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Dust and gas power spectrum in M 33 (HERM33ES)

Identifieur interne : 005D12 ( Main/Exploration ); précédent : 005D11; suivant : 005D13

Dust and gas power spectrum in M 33 (HERM33ES)

Auteurs : F. Combes [France] ; M. Boquien [France] ; C. Kramer [Espagne] ; E. M. Xilouris [Grèce] ; F. Bertoldi [Allemagne] ; J. Braine [France] ; C. Buchbender [Espagne] ; D. Calzetti [États-Unis] ; P. Gratier [France] ; F. Israel [Pays-Bas] ; B. Koribalski [Australie] ; S. Lord [États-Unis] ; G. Quintana-Lacaci [Espagne] ; M. Relano [Espagne] ; M. Röllig [Allemagne] ; G. Stacey [États-Unis] ; F. S. Tabatabaei [Allemagne] ; R. P. J. Tilanus [États-Unis] ; F. Van Der Tak [Pays-Bas] ; P. Van Der Werf [Pays-Bas] ; S. Verley [France]

Source :

RBID : Pascal:12-0194663

Descripteurs français

English descriptors

Abstract

Power spectra of deprojected images of late-type galaxies in gas or dust emission are very useful diagnostics of the dynamics and stability of their interstellar medium. Previous studies have shown that the power spectra can be approximated as two power laws, a shallow one on large scales (larger than 500 pc) and a steeper one on small scales, with the break between the two corresponding to the line-of-sight thickness of the galaxy disk. The break separates the 3D behavior of the interstellar medium on small scales, controlled by star formation and feedback, from the 2D behavior on large scales, driven by density waves in the disk. The break between these two regimes depends on the thickness of the plane, which is determined by the natural self-gravitating scale of the interstellar medium. We present a thorough analysis of the power spectra of the dust and gas emission at several wavelengths in the nearby galaxy M 33. In particular, we use the recently obtained images at five wavelengths by PACS and SPIRE onboard Herschel. The wide dynamical range (2-3 dex in scale) of most images allows us to clearly determine the change in slopes from -1.5 to -4, with some variations with wavelength. The break scale increases with wavelength from 100 pc at 24 and 100 μm to 350 pc at 500 μm, suggesting that the cool dust lies in a thicker disk than the warm dust, perhaps because of star formation that is more confined to the plane. The slope on small scales tends to be steeper at longer wavelength, meaning that the warmer dust is more concentrated in clumps. Numerical simulations of an isolated late-type galaxy, rich in gas and with no bulge, such as M 33, are carried out to better interpret these observed results. Varying the star formation and feedback parameters, it is possible to obtain a range of power spectra, with two power-law slopes and breaks, that nicely bracket the data. The small-scale power-law does indeed reflect the 3D behavior of the gas layer, steepening strongly while the feedback smoothes the structures by increasing the gas turbulence. M 33 appears to correspond to a fiducial model with an SFR of ∼0.7 M◦./yr, with 10% supernovae energy coupled to the gas kinematics.


