adsabs.harvard.edu/abs/1998ApJ...500..188I

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https://adsabs.harvard.edu/abs/1998ApJ...500..188I

The Primordial Abundance of <SUP>4</SUP>He Revisited

We use a sample of 45 low-metallicity H II regions to determine the primordial helium abundance Y<SUB>p</SUB> with a precision of better than 1%. The data includes new spectrophotometric observations of 15 blue compact galaxies (BCGs) with oxygen abundance 12 + log (O/H) between 7.83 and 8.35 (Z<SUB>⊙</SUB>/13 &lt;= Z &lt;= Z<SUB>⊙</SUB>/4), most of which were selected from the First Byurakan and the University of Michigan objective prism surveys. We have included many low-metallicity BCGs in our sample, including the two most metal-deficient galaxies known, I Zw 18 (Z<SUB>⊙</SUB>/55) and SBS 0335-052 (Z<SUB>⊙</SUB>/43). We have carefully investigated the physical effects that may make the He I line intensities deviate from their recombination values, such as collisional and fluorescent enhancements, underlying He I stellar absorption, and absorption by Galactic interstellar Na I. By extrapolating the Y versus O/H and Y versus N/H linear regressions to O/H = N/H = 0, we obtain Y<SUB>p</SUB> = 0.244 +/- 0.002 and 0.245 +/- 0.001, respectively, in agreement with the study of Izotov, Thuan, &amp; Lipovetsky, but higher than previous determinations (Y<SUB>p</SUB> = 0.230-0.234). Part of the difference comes from the fact that previous investigators have used the northwest component of I Zw 18 in the determination of Y<SUB>p</SUB>. This component is subject to strong underlying He I stellar absorption that reduces the He I line intensities by 5%-25%. The derived Y is 0.233 +/- 0.008 from the He I λ6678 line. Instead, by using the southeast component of I Zw 18, which is much less subject to underlying He I stellar absorption, we obtain Y = 0.242 +/- 0.009. The mean Y of the two most metal-deficient BCGs, I Zw 18 and SBS 0335-052, is Ȳ=0.245+/-0.004, in excellent agreement with the Y<SUB>p</SUB> derived from the linear regressions. We derive a slope dY/dZ = 2.3 +/- 1.0, considerably smaller than those derived before. With this smaller slope and taking into account the errors, chemical evolution models with an outflow of well-mixed material can be built for star-forming dwarf galaxies that satisfy all the observational constraints. Our Y<SUB>p</SUB> gives Ω<SUB>b</SUB>h<SUP>2</SUP><SUB>50</SUB>=0.058+/-0.007, consistent with the lower limit set by dynamical measurements and X-ray observations of clusters of galaxies. It is also consistent, within the framework of standard big bang nucleosynthesis theory, with measurements of primordial <SUP>7</SUP>Li in galactic halo stars, and at the 1 σ level with the D/H abundance measured in absorption systems toward quasars by Tytler &amp; Burles.



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The Primordial Abundance of <SUP>4</SUP>He Revisited

https://adsabs.harvard.edu/abs/1998ApJ...500..188I

We use a sample of 45 low-metallicity H II regions to determine the primordial helium abundance Y<SUB>p</SUB> with a precision of better than 1%. The data includes new spectrophotometric observations of 15 blue compact galaxies (BCGs) with oxygen abundance 12 + log (O/H) between 7.83 and 8.35 (Z<SUB>⊙</SUB>/13 &lt;= Z &lt;= Z<SUB>⊙</SUB>/4), most of which were selected from the First Byurakan and the University of Michigan objective prism surveys. We have included many low-metallicity BCGs in our sample, including the two most metal-deficient galaxies known, I Zw 18 (Z<SUB>⊙</SUB>/55) and SBS 0335-052 (Z<SUB>⊙</SUB>/43). We have carefully investigated the physical effects that may make the He I line intensities deviate from their recombination values, such as collisional and fluorescent enhancements, underlying He I stellar absorption, and absorption by Galactic interstellar Na I. By extrapolating the Y versus O/H and Y versus N/H linear regressions to O/H = N/H = 0, we obtain Y<SUB>p</SUB> = 0.244 +/- 0.002 and 0.245 +/- 0.001, respectively, in agreement with the study of Izotov, Thuan, &amp; Lipovetsky, but higher than previous determinations (Y<SUB>p</SUB> = 0.230-0.234). Part of the difference comes from the fact that previous investigators have used the northwest component of I Zw 18 in the determination of Y<SUB>p</SUB>. This component is subject to strong underlying He I stellar absorption that reduces the He I line intensities by 5%-25%. The derived Y is 0.233 +/- 0.008 from the He I λ6678 line. Instead, by using the southeast component of I Zw 18, which is much less subject to underlying He I stellar absorption, we obtain Y = 0.242 +/- 0.009. The mean Y of the two most metal-deficient BCGs, I Zw 18 and SBS 0335-052, is Ȳ=0.245+/-0.004, in excellent agreement with the Y<SUB>p</SUB> derived from the linear regressions. We derive a slope dY/dZ = 2.3 +/- 1.0, considerably smaller than those derived before. With this smaller slope and taking into account the errors, chemical evolution models with an outflow of well-mixed material can be built for star-forming dwarf galaxies that satisfy all the observational constraints. Our Y<SUB>p</SUB> gives Ω<SUB>b</SUB>h<SUP>2</SUP><SUB>50</SUB>=0.058+/-0.007, consistent with the lower limit set by dynamical measurements and X-ray observations of clusters of galaxies. It is also consistent, within the framework of standard big bang nucleosynthesis theory, with measurements of primordial <SUP>7</SUP>Li in galactic halo stars, and at the 1 σ level with the D/H abundance measured in absorption systems toward quasars by Tytler &amp; Burles.



