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Properties of Galactic early-type O-supergiants A combined FUV-UV and optical analysis

Identifieur interne : 003581 ( PascalFrancis/Corpus ); précédent : 003580; suivant : 003582

Properties of Galactic early-type O-supergiants A combined FUV-UV and optical analysis

Auteurs : J.-C. Bouret ; D. J. Hillier ; T. Lanz ; A. W. Fullerton

Source :

RBID : Pascal:12-0411601

Descripteurs français

English descriptors

Abstract

Aims. We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from 04 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Methods. Using the non-LTE wind code CMFGEN we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and wind parameters. We derived effective temperatures, luminosities, surface gravities, surface abundances, mass-loss rates, wind terminal velocities, and clumping filling factors. Results. The supergiants define a very clear evolutionary sequence, in terms of ages and masses, from younger and more massive stars to older stars with lower initial masses. O4 supergiants cluster around the 3 Myr isochrone and are more massive than 60 M◦., while the O5 to 07.5 stars have masses in the range 50-40 Mo and are 4 ± 0.3 Myr old. The surface chemical composition is typical of evolved O supergiants (nitrogen-rich, carbon- and oxygen-poor). While the observed ranges of carbon and nitrogen mass-fractions are compatible with those expected from evolutionary models for the measured stellar masses, the N/C ratios as a function of age are inconsistent with the theoretical predictions for the four earliest (O4 spectral type) stars of the sample. We question the efficiency of rotational mixing as a function of age for these stars and suggest that another mechanism may be needed to explain the observed abundance patterns. Mass-loss rates derived with clumped-models range within a factor of three of the theoretical mass-loss rates. The corresponding volume-filling factors associated with small-scale clumping are 0.05 ± 0.02. Clumping is found to start close to the photosphere for all but three stars, two of which are fast rotators.

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Pour connaître la documentation sur le format Inist Standard.

pA  
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A02 01      @0 AAEJAF
A03   1    @0 Astron. astrophys. : (Berl., Print)
A05       @2 544
A06       @3 p. 1
A08 01  1  ENG  @1 Properties of Galactic early-type O-supergiants A combined FUV-UV and optical analysis
A11 01  1    @1 BOURET (J.-C.)
A11 02  1    @1 HILLIER (D. J.)
A11 03  1    @1 LANZ (T.)
A11 04  1    @1 FULLERTON (A. W.)
A14 01      @1 Laboratoire d'Astrophysique de Marseille, Université d'Aix-Marseille & CNRS, UMR7326, 38 rue F. Joliot-Curie @2 13388 Marseille @3 FRA @Z 1 aut.
A14 02      @1 Department of Physics and Astronomy, University of Pittsburgh @2 Pittsburgh, PA 15260 @3 USA @Z 2 aut.
A14 03      @1 Laboratoire J.-L. Lagrange, UMR 7293, Universite de Nice-Sophia Antipolis, CNRS, Observatoire de la Cote d'Azur, BP 4229 @2 06304 Nice @3 FRA @Z 3 aut.
A14 04      @1 Space Telescope Science Institute, 3700 San Martin Drive @2 Baltimore, MD 21218 @3 USA @Z 4 aut.
A20       @2 A67.1-A67.30
A21       @1 2012
A23 01      @0 ENG
A43 01      @1 INIST @2 14176 @5 354000506819240610
A44       @0 0000 @1 © 2012 INIST-CNRS. All rights reserved.
A45       @0 1 p.
A47 01  1    @0 12-0411601
A60       @1 P
A61       @0 A
A64 01  1    @0 Astronomy and astrophysics : (Berlin. Print)
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C01 01    ENG  @0 Aims. We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from 04 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Methods. Using the non-LTE wind code CMFGEN we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and wind parameters. We derived effective temperatures, luminosities, surface gravities, surface abundances, mass-loss rates, wind terminal velocities, and clumping filling factors. Results. The supergiants define a very clear evolutionary sequence, in terms of ages and masses, from younger and more massive stars to older stars with lower initial masses. O4 supergiants cluster around the 3 Myr isochrone and are more massive than 60 M◦., while the O5 to 07.5 stars have masses in the range 50-40 Mo and are 4 ± 0.3 Myr old. The surface chemical composition is typical of evolved O supergiants (nitrogen-rich, carbon- and oxygen-poor). While the observed ranges of carbon and nitrogen mass-fractions are compatible with those expected from evolutionary models for the measured stellar masses, the N/C ratios as a function of age are inconsistent with the theoretical predictions for the four earliest (O4 spectral type) stars of the sample. We question the efficiency of rotational mixing as a function of age for these stars and suggest that another mechanism may be needed to explain the observed abundance patterns. Mass-loss rates derived with clumped-models range within a factor of three of the theoretical mass-loss rates. The corresponding volume-filling factors associated with small-scale clumping are 0.05 ± 0.02. Clumping is found to start close to the photosphere for all but three stars, two of which are fast rotators.
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C03 10  3  ENG  @0 Surface gravity @5 35
C03 11  3  FRE  @0 Abondance @5 36
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C03 12  3  FRE  @0 Facteur remplissage @5 37
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Format Inist (serveur)

