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K-band observations of boxy bulges. I. Morphology and surface brightness profiles

Identifieur interne : 001E05 ( PascalFrancis/Curation ); précédent : 001E04; suivant : 001E06

K-band observations of boxy bulges. I. Morphology and surface brightness profiles

Auteurs : M. Bureau [Royaume-Uni] ; G. Aronica [Allemagne, France] ; E. Athanassoula [France] ; R.-J. Dettmar [Allemagne] ; A. Bosma [France] ; K. C. Freeman [Australie]

Source :

RBID : Pascal:06-0351143

Descripteurs français

English descriptors

Abstract

In this first paper of a series on the structure of boxy and peanut-shaped (B/PS) bulges, Kn-band observations of a sample of 30 edge-on spiral galaxies are described and discussed. Kn-band observations best trace the dominant luminous galactic mass and are minimally affected by dust. Images, unsharp-masked images, as well as major-axis and vertically summed surface brightness profiles are presented and discussed. Galaxies with a B/PS bulge tend to have a more complex morphology than galaxies with other bulge types, more often showing centred or off-centred X structures, secondary maxima along the major-axis and spiral-like structures. While probably not uniquely related to bars, those features are observed in three-dimensional N-body simulations of barred discs and may trace the main bar orbit families. The surface brightness profiles of galaxies with a B/PS bulge are also more complex, typically containing three or more clearly separated regions, including a shallow or flat intermediate region (Freeman Type II profiles). The breaks in the profiles offer evidence for bar-driven transfer of angular momentum and radial redistribution of material. The profiles further suggest a rapid variation of the scaleheight of the disc material, contrary to conventional wisdom but again as expected from the vertical resonances and instabilities present in barred discs. Interestingly, the steep inner region of the surface brightness profiles is often shorter than the isophotally thick part of the galaxies, itself always shorter than the flat intermediate region of the profiles. The steep inner region is also much more prominent along the major-axis than in the vertically summed profiles. Similarly to other recent work but contrary to the standard 'bulge + disc' model (where the bulge is both thick and steep), we thus propose that galaxies with a B/PS bulge are composed of a thin concentrated disc (a disc-like bulge) contained within a partially thick bar (the B/PS bulge), itself contained within a thin outer disc. The inner disc likely formed secularly through bar-driven processes and is responsible for the steep inner region of the surface brightness profiles, traditionally associated with a classic bulge, while the bar is responsible for the flat intermediate region of the surface brightness profiles and the thick complex morphological structures observed. Those components are strongly coupled dynamically and are formed mostly of the same (disc) material, shaped by the weak but relentless action of the bar resonances. Any competing formation scenario for galaxies with a B/PS bulge, which represent at least 45 per cent of the local disc galaxy population, must explain equally well and self-consistently the above morphological and photometric properties, the complex gas and stellar kinematics observed, and the correlations between them.
pA  
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A08 01  1  ENG  @1 K-band observations of boxy bulges. I. Morphology and surface brightness profiles
A11 01  1    @1 BUREAU (M.)
A11 02  1    @1 ARONICA (G.)
A11 03  1    @1 ATHANASSOULA (E.)
A11 04  1    @1 DETTMAR (R.-J.)
A11 05  1    @1 BOSMA (A.)
A11 06  1    @1 FREEMAN (K. C.)
A14 01      @1 Sub-Department of Astrophysics, University of Oxford, Denys Wilkinson Building, Keble Road @2 Oxford OX1 3RH @3 GBR @Z 1 aut.
A14 02      @1 Astronamisches Institut, Ruhr-Universität Bochum @2 44780 Bochum @3 DEU @Z 2 aut. @Z 4 aut.
A14 03      @1 Observatoire de Marseille, 2 place Le Verrier @2 13248 Marseille @3 FRA @Z 2 aut. @Z 3 aut. @Z 5 aut.
A14 04      @1 Research School of Astronomy and Astrophysics, The Australian National University, Weston Creek P.O @2 ACT 2611 @3 AUS @Z 6 aut.