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https://adsabs.harvard.edu/abs/1998ApJ...500..188I

The Primordial Abundance of <SUP>4</SUP>He Revisited

We use a sample of 45 low-metallicity H II regions to determine the primordial helium abundance Y<SUB>p</SUB> with a precision of better than 1%. The data includes new spectrophotometric observations of 15 blue compact galaxies (BCGs) with oxygen abundance 12 + log (O/H) between 7.83 and 8.35 (Z<SUB>⊙</SUB>/13 &lt;= Z &lt;= Z<SUB>⊙</SUB>/4), most of which were selected from the First Byurakan and the University of Michigan objective prism surveys. We have included many low-metallicity BCGs in our sample, including the two most metal-deficient galaxies known, I Zw 18 (Z<SUB>⊙</SUB>/55) and SBS 0335-052 (Z<SUB>⊙</SUB>/43). We have carefully investigated the physical effects that may make the He I line intensities deviate from their recombination values, such as collisional and fluorescent enhancements, underlying He I stellar absorption, and absorption by Galactic interstellar Na I. By extrapolating the Y versus O/H and Y versus N/H linear regressions to O/H = N/H = 0, we obtain Y<SUB>p</SUB> = 0.244 +/- 0.002 and 0.245 +/- 0.001, respectively, in agreement with the study of Izotov, Thuan, &amp; Lipovetsky, but higher than previous determinations (Y<SUB>p</SUB> = 0.230-0.234). Part of the difference comes from the fact that previous investigators have used the northwest component of I Zw 18 in the determination of Y<SUB>p</SUB>. This component is subject to strong underlying He I stellar absorption that reduces the He I line intensities by 5%-25%. The derived Y is 0.233 +/- 0.008 from the He I λ6678 line. Instead, by using the southeast component of I Zw 18, which is much less subject to underlying He I stellar absorption, we obtain Y = 0.242 +/- 0.009. The mean Y of the two most metal-deficient BCGs, I Zw 18 and SBS 0335-052, is Ȳ=0.245+/-0.004, in excellent agreement with the Y<SUB>p</SUB> derived from the linear regressions. We derive a slope dY/dZ = 2.3 +/- 1.0, considerably smaller than those derived before. With this smaller slope and taking into account the errors, chemical evolution models with an outflow of well-mixed material can be built for star-forming dwarf galaxies that satisfy all the observational constraints. Our Y<SUB>p</SUB> gives Ω<SUB>b</SUB>h<SUP>2</SUP><SUB>50</SUB>=0.058+/-0.007, consistent with the lower limit set by dynamical measurements and X-ray observations of clusters of galaxies. It is also consistent, within the framework of standard big bang nucleosynthesis theory, with measurements of primordial <SUP>7</SUP>Li in galactic halo stars, and at the 1 σ level with the D/H abundance measured in absorption systems toward quasars by Tytler &amp; Burles.

