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Eight new T4.5–T7.5 dwarfs discovered in the UKIDSS Large Area Survey Data Release 1

Identifieur interne : 002067 ( Istex/Corpus ); précédent : 002066; suivant : 002068

Eight new T4.5–T7.5 dwarfs discovered in the UKIDSS Large Area Survey Data Release 1

Auteurs : N. Lodieu ; D. J. Pinfield ; S. K. Leggett ; R. F. Jameson ; D. J. Mortlock ; S. J. Warren ; B. Burningham ; P. W. Lucas ; K. Chiu ; M. C. Liu ; B. P. Venemans ; R. G. Mcmahon ; F. Allard ; I. Baraffe ; D. Barrado Y Navascués ; G. Carraro ; S. L. Casewell ; G. Chabrier ; R. J. Chappelle ; F. Clarke ; A. C. Day-Jones ; N. R. Deacon ; P. D. Dobbie ; S. L. Folkes ; N. C. Hambly ; P. C. Hewett ; S. T. Hodgkin ; H. R. A. Jones ; T. R. Kendall ; A. Magazzù ; E. L. Martín ; M. J. Mccaughrean ; T. Nakajima ; Y. Pavlenko ; M. Tamura ; C. G. Tinney ; M. R. Zapatero Osorio

Source :

RBID : ISTEX:AC16091DC4DD5A93B1138A2DE94DFE720827D8F4

Abstract

We present eight new T4.5–T7.5 dwarfs identified in the UKIRT (United Kingdom Infrared Telescope) Infrared Deep Sky Survey (UKIDSS) Large Area Survey (LAS) Data Release 1 (DR1). In addition we have recovered the T4.5 dwarf SDSS J020742.91+000056.2 and the T8.5 dwarf ULAS J003402.77−005206.7. Photometric candidates were picked up in two-colour diagrams over 190 deg2 (DR1) and selected in at least two filters. All candidates exhibit near-infrared spectra with strong methane and water absorption bands characteristic of T dwarfs and the derived spectral types follow the unified scheme of Burgasser et al.. We have found six new T4.5–T5.5 dwarfs, one T7 dwarf, one T7.5 dwarf and recovered a T4.5 dwarf and a T8.5 dwarf. We provide distance estimates which lie in the 15–85 pc range; the T7.5 and T8.5 dwarfs are probably within 25 pc of the Sun. We conclude with a discussion of the number of T dwarfs expected after completion of the LAS, comparing these initial results to theoretical simulations.