NO : PASCAL 12-0411601 INIST
ET : Properties of Galactic early-type O-supergiants A combined FUV-UV and optical analysis
AU : BOURET (J.-C.); HILLIER (D. J.); LANZ (T.); FULLERTON (A. W.)
AF : Laboratoire d'Astrophysique de Marseille, Université d'Aix-Marseille & CNRS, UMR7326, 38 rue F. Joliot-Curie/13388 Marseille/France (1 aut.); Department of Physics and Astronomy, University of Pittsburgh/Pittsburgh, PA 15260/Etats-Unis (2 aut.); Laboratoire J.-L. Lagrange, UMR 7293, Universite de Nice-Sophia Antipolis, CNRS, Observatoire de la Cote d'Azur, BP 4229/06304 Nice/France (3 aut.); Space Telescope Science Institute, 3700 San Martin Drive/Baltimore, MD 21218/Etats-Unis (4 aut.)
DT : Publication en série; Niveau analytique
SO : Astronomy and astrophysics : (Berlin. Print); ISSN 0004-6361; Coden AAEJAF; France; Da. 2012; Vol. 544; No. p. 1; A67.1-A67.30; Bibl. 1 p.
LA : Anglais
EA : Aims. We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from 04 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Methods. Using the non-LTE wind code CMFGEN we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and wind parameters. We derived effective temperatures, luminosities, surface gravities, surface abundances, mass-loss rates, wind terminal velocities, and clumping filling factors. Results. The supergiants define a very clear evolutionary sequence, in terms of ages and masses, from younger and more massive stars to older stars with lower initial masses. O4 supergiants cluster around the 3 Myr isochrone and are more massive than 60 M◦., while the O5 to 07.5 stars have masses in the range 50-40 Mo and are 4 ± 0.3 Myr old. The surface chemical composition is typical of evolved O supergiants (nitrogen-rich, carbon- and oxygen-poor). While the observed ranges of carbon and nitrogen mass-fractions are compatible with those expected from evolutionary models for the measured stellar masses, the N/C ratios as a function of age are inconsistent with the theoretical predictions for the four earliest (O4 spectral type) stars of the sample. We question the efficiency of rotational mixing as a function of age for these stars and suggest that another mechanism may be needed to explain the observed abundance patterns. Mass-loss rates derived with clumped-models range within a factor of three of the theoretical mass-loss rates. The corresponding volume-filling factors associated with small-scale clumping are 0.05 ± 0.02. Clumping is found to start close to the photosphere for all but three stars, two of which are fast rotators.
CC : 001E03
FD : Supergéante; Type spectral; Perte masse; Taux perte; Etoile O; Distribution vent; Ecart équilibre thermodynamique local; Température effective; Luminosité; Gravité surface; Abondance; Facteur remplissage; Age; Etoile massive; Isochrone; Masse stellaire; Composition chimique; Modèle; Mélangeage; Rotateur; Etoile premier type; Vent stellaire; Evolution stellaire
ED : Supergiant stars; Spectral type; Mass loss; Loss rate; O stars; Wind field; Non-LTE; Effective temperature; Luminosity; Surface gravity; Abundance; Fill factor; Age; Massive stars; Isochrone; Stellar mass; Chemical composition; Models; Mixing; Rotator; Early type stars; Stellar winds; Stellar evolution
SD : Tipo espectral; Porcentaje pérdida; Distribución viento; Edad; Isocrono; Modelo; Rotador
LO : INIST-14176.354000506819240610
ID : 12-0411601