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C01 01    ENG  @0 In this first paper of a series on the structure of boxy and peanut-shaped (B/PS) bulges, Kn-band observations of a sample of 30 edge-on spiral galaxies are described and discussed. Kn-band observations best trace the dominant luminous galactic mass and are minimally affected by dust. Images, unsharp-masked images, as well as major-axis and vertically summed surface brightness profiles are presented and discussed. Galaxies with a B/PS bulge tend to have a more complex morphology than galaxies with other bulge types, more often showing centred or off-centred X structures, secondary maxima along the major-axis and spiral-like structures. While probably not uniquely related to bars, those features are observed in three-dimensional N-body simulations of barred discs and may trace the main bar orbit families. The surface brightness profiles of galaxies with a B/PS bulge are also more complex, typically containing three or more clearly separated regions, including a shallow or flat intermediate region (Freeman Type II profiles). The breaks in the profiles offer evidence for bar-driven transfer of angular momentum and radial redistribution of material. The profiles further suggest a rapid variation of the scaleheight of the disc material, contrary to conventional wisdom but again as expected from the vertical resonances and instabilities present in barred discs. Interestingly, the steep inner region of the surface brightness profiles is often shorter than the isophotally thick part of the galaxies, itself always shorter than the flat intermediate region of the profiles. The steep inner region is also much more prominent along the major-axis than in the vertically summed profiles. Similarly to other recent work but contrary to the standard 'bulge + disc' model (where the bulge is both thick and steep), we thus propose that galaxies with a B/PS bulge are composed of a thin concentrated disc (a disc-like bulge) contained within a partially thick bar (the B/PS bulge), itself contained within a thin outer disc. The inner disc likely formed secularly through bar-driven processes and is responsible for the steep inner region of the surface brightness profiles, traditionally associated with a classic bulge, while the bar is responsible for the flat intermediate region of the surface brightness profiles and the thick complex morphological structures observed. Those components are strongly coupled dynamically and are formed mostly of the same (disc) material, shaped by the weak but relentless action of the bar resonances. Any competing formation scenario for galaxies with a B/PS bulge, which represent at least 45 per cent of the local disc galaxy population, must explain equally well and self-consistently the above morphological and photometric properties, the complex gas and stellar kinematics observed, and the correlations between them.
C02 01  3    @0 001E03
C03 01  3  FRE  @0 Morphologie @5 26
C03 01  3  ENG  @0 Morphology @5 26
C03 02  X  FRE  @0 Brillance surface @5 27
C03 02  X  ENG  @0 Surface brightness @5 27
C03 02  X  SPA  @0 Brillantez superficie @5 27
C03 03  3  FRE  @0 Galaxies spirales @5 28
C03 03  3  ENG  @0 Spiral galaxies @5 28
C03 04  X  FRE  @0 Structure spirale @5 29
C03 04  X  ENG  @0 Spiral structure @5 29
C03 04  X  SPA  @0 Estructura espiral @5 29
C03 05  3  FRE  @0 Simulation numérique @5 30
C03 05  3  ENG  @0 Digital simulation @5 30
C03 06  X  FRE  @0 Système n corps @5 31
C03 06  X  ENG  @0 N body system @5 31
C03 06  X  SPA  @0 Sistema n cuerpos @5 31
C03 07  3  FRE  @0 Orbite @5 32
C03 07  3  ENG  @0 Orbits @5 32
C03 08  3  FRE  @0 Transfert moment cinétique @5 33
C03 08  3  ENG  @0 Angular momentum transfer @5 33
C03 09  X  FRE  @0 Variation rapide @5 34
C03 09  X  ENG  @0 Fast variation @5 34
C03 09  X  SPA  @0 Variación rápida @5 34
C03 10  3  FRE  @0 Résonance @5 35
C03 10  3  ENG  @0 Resonance @5 35
C03 11  3  FRE  @0 Instabilité @5 36
C03 11  3  ENG  @0 Instability @5 36
C03 12  X  FRE  @0 Modèle @5 37
C03 12  X  ENG  @0 Models @5 37
C03 12  X  SPA  @0 Modelo @5 37
C03 13  X  FRE  @0 Couplage fort @5 38
C03 13  X  ENG  @0 Strong coupling @5 38
C03 13  X  SPA  @0 Acoplamiento fuerte @5 38
C03 14  3  FRE  @0 Formation galaxies @5 39
C03 14  3  ENG  @0 Galaxy formation @5 39
C03 15  3  FRE  @0 Galaxies disques @5 40
C03 15  3  ENG  @0 Disk galaxies @5 40
C03 16  X  FRE  @0 Cinématique stellaire @5 41
C03 16  X  ENG  @0 Stellar kinematics @5 41
C03 16  X  SPA  @0 Cinematica estelar @5 41
C03 17  3  FRE  @0 Corrélation @5 42
C03 17  3  ENG  @0 Correlations @5 42
C03 18  3  FRE  @0 Photométrie @5 43
C03 18  3  ENG  @0 Photometry @5 43
C03 19  3  FRE  @0 Bulbe galaxies @4 CD @5 96
C03 19  3  ENG  @0 Galaxy bulge @4 CD @5 96
C03 19  3  SPA  @0 Bulbo galaxias @4 CD @5 96
C03 20  3  FRE  @0 Evolution galaxies @4 CD @5 97
C03 20  3  ENG  @0 Galaxy evolution @4 CD @5 97
C03 20  3  SPA  @0 Evolución galaxias @4 CD @5 97
C03 21  3  FRE  @0 Structure galaxies @4 CD @5 98
C03 21  3  ENG  @0 Galaxy structure @4 CD @5 98
C03 21  3  SPA  @0 Estructura galaxias @4 CD @5 98
N21       @1 233
N44 01      @1 OTO
N82       @1 OTO