Url:
DOI: 10.1111/j.1365-2966.2007.12023.x

Links to Exploration step

ISTEX:AC16091DC4DD5A93B1138A2DE94DFE720827D8F4

Le document en format XML

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<mods:affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</mods:affiliation>
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<name sortKey="Burningham, B" sort="Burningham, B" uniqKey="Burningham B" first="B." last="Burningham">B. Burningham</name>
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<name sortKey="Lucas, P W" sort="Lucas, P W" uniqKey="Lucas P" first="P. W." last="Lucas">P. W. Lucas</name>
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<name sortKey="Chiu, K" sort="Chiu, K" uniqKey="Chiu K" first="K." last="Chiu">K. Chiu</name>
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<name sortKey="Liu, M C" sort="Liu, M C" uniqKey="Liu M" first="M. C." last="Liu">M. C. Liu</name>
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<mods:affiliation>‡Alfred P. Sloan Research Fellow.</mods:affiliation>
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<name sortKey="Venemans, B P" sort="Venemans, B P" uniqKey="Venemans B" first="B. P." last="Venemans">B. P. Venemans</name>
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<name sortKey="Mcmahon, R G" sort="Mcmahon, R G" uniqKey="Mcmahon R" first="R. G." last="Mcmahon">R. G. Mcmahon</name>
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<name sortKey="Allard, F" sort="Allard, F" uniqKey="Allard F" first="F." last="Allard">F. Allard</name>
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<name sortKey="Baraffe, I" sort="Baraffe, I" uniqKey="Baraffe I" first="I." last="Baraffe">I. Baraffe</name>
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<name sortKey="Y Navascues, D Barrado" sort="Y Navascues, D Barrado" uniqKey="Y Navascues D" first="D. Barrado" last="Y Navascués">D. Barrado Y Navascués</name>
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<name sortKey="Carraro, G" sort="Carraro, G" uniqKey="Carraro G" first="G." last="Carraro">G. Carraro</name>
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<name sortKey="Casewell, S L" sort="Casewell, S L" uniqKey="Casewell S" first="S. L." last="Casewell">S. L. Casewell</name>
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<name sortKey="Chabrier, G" sort="Chabrier, G" uniqKey="Chabrier G" first="G." last="Chabrier">G. Chabrier</name>
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<name sortKey="Chappelle, R J" sort="Chappelle, R J" uniqKey="Chappelle R" first="R. J." last="Chappelle">R. J. Chappelle</name>
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<name sortKey="Clarke, F" sort="Clarke, F" uniqKey="Clarke F" first="F." last="Clarke">F. Clarke</name>
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<mods:affiliation>Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU</mods:affiliation>
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<name sortKey="Day Jones, A C" sort="Day Jones, A C" uniqKey="Day Jones A" first="A. C." last="Day-Jones">A. C. Day-Jones</name>
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<name sortKey="Deacon, N R" sort="Deacon, N R" uniqKey="Deacon N" first="N. R." last="Deacon">N. R. Deacon</name>
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<mods:affiliation>Department of Astrophysics, Radboud University Nijmegen, PO Box 9010, 6500 GL Nijmegen, the Netherlands</mods:affiliation>
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<name sortKey="Dobbie, P D" sort="Dobbie, P D" uniqKey="Dobbie P" first="P. D." last="Dobbie">P. D. Dobbie</name>
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<mods:affiliation>Anglo-Australian Observatory, PO Box 296, Epping 1710, Australia</mods:affiliation>
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<name sortKey="Hambly, N C" sort="Hambly, N C" uniqKey="Hambly N" first="N. C." last="Hambly">N. C. Hambly</name>
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<name sortKey="Hewett, P C" sort="Hewett, P C" uniqKey="Hewett P" first="P. C." last="Hewett">P. C. Hewett</name>
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<name sortKey="Hodgkin, S T" sort="Hodgkin, S T" uniqKey="Hodgkin S" first="S. T." last="Hodgkin">S. T. Hodgkin</name>
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<mods:affiliation>Institute of Astronomy, Madingley Road, Cambridge CB3 0HA</mods:affiliation>
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<name sortKey="Jones, H R A" sort="Jones, H R A" uniqKey="Jones H" first="H. R. A." last="Jones">H. R. A. Jones</name>