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<div type="abstract" xml:lang="en">Aims. We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from 04 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Methods. Using the non-LTE wind code C
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<sub>MFGE</sub>
N we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and wind parameters. We derived effective temperatures, luminosities, surface gravities, surface abundances, mass-loss rates, wind terminal velocities, and clumping filling factors. Results. The supergiants define a very clear evolutionary sequence, in terms of ages and masses, from younger and more massive stars to older stars with lower initial masses. O4 supergiants cluster around the 3 Myr isochrone and are more massive than 60 M
<sub>◦.</sub>
, while the O5 to 07.5 stars have masses in the range 50-40 M
<sub>o</sub>
and are 4 ± 0.3 Myr old. The surface chemical composition is typical of evolved O supergiants (nitrogen-rich, carbon- and oxygen-poor). While the observed ranges of carbon and nitrogen mass-fractions are compatible with those expected from evolutionary models for the measured stellar masses, the N/C ratios as a function of age are inconsistent with the theoretical predictions for the four earliest (O4 spectral type) stars of the sample. We question the efficiency of rotational mixing as a function of age for these stars and suggest that another mechanism may be needed to explain the observed abundance patterns. Mass-loss rates derived with clumped-models range within a factor of three of the theoretical mass-loss rates. The corresponding volume-filling factors associated with small-scale clumping are 0.05 ± 0.02. Clumping is found to start close to the photosphere for all but three stars, two of which are fast rotators.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001E03</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE">
<s0>Supergéante</s0>
<s5>26</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG">
<s0>Supergiant stars</s0>
<s5>26</s5>
</fC03>
<fC03 i1="02" i2="X" l="FRE">
<s0>Type spectral</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="ENG">
<s0>Spectral type</s0>
<s5>27</s5>
</fC03>
<fC03 i1="02" i2="X" l="SPA">
<s0>Tipo espectral</s0>
<s5>27</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Perte masse</s0>
<s5>28</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Mass loss</s0>
<s5>28</s5>
</fC03>
<fC03 i1="04" i2="X" l="FRE">
<s0>Taux perte</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="ENG">
<s0>Loss rate</s0>
<s5>29</s5>
</fC03>
<fC03 i1="04" i2="X" l="SPA">
<s0>Porcentaje pérdida</s0>
<s5>29</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Etoile O</s0>
<s5>30</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>O stars</s0>
<s5>30</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE">
<s0>Distribution vent</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG">
<s0>Wind field</s0>
<s5>31</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA">
<s0>Distribución viento</s0>
<s5>31</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Ecart équilibre thermodynamique local</s0>
<s5>32</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Non-LTE</s0>
<s5>32</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Température effective</s0>
<s5>33</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Effective temperature</s0>
<s5>33</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Luminosité</s0>
<s5>34</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Luminosity</s0>
<s5>34</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Gravité surface</s0>
<s5>35</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Surface gravity</s0>
<s5>35</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Abondance</s0>
<s5>36</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Abundance</s0>
<s5>36</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Facteur remplissage</s0>
<s5>37</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Fill factor</s0>
<s5>37</s5>
</fC03>
<fC03 i1="13" i2="X" l="FRE">
<s0>Age</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="ENG">
<s0>Age</s0>
<s5>38</s5>
</fC03>
<fC03 i1="13" i2="X" l="SPA">
<s0>Edad</s0>
<s5>38</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Etoile massive</s0>
<s5>39</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Massive stars</s0>
<s5>39</s5>
</fC03>
<fC03 i1="15" i2="X" l="FRE">
<s0>Isochrone</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="X" l="ENG">
<s0>Isochrone</s0>
<s5>40</s5>
</fC03>
<fC03 i1="15" i2="X" l="SPA">
<s0>Isocrono</s0>
<s5>40</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE">
<s0>Masse stellaire</s0>
<s5>41</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG">
<s0>Stellar mass</s0>
<s5>41</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE">
<s0>Composition chimique</s0>
<s5>42</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG">
