2012
DOI: 10.1088/0004-637x/761/1/10
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THE EFFECT OF THE14N(p, γ)15O REACTION ON THE BLUE LOOPS IN INTERMEDIATE-MASS STARS

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Cited by 18 publications
(22 citation statements)
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“…The minimum core masses at the first thermal pulse and first TDU are higher in the Z = 0.007 models. Besides the difference in metallicity, the stellar evolutionary code used for the calculations has been updated to use the LUNA rate (Bemmerer et al 2006) of which govern energy generation during core He burning and therefore the size of the core at the beginning of the AGB (e.g., Castellani et al 1992;Imbriani et al 2001;Halabi et al 2012).…”
Section: The Third Dredge-upmentioning
confidence: 99%
“…The minimum core masses at the first thermal pulse and first TDU are higher in the Z = 0.007 models. Besides the difference in metallicity, the stellar evolutionary code used for the calculations has been updated to use the LUNA rate (Bemmerer et al 2006) of which govern energy generation during core He burning and therefore the size of the core at the beginning of the AGB (e.g., Castellani et al 1992;Imbriani et al 2001;Halabi et al 2012).…”
Section: The Third Dredge-upmentioning
confidence: 99%
“…The mean reason behind triggering the blue loop is the enforcement of the SHB. A recent study showing the sensitivity of the loop formation to convective mixing and nuclear reaction is presented by [1]. It is intersecting to note that these blue loops occur in the region of the cepheid instabilities so that available observations may be used for testing the theoretical description of their formation (see [1] for details).…”
Section: The Evolution To the Agb Phasementioning
confidence: 99%
“…A recent study showing the sensitivity of the loop formation to convective mixing and nuclear reaction is presented by [1]. It is intersecting to note that these blue loops occur in the region of the cepheid instabilities so that available observations may be used for testing the theoretical description of their formation (see [1] for details). The core helium burning phase ends after the position 6, and the star evolves back to the RGB, where envelope convection develops again and this is the second dredge up episode which is marked in the right panel in Fig.…”
Section: The Evolution To the Agb Phasementioning
confidence: 99%
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“…We use the mixing scheme described in [13]. The overshooting distance is expressed as l= H p , where H p is the pressure scale height.…”
Section: Effect Of Core Overshootingmentioning
confidence: 99%