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<mods:affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</mods:affiliation>
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<name sortKey="Kendall, T R" sort="Kendall, T R" uniqKey="Kendall T" first="T. R." last="Kendall">T. R. Kendall</name>
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<mods:affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</mods:affiliation>
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<name sortKey="Magazzu, A" sort="Magazzu, A" uniqKey="Magazzu A" first="A." last="Magazzù">A. Magazzù</name>
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<mods:affiliation>Fundación Galileo Galilei-INAF, Apartado 565, E-38700 Santa Cruz de La Palma, Spain</mods:affiliation>
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<name sortKey="Martin, E L" sort="Martin, E L" uniqKey="Martin E" first="E. L." last="Martín">E. L. Martín</name>
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<name sortKey="Mccaughrean, M J" sort="Mccaughrean, M J" uniqKey="Mccaughrean M" first="M. J." last="Mccaughrean">M. J. Mccaughrean</name>
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<mods:affiliation>School of Physics, University of Exeter, Stocker Road, Exeter, Devon EX4 4QL</mods:affiliation>
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<name sortKey="Nakajima, T" sort="Nakajima, T" uniqKey="Nakajima T" first="T." last="Nakajima">T. Nakajima</name>
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<mods:affiliation>National Astronomical Observatory, Mitaka, Tokyo 181-8588, Japan</mods:affiliation>
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<name sortKey="Pavlenko, Y" sort="Pavlenko, Y" uniqKey="Pavlenko Y" first="Y." last="Pavlenko">Y. Pavlenko</name>
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<mods:affiliation>Main Astronomical Observatory, National Academy of Sciences, Zabolotnoho 27, Kyiv-127 03680, Ukraine</mods:affiliation>
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<name sortKey="Tamura, M" sort="Tamura, M" uniqKey="Tamura M" first="M." last="Tamura">M. Tamura</name>
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<mods:affiliation>National Astronomical Observatory, Mitaka, Tokyo 181-8588, Japan</mods:affiliation>
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<name sortKey="Tinney, C G" sort="Tinney, C G" uniqKey="Tinney C" first="C. G." last="Tinney">C. G. Tinney</name>
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<mods:affiliation>Anglo-Australian Observatory, PO Box 296, Epping 1710, Australia</mods:affiliation>
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<name sortKey="Zapatero Osorio, M R" sort="Zapatero Osorio, M R" uniqKey="Zapatero Osorio M" first="M. R." last="Zapatero Osorio">M. R. Zapatero Osorio</name>
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<title level="a">Eight new T4.5–T7.5 dwarfs discovered in the UKIDSS Large Area Survey Data Release 1</title>
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<name sortKey="Lodieu, N" sort="Lodieu, N" uniqKey="Lodieu N" first="N." last="Lodieu">N. Lodieu</name>
<affiliation>
<mods:affiliation>Instituto de Astrofísica de Canarias, Vía Láctea s/n, E-38205 La Laguna, Tenerife, Spain</mods:affiliation>
</affiliation>
<affiliation>
<mods:affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</mods:affiliation>
</affiliation>
<affiliation>
<mods:affiliation>E-mail: nlodieu@iac.es</mods:affiliation>
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<mods:affiliation></mods:affiliation>
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<mods:affiliation>E-mail: nlodieu@iac.es</mods:affiliation>
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<name sortKey="Pinfield, D J" sort="Pinfield, D J" uniqKey="Pinfield D" first="D. J." last="Pinfield">D. J. Pinfield</name>
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<mods:affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</mods:affiliation>
</affiliation>
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<name sortKey="Leggett, S K" sort="Leggett, S K" uniqKey="Leggett S" first="S. K." last="Leggett">S. K. Leggett</name>
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<mods:affiliation>Gemini Observatory, 670 N. A'ohoku Place, Hilo, HI 96720, USA</mods:affiliation>
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<name sortKey="Jameson, R F" sort="Jameson, R F" uniqKey="Jameson R" first="R. F." last="Jameson">R. F. Jameson</name>
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<mods:affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</mods:affiliation>
