Constraints on z ≈ 10 galaxies from the deepest Hubble Space Telescope NICMOS fields

R. J. Bouwens, G. D. Illingworth, Rodger I Thompson, M. Franx

Research output: Contribution to journalArticle

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Abstract

We use all available fields with deep NICMOS imaging to search for J 110-dropouts (H160,AB ≲ 28) at z ≈ 10. Our primary data set for this search is the two J110 + H160 ICMOS fields taken in parallel with the Advanced Camera for Surveys (ACS) Hubble Ultra Deep Field (UDF). The 5 σ limiting magnitudes were ∼28.6 in J 110 and ∼28.5 in H160 (0″.6 apertures). Several shallower fields were also used: J110 + H160 NICMOS frames available over the Hubble Deep Field (HDF) North, the HDF-South NICMOS parallel, and the ACS UDF (with 5 a limiting magnitudes in J110 and H160 ranging from 27.0 to 28.2). The primary selection criterion was (J110-H160)AB > 1-8. Eleven such sources were found in all search fields using this criterion. Eight of these are clearly ruled out as credible z ≈ 10 sources, either as a result of detections (>2 a) blueward of J110 or their colors redward of the break (H160-K ∼ 1.5) (redder than ≳98% of lower redshift dropouts). The nature of the three remaining sources could not be determined from the data. This number appears consistent with the expected contamination from low-redshift interlopers. Analysis of the stacked images for the three candidates also suggests some contamination. Regardless of their true redshifts, the actual number of z ≈ 10 sources must be three or fewer. To assess the significance of these results, two lower redshift samples (a z ∼ 3.8 B-dropout and z ∼ 6 i-dropout sample) were projected to z ∼ 7-13 using a (1 + z) -1 size scaling (for fixed luminosity). They were added to the image frames and the selection was repeated, giving 15.6 and 4.8 J110- dropouts, respectively. This suggests that to the limit of this probe (≈0.3Lz=3*), there has been evolution from z ∼ 3.8 and possibly from z ∼ 6. This is consistent with the strong evolution already noted at z ∼ 6 and z ∼ 7.5 relative to z ∼ 3-4. Even assuming that three sources from this probe are at z ≈ 10, the rest-frame continuum UV (∼1500 ̊) luminosity density at z ∼ 10 (integrated down to 0.3Lz=3*) is just 0.19-0.09+0.13 times that at z ∼ 3.8 (or 0.19-0.10+0.15 times, including the small effect from cosmic variance). However, if none of our sources are at z ≈ 10, this ratio has a 1 σ upper limit of 0.07.

Original languageEnglish (US)
JournalAstrophysical Journal
Volume624
Issue number1 II
DOIs
StatePublished - May 1 2005

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dropouts
Hubble Space Telescope
probe
galaxies
contamination
cameras
luminosity
probes
apertures
continuums
color
scaling
detection
analysis
effect

Keywords

  • Galaxies: evolution
  • Galaxies: high-redshift

ASJC Scopus subject areas

  • Space and Planetary Science

Cite this

Constraints on z ≈ 10 galaxies from the deepest Hubble Space Telescope NICMOS fields. / Bouwens, R. J.; Illingworth, G. D.; Thompson, Rodger I; Franx, M.

In: Astrophysical Journal, Vol. 624, No. 1 II, 01.05.2005.

Research output: Contribution to journalArticle

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abstract = "We use all available fields with deep NICMOS imaging to search for J 110-dropouts (H160,AB ≲ 28) at z ≈ 10. Our primary data set for this search is the two J110 + H160 ICMOS fields taken in parallel with the Advanced Camera for Surveys (ACS) Hubble Ultra Deep Field (UDF). The 5 σ limiting magnitudes were ∼28.6 in J 110 and ∼28.5 in H160 (0″.6 apertures). Several shallower fields were also used: J110 + H160 NICMOS frames available over the Hubble Deep Field (HDF) North, the HDF-South NICMOS parallel, and the ACS UDF (with 5 a limiting magnitudes in J110 and H160 ranging from 27.0 to 28.2). The primary selection criterion was (J110-H160)AB > 1-8. Eleven such sources were found in all search fields using this criterion. Eight of these are clearly ruled out as credible z ≈ 10 sources, either as a result of detections (>2 a) blueward of J110 or their colors redward of the break (H160-K ∼ 1.5) (redder than ≳98{\%} of lower redshift dropouts). The nature of the three remaining sources could not be determined from the data. This number appears consistent with the expected contamination from low-redshift interlopers. Analysis of the stacked images for the three candidates also suggests some contamination. Regardless of their true redshifts, the actual number of z ≈ 10 sources must be three or fewer. To assess the significance of these results, two lower redshift samples (a z ∼ 3.8 B-dropout and z ∼ 6 i-dropout sample) were projected to z ∼ 7-13 using a (1 + z) -1 size scaling (for fixed luminosity). They were added to the image frames and the selection was repeated, giving 15.6 and 4.8 J110- dropouts, respectively. This suggests that to the limit of this probe (≈0.3Lz=3*), there has been evolution from z ∼ 3.8 and possibly from z ∼ 6. This is consistent with the strong evolution already noted at z ∼ 6 and z ∼ 7.5 relative to z ∼ 3-4. Even assuming that three sources from this probe are at z ≈ 10, the rest-frame continuum UV (∼1500 ̊) luminosity density at z ∼ 10 (integrated down to 0.3Lz=3*) is just 0.19-0.09+0.13 times that at z ∼ 3.8 (or 0.19-0.10+0.15 times, including the small effect from cosmic variance). However, if none of our sources are at z ≈ 10, this ratio has a 1 σ upper limit of 0.07.",
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T1 - Constraints on z ≈ 10 galaxies from the deepest Hubble Space Telescope NICMOS fields

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AU - Illingworth, G. D.

