obtained by linearizing at traveling waves that occur in the one-dimensional version of the M
5
-model for mesenchymal cell movement inside a directed tissue made up of highly aligned fibers. We show that traveling waves are spectrally unstable in
L
2
(ℝ; ℂ
3
) as the essential spectrum includes the imaginary axis. Tools in the proof include exponential dichotomies and Fredholm properties. We prove that a weighted space
L
w
2
(ℝ; ℂ
3
) with the same function for the tree variables of the linearized operator is no suitable to shift the essential spectrum to the left of the imaginary axis. We find a pair of appropriate weight functions whereby on the weighted space
L
wα
2
(ℝ; ℂ
2
) ×
L
wε
2
(ℝ; ℂ) the essential spectrum lies on {
Reλ
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5
-model for mesenchymal cell movement inside a directed tissue made up of highly aligned fibers. We show that traveling waves are spectrally unstable in
L
2
(ℝ; ℂ
3
) as the essential spectrum includes the imaginary axis. Tools in the proof include exponential dichotomies and Fredholm properties. We prove that a weighted space
L
w
2
(ℝ; ℂ
3
) with the same function for the tree variables of the linearized operator is no suitable to shift the essential spectrum to the left of the imaginary axis. We find a pair of appropriate weight functions whereby on the weighted space
L
wα
2
(ℝ; ℂ
2
) ×
L
wε
2
(ℝ; ℂ) the essential spectrum lies on {
Reλ
<0}, outside the imaginary axis.</abstract><doi>10.1051/mmnp/2020039</doi><orcidid>https://orcid.org/0000-0001-9153-657X</orcidid><oa>free_for_read</oa></addata></record> |
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source | Free E-Journal (出版社公開部分のみ); Alma/SFX Local Collection |
title | Spectrum of the M 5 -traveling waves |
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