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<name sortKey="Mortlock, D J" sort="Mortlock, D J" uniqKey="Mortlock D" first="D. J." last="Mortlock">D. J. Mortlock</name>
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<mods:affiliation>Astrophysics Group, Imperial College London, Blackett Laboratory, Prince Consort Road, London SW7 2AZ</mods:affiliation>
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<name sortKey="Warren, S J" sort="Warren, S J" uniqKey="Warren S" first="S. J." last="Warren">S. J. Warren</name>
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<mods:affiliation>Astrophysics Group, Imperial College London, Blackett Laboratory, Prince Consort Road, London SW7 2AZ</mods:affiliation>
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<name sortKey="Burningham, B" sort="Burningham, B" uniqKey="Burningham B" first="B." last="Burningham">B. Burningham</name>
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<mods:affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</mods:affiliation>
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<name sortKey="Lucas, P W" sort="Lucas, P W" uniqKey="Lucas P" first="P. W." last="Lucas">P. W. Lucas</name>
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<name sortKey="Chiu, K" sort="Chiu, K" uniqKey="Chiu K" first="K." last="Chiu">K. Chiu</name>
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<mods:affiliation>School of Physics, University of Exeter, Stocker Road, Exeter, Devon EX4 4QL</mods:affiliation>
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<name sortKey="Liu, M C" sort="Liu, M C" uniqKey="Liu M" first="M. C." last="Liu">M. C. Liu</name>
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<mods:affiliation>Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, USA</mods:affiliation>
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<mods:affiliation>‡Alfred P. Sloan Research Fellow.</mods:affiliation>
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<name sortKey="Venemans, B P" sort="Venemans, B P" uniqKey="Venemans B" first="B. P." last="Venemans">B. P. Venemans</name>
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<mods:affiliation>Institute of Astronomy, Madingley Road, Cambridge CB3 0HA</mods:affiliation>
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<name sortKey="Mcmahon, R G" sort="Mcmahon, R G" uniqKey="Mcmahon R" first="R. G." last="Mcmahon">R. G. Mcmahon</name>
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<name sortKey="Allard, F" sort="Allard, F" uniqKey="Allard F" first="F." last="Allard">F. Allard</name>
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<mods:affiliation>CRAL, Ecole Normale Supérieure de Lyon, 46 Allée d'Italie, Université de Lyon, F-69364 Lyon Cédex 7, France</mods:affiliation>
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<name sortKey="Baraffe, I" sort="Baraffe, I" uniqKey="Baraffe I" first="I." last="Baraffe">I. Baraffe</name>
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<mods:affiliation>CRAL, Ecole Normale Supérieure de Lyon, 46 Allée d'Italie, Université de Lyon, F-69364 Lyon Cédex 7, France</mods:affiliation>
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<name sortKey="Y Navascues, D Barrado" sort="Y Navascues, D Barrado" uniqKey="Y Navascues D" first="D. Barrado" last="Y Navascués">D. Barrado Y Navascués</name>
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<mods:affiliation>Laboratorio de Astrofísica Espacial y Física Fundamental, INTA, PO Box 50727, E-2808 Madrid, Spain</mods:affiliation>
</affiliation>
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<name sortKey="Carraro, G" sort="Carraro, G" uniqKey="Carraro G" first="G." last="Carraro">G. Carraro</name>
<affiliation>
<mods:affiliation>Departamento de Astronomia, Universidad de Chile, Casilla 36-D, Santiago, Chile</mods:affiliation>
</affiliation>
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<author>
<name sortKey="Casewell, S L" sort="Casewell, S L" uniqKey="Casewell S" first="S. L." last="Casewell">S. L. Casewell</name>
<affiliation>
<mods:affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</mods:affiliation>
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<name sortKey="Chabrier, G" sort="Chabrier, G" uniqKey="Chabrier G" first="G." last="Chabrier">G. Chabrier</name>
<affiliation>
<mods:affiliation>Institute of Astronomy, Madingley Road, Cambridge CB3 0HA</mods:affiliation>
</affiliation>
</author>
<author>
<name sortKey="Chappelle, R J" sort="Chappelle, R J" uniqKey="Chappelle R" first="R. J." last="Chappelle">R. J. Chappelle</name>
<affiliation>