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Pascal:06-0351143

Le document en format XML

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<div type="abstract" xml:lang="en">In this first paper of a series on the structure of boxy and peanut-shaped (B/PS) bulges, Kn-band observations of a sample of 30 edge-on spiral galaxies are described and discussed. Kn-band observations best trace the dominant luminous galactic mass and are minimally affected by dust. Images, unsharp-masked images, as well as major-axis and vertically summed surface brightness profiles are presented and discussed. Galaxies with a B/PS bulge tend to have a more complex morphology than galaxies with other bulge types, more often showing centred or off-centred X structures, secondary maxima along the major-axis and spiral-like structures. While probably not uniquely related to bars, those features are observed in three-dimensional N-body simulations of barred discs and may trace the main bar orbit families. The surface brightness profiles of galaxies with a B/PS bulge are also more complex, typically containing three or more clearly separated regions, including a shallow or flat intermediate region (Freeman Type II profiles). The breaks in the profiles offer evidence for bar-driven transfer of angular momentum and radial redistribution of material. The profiles further suggest a rapid variation of the scaleheight of the disc material, contrary to conventional wisdom but again as expected from the vertical resonances and instabilities present in barred discs. Interestingly, the steep inner region of the surface brightness profiles is often shorter than the isophotally thick part of the galaxies, itself always shorter than the flat intermediate region of the profiles. The steep inner region is also much more prominent along the major-axis than in the vertically summed profiles. Similarly to other recent work but contrary to the standard 'bulge + disc' model (where the bulge is both thick and steep), we thus propose that galaxies with a B/PS bulge are composed of a thin concentrated disc (a disc-like bulge) contained within a partially thick bar (the B/PS bulge), itself contained within a thin outer disc. The inner disc likely formed secularly through bar-driven processes and is responsible for the steep inner region of the surface brightness profiles, traditionally associated with a classic bulge, while the bar is responsible for the flat intermediate region of the surface brightness profiles and the thick complex morphological structures observed. Those components are strongly coupled dynamically and are formed mostly of the same (disc) material, shaped by the weak but relentless action of the bar resonances. Any competing formation scenario for galaxies with a B/PS bulge, which represent at least 45 per cent of the local disc galaxy population, must explain equally well and self-consistently the above morphological and photometric properties, the complex gas and stellar kinematics observed, and the correlations between them.</div>
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<s1>Research School of Astronomy and Astrophysics, The Australian National University, Weston Creek P.O</s1>
<s2>ACT 2611</s2>
<s3>AUS</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA20>
<s1>753-772</s1>
</fA20>
<fA21>
<s1>2006</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>2067</s2>
<s5>354000139014430150</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2006 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>1 p.1/4</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>06-0351143</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Monthly Notices of the Royal Astronomical Society</s0>
</fA64>
<fA66 i1="01">
<s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>In this first paper of a series on the structure of boxy and peanut-shaped (B/PS) bulges, Kn-band observations of a sample of 30 edge-on spiral galaxies are described and discussed. Kn-band observations best trace the dominant luminous galactic mass and are minimally affected by dust. Images, unsharp-masked images, as well as major-axis and vertically summed surface brightness profiles are presented and discussed. Galaxies with a B/PS bulge tend to have a more complex morphology than galaxies with other bulge types, more often showing centred or off-centred X structures, secondary maxima along the major-axis and spiral-like structures. While probably not uniquely related to bars, those features are observed in three-dimensional N-body simulations of barred discs and may trace the main bar orbit families. The surface brightness profiles of galaxies with a B/PS bulge are also more complex, typically containing three or more clearly separated regions, including a shallow or flat intermediate region (Freeman Type II profiles). The breaks in the profiles offer evidence for bar-driven transfer of angular momentum and radial redistribution of material. The profiles further suggest a rapid variation of the scaleheight of the disc material, contrary to conventional wisdom but again as expected from the vertical resonances and instabilities present in barred discs. Interestingly, the steep inner region of the surface brightness profiles is often shorter than the isophotally thick part of the galaxies, itself always shorter than the flat intermediate region of the profiles. The steep