AU - Thompson, Rodger I

AU - Franx, M.

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N2 - We use all available fields with deep NICMOS imaging to search for J 110-dropouts (H160,AB ≲ 28) at z ≈ 10. Our primary data set for this search is the two J110 + H160 ICMOS fields taken in parallel with the Advanced Camera for Surveys (ACS) Hubble Ultra Deep Field (UDF). The 5 σ limiting magnitudes were ∼28.6 in J 110 and ∼28.5 in H160 (0″.6 apertures). Several shallower fields were also used: J110 + H160 NICMOS frames available over the Hubble Deep Field (HDF) North, the HDF-South NICMOS parallel, and the ACS UDF (with 5 a limiting magnitudes in J110 and H160 ranging from 27.0 to 28.2). The primary selection criterion was (J110-H160)AB > 1-8. Eleven such sources were found in all search fields using this criterion. Eight of these are clearly ruled out as credible z ≈ 10 sources, either as a result of detections (>2 a) blueward of J110 or their colors redward of the break (H160-K ∼ 1.5) (redder than ≳98% of lower redshift dropouts). The nature of the three remaining sources could not be determined from the data. This number appears consistent with the expected contamination from low-redshift interlopers. Analysis of the stacked images for the three candidates also suggests some contamination. Regardless of their true redshifts, the actual number of z ≈ 10 sources must be three or fewer. To assess the significance of these results, two lower redshift samples (a z ∼ 3.8 B-dropout and z ∼ 6 i-dropout sample) were projected to z ∼ 7-13 using a (1 + z) -1 size scaling (for fixed luminosity). They were added to the image frames and the selection was repeated, giving 15.6 and 4.8 J110- dropouts, respectively. This suggests that to the limit of this probe (≈0.3Lz=3*), there has been evolution from z ∼ 3.8 and possibly from z ∼ 6. This is consistent with the strong evolution already noted at z ∼ 6 and z ∼ 7.5 relative to z ∼ 3-4. Even assuming that three sources from this probe are at z ≈ 10, the rest-frame continuum UV (∼1500 ̊) luminosity density at z ∼ 10 (integrated down to 0.3Lz=3*) is just 0.19-0.09+0.13 times that at z ∼ 3.8 (or 0.19-0.10+0.15 times, including the small effect from cosmic variance). However, if none of our sources are at z ≈ 10, this ratio has a 1 σ upper limit of 0.07.

AB - We use all available fields with deep NICMOS imaging to search for J 110-dropouts (H160,AB ≲ 28) at z ≈ 10. Our primary data set for this search is the two J110 + H160 ICMOS fields taken in parallel with the Advanced Camera for Surveys (ACS) Hubble Ultra Deep Field (UDF). The 5 σ limiting magnitudes were ∼28.6 in J 110 and ∼28.5 in H160 (0″.6 apertures). Several shallower fields were also used: J110 + H160 NICMOS frames available over the Hubble Deep Field (HDF) North, the HDF-South NICMOS parallel, and the ACS UDF (with 5 a limiting magnitudes in J110 and H160 ranging from 27.0 to 28.2). The primary selection criterion was (J110-H160)AB > 1-8. Eleven such sources were found in all search fields using this criterion. Eight of these are clearly ruled out as credible z ≈ 10 sources, either as a result of detections (>2 a) blueward of J110 or their colors redward of the break (H160-K ∼ 1.5) (redder than ≳98% of lower redshift dropouts). The nature of the three remaining sources could not be determined from the data. This number appears consistent with the expected contamination from low-redshift interlopers. Analysis of the stacked images for the three candidates also suggests some contamination. Regardless of their true redshifts, the actual number of z ≈ 10 sources must be three or fewer. To assess the significance of these results, two lower redshift samples (a z ∼ 3.8 B-dropout and z ∼ 6 i-dropout sample) were projected to z ∼ 7-13 using a (1 + z) -1 size scaling (for fixed luminosity). They were added to the image frames and the selection was repeated, giving 15.6 and 4.8 J110- dropouts, respectively. This suggests that to the limit of this probe (≈0.3Lz=3*), there has been evolution from z ∼ 3.8 and possibly from z ∼ 6. This is consistent with the strong evolution already noted at z ∼ 6 and z ∼ 7.5 relative to z ∼ 3-4. Even assuming that three sources from this probe are at z ≈ 10, the rest-frame continuum UV (∼1500 ̊) luminosity density at z ∼ 10 (integrated down to 0.3Lz=3*) is just 0.19-0.09+0.13 times that at z ∼ 3.8 (or 0.19-0.10+0.15 times, including the small effect from cosmic variance). However, if none of our sources are at z ≈ 10, this ratio has a 1 σ upper limit of 0.07.

KW - Galaxies: evolution

KW - Galaxies: high-redshift

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