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<name sortKey="Quintana Lacaci, G" sort="Quintana Lacaci, G" uniqKey="Quintana Lacaci G" first="G." last="Quintana-Lacaci">G. Quintana-Lacaci</name>
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<name sortKey="Relano, M" sort="Relano, M" uniqKey="Relano M" first="M." last="Relano">M. Relano</name>
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<country>Espagne</country>
<placeName>
<settlement type="city">Grenade (Espagne)</settlement>
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<orgName type="university">Université de Grenade</orgName>
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</author>
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<name sortKey="Rollig, M" sort="Rollig, M" uniqKey="Rollig M" first="M." last="Röllig">M. Röllig</name>
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<settlement type="city">Cologne</settlement>
<settlement type="city">Cologne</settlement>
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<country>États-Unis</country>
<placeName>
<settlement type="city">Ithaca (New York)</settlement>
<region type="state">État de New York</region>
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<orgName type="university">Université Cornell</orgName>
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</author>
<author>
<name sortKey="Tabatabaei, F S" sort="Tabatabaei, F S" uniqKey="Tabatabaei F" first="F. S." last="Tabatabaei">F. S. Tabatabaei</name>
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<s1>Max Planck Institut fur Astronomie, Königstuhl 17</s1>
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<name sortKey="Verley, S" sort="Verley, S" uniqKey="Verley S" first="S." last="Verley">S. Verley</name>
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<country>France</country>
<wicri:noRegion>75014 Paris</wicri:noRegion>
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<settlement type="city">Paris</settlement>
<region type="région" nuts="2">Île-de-France</region>
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</author>
</analytic>
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<title level="j" type="main">Astronomy and astrophysics : (Berlin. Print)</title>
<title level="j" type="abbreviated">Astron. astrophys. : (Berl., Print)</title>
<idno type="ISSN">0004-6361</idno>
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<date when="2012">2012</date>
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<title level="j" type="main">Astronomy and astrophysics : (Berlin. Print)</title>
<title level="j" type="abbreviated">Astron. astrophys. : (Berl., Print)</title>
<idno type="ISSN">0004-6361</idno>
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<textClass>
<keywords scheme="KwdEn" xml:lang="en">
<term>Density waves</term>
<term>Digital simulation</term>
<term>Disk galaxies</term>
<term>Dynamic stability</term>
<term>Feedback</term>
<term>Galaxy structure</term>
<term>Interstellar matter</term>
<term>Kinematics</term>
<term>Late type galaxies</term>
<term>Local group</term>
<term>Models</term>
<term>Power law</term>
<term>Power spectra</term>
<term>Self-gravitating systems</term>
<term>Spiral galaxies</term>
<term>Star formation</term>
<term>Supernovae</term>
<term>Turbulence</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Spectre puissance</term>
<term>Galaxies type avancé</term>
<term>Stabilité dynamique</term>
<term>Matière interstellaire</term>
<term>Loi puissance</term>
<term>Galaxies disques</term>
<term>Formation stellaire</term>
<term>Boucle réaction</term>
<term>Onde densité</term>
<term>Système autogravitant</term>
<term>Simulation numérique</term>
<term>Turbulence</term>
<term>Modèle</term>
<term>Supernova</term>
<term>Cinématique</term>
<term>Structure galaxies</term>
<term>Galaxies spirales</term>
<term>Groupe local</term>
</keywords>
</textClass>
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<front>
<div type="abstract" xml:lang="en">Power spectra of deprojected images of late-type galaxies in gas or dust emission are very useful diagnostics of the dynamics and stability of their interstellar medium. Previous studies have shown that the power spectra can be approximated as two power laws, a shallow one on large scales (larger than 500 pc) and a steeper one on small scales, with the break between the two corresponding to the line-of-sight thickness of the galaxy disk. The break separates the 3D behavior of the interstellar medium on small scales, controlled by star formation and feedback, from the 2D behavior on large scales, driven by density waves in the disk. The break between these two regimes depends on the thickness of the plane, which is determined by the natural self-gravitating scale of the interstellar medium. We present a thorough analysis of the power spectra of the dust and gas emission at several wavelengths in