inner region is also much more prominent along the major-axis than in the vertically summed profiles. Similarly to other recent work but contrary to the standard 'bulge + disc' model (where the bulge is both thick and steep), we thus propose that galaxies with a B/PS bulge are composed of a thin concentrated disc (a disc-like bulge) contained within a partially thick bar (the B/PS bulge), itself contained within a thin outer disc. The inner disc likely formed secularly through bar-driven processes and is responsible for the steep inner region of the surface brightness profiles, traditionally associated with a classic bulge, while the bar is responsible for the flat intermediate region of the surface brightness profiles and the thick complex morphological structures observed. Those components are strongly coupled dynamically and are formed mostly of the same (disc) material, shaped by the weak but relentless action of the bar resonances. Any competing formation scenario for galaxies with a B/PS bulge, which represent at least 45 per cent of the local disc galaxy population, must explain equally well and self-consistently the above morphological and photometric properties, the complex gas and stellar kinematics observed, and the correlations between them.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Morphologie</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Morphology</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE">
<s0>Brillance surface</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG">
<s0>Surface brightness</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA">
<s0>Brillantez superficie</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Galaxies spirales</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Spiral galaxies</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Structure spirale</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Spiral structure</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Estructura espiral</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Simulation numérique</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Digital simulation</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Système n corps</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>N body system</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Sistema n cuerpos</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Orbite</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Orbits</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Transfert moment cinétique</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Angular momentum transfer</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Variation rapide</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Fast variation</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Variación rápida</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Résonance</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Resonance</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Instabilité</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Instability</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE">
<s0>Modèle</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG">
<s0>Models</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA">
<s0>Modelo</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Couplage fort</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>Strong coupling</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA">
<s0>Acoplamiento fuerte</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Formation galaxies</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Galaxy formation</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE">
<s0>Galaxies disques</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG">
<s0>Disk galaxies</s0>
<s5>40</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE">
<s0>Cinématique stellaire</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG">
<s0>Stellar kinematics</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA">
<s0>Cinematica estelar</s0>
<s5>41</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE">
<s0>Corrélation</s0>
<s5>42</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG">
<s0>Correlations</s0>
<s5>42</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE">
<s0>Photométrie</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG">
<s0>Photometry</s0>
<s5>43</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE">
<s0>Bulbe galaxies</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG">
<s0>Galaxy bulge</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="19" i2="3" l="SPA">
<s0>Bulbo galaxias</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE">
<s0>Evolution galaxies</s0>
<s4>CD</s4>
<s5>97</s5>
</fC03>
<fC03 i1="20" i2="3" l="ENG">
<s0>Galaxy evolution</s0>
<s4>CD</s4>
<s5>97</s5>
</fC03>
<fC03 i1="20" i2="3" l="SPA">
<s0>Evolución galaxias</s0>
<s4>CD</s4>
<s5>97</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE">
<s0>Structure galaxies</s0>
<s4>CD</s4>
<s5>98</s5>
</fC03>
<fC03 i1="21" i2="3" l="ENG">
<s0>Galaxy structure</s0>
<s4>CD</s4>
<s5>98</s5>
</fC03>
<fC03 i1="21" i2="3" l="SPA">
<s0>Estructura galaxias</s0>
<s4>CD</s4>
<s5>98</s5>
</fC03>
<fN21>
<s1>233</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
</inist>
</record>

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