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      The Primordial Abundance of <SUP>4</SUP>He Revisited
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      We use a sample of 45 low-metallicity H II regions to determine the primordial helium abundance Y<SUB>p</SUB> with a precision of better than 1%. The data includes new spectrophotometric observations of 15 blue compact galaxies (BCGs) with oxygen abundance 12 + log (O/H) between 7.83 and 8.35 (Z<SUB>⊙</SUB>/13 &lt;= Z &lt;= Z<SUB>⊙</SUB>/4), most of which were selected from the First Byurakan and the University of Michigan objective prism surveys. We have included many low-metallicity BCGs in our sample, including the two most metal-deficient galaxies known, I Zw 18 (Z<SUB>⊙</SUB>/55) and SBS 0335-052 (Z<SUB>⊙</SUB>/43). We have carefully investigated the physical effects that may make the He I line intensities deviate from their recombination values, such as collisional and fluorescent enhancements, underlying He I stellar absorption, and absorption by Galactic interstellar Na I. By extrapolating the Y versus O/H and Y versus N/H linear regressions to O/H = N/H = 0, we obtain Y<SUB>p</SUB> = 0.244 +/- 0.002 and 0.245 +/- 0.001, respectively, in agreement with the study of Izotov, Thuan, &amp; Lipovetsky, but higher than previous determinations (Y<SUB>p</SUB> = 0.230-0.234). Part of the difference comes from the fact that previous investigators have used the northwest component of I Zw 18 in the determination of Y<SUB>p</SUB>. This component is subject to strong underlying He I stellar absorption that reduces the He I line intensities by 5%-25%. The derived Y is 0.233 +/- 0.008 from the He I λ6678 line. Instead, by using the southeast component of I Zw 18, which is much less subject to underlying He I stellar absorption, we obtain Y = 0.242 +/- 0.009. The mean Y of the two most metal-deficient BCGs, I Zw 18 and SBS 0335-052, is Ȳ=0.245+/-0.004, in excellent agreement with the Y<SUB>p</SUB> derived from the linear regressions. We derive a slope dY/dZ = 2.3 +/- 1.0, considerably smaller than those derived before. With this smaller slope and taking into account the errors, chemical evolution models with an outflow of well-mixed material can be built for star-forming dwarf galaxies that satisfy all the observational constraints. Our Y<SUB>p</SUB> gives Ω<SUB>b</SUB>h<SUP>2</SUP><SUB>50</SUB>=0.058+/-0.007, consistent with the lower limit set by dynamical measurements and X-ray observations of clusters of galaxies. It is also consistent, within the framework of standard big bang nucleosynthesis theory, with measurements of primordial <SUP>7</SUP>Li in galactic halo stars, and at the 1 σ level with the D/H abundance measured in absorption systems toward quasars by Tytler &amp; Burles.
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      We use a sample of 45 low-metallicity H II regions to determine the primordial helium abundance Y<SUB>p</SUB> with a precision of better than 1%. The data includes new spectrophotometric observations of 15 blue compact galaxies (BCGs) with oxygen abundance 12 + log (O/H) between 7.83 and 8.35 (Z<SUB>⊙</SUB>/13 &lt;= Z &lt;= Z<SUB>⊙</SUB>/4), most of which were selected from the First Byurakan and the University of Michigan objective prism surveys. We have included many low-metallicity BCGs in our sample, including the two most metal-deficient galaxies known, I Zw 18 (Z<SUB>⊙</SUB>/55) and SBS 0335-052 (Z<SUB>⊙</SUB>/43). We have carefully investigated the physical effects that may make the He I line intensities deviate from their recombination values, such as collisional and fluorescent enhancements, underlying He I stellar absorption, and absorption by Galactic interstellar Na I. By extrapolating the Y versus O/H and Y versus N/H linear regressions to O/H = N/H = 0, we obtain Y<SUB>p</SUB> = 0.244 +/- 0.002 and 0.245 +/- 0.001, respectively, in agreement with the study of Izotov, Thuan, &amp; Lipovetsky, but higher than previous determinations (Y<SUB>p</SUB> = 0.230-0.234). Part of the difference comes from the fact that previous investigators have used the northwest component of I Zw 18 in the determination of Y<SUB>p</SUB>. This component is subject to strong underlying He I stellar absorption that reduces the He I line intensities by 5%-25%. The derived Y is 0.233 +/- 0.008 from the He I λ6678 line. Instead, by using the southeast component of I Zw 18, which is much less subject to underlying He I stellar absorption, we obtain Y = 0.242 +/- 0.009. The mean Y of the two most metal-deficient BCGs, I Zw 18 and SBS 0335-052, is Ȳ=0.245+/-0.004, in excellent agreement with the Y<SUB>p</SUB> derived from the linear regressions. We derive a slope dY/dZ = 2.3 +/- 1.0, considerably smaller than those derived before. With this smaller slope and taking into account the errors, chemical evolution models with an outflow of well-mixed material can be built for star-forming dwarf galaxies that satisfy all the observational constraints. Our Y<SUB>p</SUB> gives Ω<SUB>b</SUB>h<SUP>2</SUP><SUB>50</SUB>=0.058+/-0.007, consistent with the lower limit set by dynamical measurements and X-ray observations of clusters of galaxies. It is also consistent, within the framework of standard big bang nucleosynthesis theory, with measurements of primordial <SUP>7</SUP>Li in galactic halo stars, and at the 1 σ level with the D/H abundance measured in absorption systems toward quasars by Tytler &amp; Burles.
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