the nearby galaxy M 33. In particular, we use the recently obtained images at five wavelengths by PACS and SPIRE onboard Herschel. The wide dynamical range (2-3 dex in scale) of most images allows us to clearly determine the change in slopes from -1.5 to -4, with some variations with wavelength. The break scale increases with wavelength from 100 pc at 24 and 100 μm to 350 pc at 500 μm, suggesting that the cool dust lies in a thicker disk than the warm dust, perhaps because of star formation that is more confined to the plane. The slope on small scales tends to be steeper at longer wavelength, meaning that the warmer dust is more concentrated in clumps. Numerical simulations of an isolated late-type galaxy, rich in gas and with no bulge, such as M 33, are carried out to better interpret these observed results. Varying the star formation and feedback parameters, it is possible to obtain a range of power spectra, with two power-law slopes and breaks, that nicely bracket the data. The small-scale power-law does indeed reflect the 3D behavior of the gas layer, steepening strongly while the feedback smoothes the structures by increasing the gas turbulence. M 33 appears to correspond to a fiducial model with an SFR of ∼0.7 M
<sub>◦.</sub>
/yr, with 10% supernovae energy coupled to the gas kinematics.</div>
</front>
</TEI>
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<list>
<country>
<li>Allemagne</li>
<li>Australie</li>
<li>Espagne</li>
<li>France</li>
<li>Grèce</li>
<li>Pays-Bas</li>
<li>États-Unis</li>
</country>
<region>
<li>Andalousie</li>
<li>Attique (région)</li>
<li>District de Cologne</li>
<li>Massachusetts</li>
<li>Provence-Alpes-Côte d'Azur</li>
<li>Rhénanie-du-Nord-Westphalie</li>
<li>État de New York</li>
<li>Île-de-France</li>
</region>
<settlement>
<li>Amherst (Massachusetts)</li>
<li>Athènes</li>
<li>Bonn</li>
<li>Cologne</li>
<li>Grenade (Espagne)</li>
<li>Ithaca (New York)</li>
<li>Marseille</li>
<li>Paris</li>
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<orgName>
<li>Université Cornell</li>
<li>Université de Cologne</li>
<li>Université de Grenade</li>
<li>Université du Massachusetts</li>
</orgName>
</list>
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<country name="France">
<region name="Île-de-France">
<name sortKey="Combes, F" sort="Combes, F" uniqKey="Combes F" first="F." last="Combes">F. Combes</name>
</region>
<name sortKey="Boquien, M" sort="Boquien, M" uniqKey="Boquien M" first="M." last="Boquien">M. Boquien</name>
<name sortKey="Braine, J" sort="Braine, J" uniqKey="Braine J" first="J." last="Braine">J. Braine</name>
<name sortKey="Gratier, P" sort="Gratier, P" uniqKey="Gratier P" first="P." last="Gratier">P. Gratier</name>
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<region name="Andalousie">
<name sortKey="Kramer, C" sort="Kramer, C" uniqKey="Kramer C" first="C." last="Kramer">C. Kramer</name>
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<name sortKey="Buchbender, C" sort="Buchbender, C" uniqKey="Buchbender C" first="C." last="Buchbender">C. Buchbender</name>
<name sortKey="Quintana Lacaci, G" sort="Quintana Lacaci, G" uniqKey="Quintana Lacaci G" first="G." last="Quintana-Lacaci">G. Quintana-Lacaci</name>
<name sortKey="Relano, M" sort="Relano, M" uniqKey="Relano M" first="M." last="Relano">M. Relano</name>
</country>
<country name="Grèce">
<region name="Attique (région)">
<name sortKey="Xilouris, E M" sort="Xilouris, E M" uniqKey="Xilouris E" first="E. M." last="Xilouris">E. M. Xilouris</name>
</region>
</country>
<country name="Allemagne">
<region name="Rhénanie-du-Nord-Westphalie">
<name sortKey="Bertoldi, F" sort="Bertoldi, F" uniqKey="Bertoldi F" first="F." last="Bertoldi">F. Bertoldi</name>
</region>
<name sortKey="Rollig, M" sort="Rollig, M" uniqKey="Rollig M" first="M." last="Röllig">M. Röllig</name>
<name sortKey="Tabatabaei, F S" sort="Tabatabaei, F S" uniqKey="Tabatabaei F" first="F. S." last="Tabatabaei">F. S. Tabatabaei</name>
</country>
<country name="États-Unis">
<region name="Massachusetts">
<name sortKey="Calzetti, D" sort="Calzetti, D" uniqKey="Calzetti D" first="D." last="Calzetti">D. Calzetti</name>
</region>
<name sortKey="Lord, S" sort="Lord, S" uniqKey="Lord S" first="S." last="Lord">S. Lord</name>
<name sortKey="Stacey, G" sort="Stacey, G" uniqKey="Stacey G" first="G." last="Stacey">G. Stacey</name>
<name sortKey="Tilanus, R P J" sort="Tilanus, R P J" uniqKey="Tilanus R" first="R. P. J." last="Tilanus">R. P. J. Tilanus</name>
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<noRegion>
<name sortKey="Israel, F" sort="Israel, F" uniqKey="Israel F" first="F." last="Israel">F. Israel</name>
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<name sortKey="Der Werf, P Van" sort="Der Werf, P Van" uniqKey="Der Werf P" first="P. Van" last="Der Werf">P. Van Der Werf</name>
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