<s0>Chemical composition</s0>
<s5>42</s5>
</fC03>
<fC03 i1="18" i2="X" l="FRE">
<s0>Modèle</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="X" l="ENG">
<s0>Models</s0>
<s5>43</s5>
</fC03>
<fC03 i1="18" i2="X" l="SPA">
<s0>Modelo</s0>
<s5>43</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE">
<s0>Mélangeage</s0>
<s5>44</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG">
<s0>Mixing</s0>
<s5>44</s5>
</fC03>
<fC03 i1="20" i2="X" l="FRE">
<s0>Rotateur</s0>
<s5>45</s5>
</fC03>
<fC03 i1="20" i2="X" l="ENG">
<s0>Rotator</s0>
<s5>45</s5>
</fC03>
<fC03 i1="20" i2="X" l="SPA">
<s0>Rotador</s0>
<s5>45</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE">
<s0>Etoile premier type</s0>
<s5>46</s5>
</fC03>
<fC03 i1="21" i2="3" l="ENG">
<s0>Early type stars</s0>
<s5>46</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE">
<s0>Vent stellaire</s0>
<s5>47</s5>
</fC03>
<fC03 i1="22" i2="3" l="ENG">
<s0>Stellar winds</s0>
<s5>47</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE">
<s0>Evolution stellaire</s0>
<s5>48</s5>
</fC03>
<fC03 i1="23" i2="3" l="ENG">
<s0>Stellar evolution</s0>
<s5>48</s5>
</fC03>
<fN21>
<s1>317</s1>
</fN21>
<fN44 i1="01">
<s1>OTO</s1>
</fN44>
<fN82>
<s1>OTO</s1>
</fN82>
</pA>
</standard>
<server>
<NO>PASCAL 12-0411601 INIST</NO>
<ET>Properties of Galactic early-type O-supergiants A combined FUV-UV and optical analysis</ET>
<AU>BOURET (J.-C.); HILLIER (D. J.); LANZ (T.); FULLERTON (A. W.)</AU>
<AF>Laboratoire d'Astrophysique de Marseille, Université d'Aix-Marseille & CNRS, UMR7326, 38 rue F. Joliot-Curie/13388 Marseille/France (1 aut.); Department of Physics and Astronomy, University of Pittsburgh/Pittsburgh, PA 15260/Etats-Unis (2 aut.); Laboratoire J.-L. Lagrange, UMR 7293, Universite de Nice-Sophia Antipolis, CNRS, Observatoire de la Cote d'Azur, BP 4229/06304 Nice/France (3 aut.); Space Telescope Science Institute, 3700 San Martin Drive/Baltimore, MD 21218/Etats-Unis (4 aut.)</AF>
<DT>Publication en série; Niveau analytique</DT>
<SO>Astronomy and astrophysics : (Berlin. Print); ISSN 0004-6361; Coden AAEJAF; France; Da. 2012; Vol. 544; No. p. 1; A67.1-A67.30; Bibl. 1 p.</SO>
<LA>Anglais</LA>
<EA>Aims. We aim to constrain the properties and evolutionary status of early and mid-spectral type supergiants (from 04 to O7.5). These posses the highest mass-loss rates among the O stars, and exhibit conspicuous wind profiles. Methods. Using the non-LTE wind code C
<sub>MFGE</sub>
N we simultaneously analyzed the FUV-UV and optical spectral range to determine the photospheric properties and wind parameters. We derived effective temperatures, luminosities, surface gravities, surface abundances, mass-loss rates, wind terminal velocities, and clumping filling factors. Results. The supergiants define a very clear evolutionary sequence, in terms of ages and masses, from younger and more massive stars to older stars with lower initial masses. O4 supergiants cluster around the 3 Myr isochrone and are more massive than 60 M
<sub>◦.</sub>
, while the O5 to 07.5 stars have masses in the range 50-40 M
<sub>o</sub>
and are 4 ± 0.3 Myr old. The surface chemical composition is typical of evolved O supergiants (nitrogen-rich, carbon- and oxygen-poor). While the observed ranges of carbon and nitrogen mass-fractions are compatible with those expected from evolutionary models for the measured stellar masses, the N/C ratios as a function of age are inconsistent with the theoretical predictions for the four earliest (O4 spectral type) stars of the sample. We question the efficiency of rotational mixing as a function of age for these stars and suggest that another mechanism may be needed to explain the observed abundance patterns. Mass-loss rates derived with clumped-models range within a factor of three of the theoretical mass-loss rates. The corresponding volume-filling factors associated with small-scale clumping are 0.05 ± 0.02. Clumping is found to start close to the photosphere for all but three stars, two of which are fast rotators.</EA>
<CC>001E03</CC>
<FD>Supergéante; Type spectral; Perte masse; Taux perte; Etoile O; Distribution vent; Ecart équilibre thermodynamique local; Température effective; Luminosité; Gravité surface; Abondance; Facteur remplissage; Age; Etoile massive; Isochrone; Masse stellaire; Composition chimique; Modèle; Mélangeage; Rotateur; Etoile premier type; Vent stellaire; Evolution stellaire</FD>
<ED>Supergiant stars; Spectral type; Mass loss; Loss rate; O stars; Wind field; Non-LTE; Effective temperature; Luminosity; Surface gravity; Abundance; Fill factor; Age; Massive stars; Isochrone; Stellar mass; Chemical composition; Models; Mixing; Rotator; Early type stars; Stellar winds; Stellar evolution</ED>
<SD>Tipo espectral; Porcentaje pérdida; Distribución viento; Edad; Isocrono; Modelo; Rotador</SD>
<LO>INIST-14176.354000506819240610</LO>
<ID>12-0411601</ID>
</server>
</inist>
</record>

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