<mods:affiliation>Astronomical Institute, Academy of Sciences of the Czech Republic, Bocni II/1401a, 141 31 Prague, Czech Republic</mods:affiliation>
</affiliation>
</author>
<author>
<name sortKey="Clarke, F" sort="Clarke, F" uniqKey="Clarke F" first="F." last="Clarke">F. Clarke</name>
<affiliation>
<mods:affiliation>Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU</mods:affiliation>
</affiliation>
</author>
<author>
<name sortKey="Day Jones, A C" sort="Day Jones, A C" uniqKey="Day Jones A" first="A. C." last="Day-Jones">A. C. Day-Jones</name>
<affiliation>
<mods:affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</mods:affiliation>
</affiliation>
</author>
<author>
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<div type="abstract">We present eight new T4.5–T7.5 dwarfs identified in the UKIRT (United Kingdom Infrared Telescope) Infrared Deep Sky Survey (UKIDSS) Large Area Survey (LAS) Data Release 1 (DR1). In addition we have recovered the T4.5 dwarf SDSS J020742.91+000056.2 and the T8.5 dwarf ULAS J003402.77−005206.7. Photometric candidates were picked up in two-colour diagrams over 190 deg2 (DR1) and selected in at least two filters. All candidates exhibit near-infrared spectra with strong methane and water absorption bands characteristic of T dwarfs and the derived spectral types follow the unified scheme of Burgasser et al.. We have found six new T4.5–T5.5 dwarfs, one T7 dwarf, one T7.5 dwarf and recovered a T4.5 dwarf and a T8.5 dwarf. We provide distance estimates which lie in the 15–85 pc range; the T7.5 and T8.5 dwarfs are probably within 25 pc of the Sun. We conclude with a discussion of the number of T dwarfs expected after completion of the LAS, comparing these initial results to theoretical simulations.</div>
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<p>We present eight new T4.5–T7.5 dwarfs identified in the UKIRT (United Kingdom Infrared Telescope) Infrared Deep Sky Survey (UKIDSS) Large Area Survey (LAS) Data Release 1 (DR1). In addition we have recovered the T4.5 dwarf SDSS J020742.91+000056.2 and the T8.5 dwarf ULAS J003402.77−005206.7. Photometric candidates were picked up in two-colour diagrams over 190 deg2 (DR1) and selected in at least two filters. All candidates exhibit near-infrared spectra with strong methane and water absorption bands characteristic of T dwarfs and the derived spectral types follow the unified scheme of Burgasser et al.. We have found six new T4.5–T5.5 dwarfs, one T7 dwarf, one T7.5 dwarf and recovered a T4.5 dwarf and a T8.5 dwarf. We provide distance estimates which lie in the 15–85 pc range; the T7.5 and T8.5 dwarfs are probably within 25 pc of the Sun. We conclude with a discussion of the number of T dwarfs expected after completion of the LAS, comparing these initial results to theoretical simulations.</p>
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<name>
<surname>Warren</surname>
<given-names>S. J.</given-names>
</name>
<xref ref-type="aff" rid="a5">5</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Burningham</surname>
<given-names>B.</given-names>
</name>
<xref ref-type="aff" rid="a3">3</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Lucas</surname>
<given-names>P. W.</given-names>
</name>
<xref ref-type="aff" rid="a3">3</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Chiu</surname>
<given-names>K.</given-names>
</name>
<xref ref-type="aff" rid="a6">6</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Liu</surname>
<given-names>M. C.</given-names>
</name>
<xref ref-type="aff" rid="a7">7</xref>
<xref ref-type="corresp" rid="c2"></xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Venemans</surname>
<given-names>B. P.</given-names>
</name>
<xref ref-type="aff" rid="a8">8</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>McMahon</surname>
<given-names>R. G.</given-names>
</name>
<xref ref-type="aff" rid="a8">8</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Allard</surname>
<given-names>F.</given-names>
</name>
<xref ref-type="aff" rid="a9">9</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Baraffe</surname>
<given-names>I.</given-names>
</name>
<xref ref-type="aff" rid="a9">9</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Y Navascués</surname>
<given-names>D. Barrado</given-names>
</name>
<xref ref-type="aff" rid="a10">10</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Carraro</surname>
<given-names>G.</given-names>
</name>
<xref ref-type="aff" rid="a11">11</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Casewell</surname>
<given-names>S. L.</given-names>
</name>
<xref ref-type="aff" rid="a2">2</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Chabrier</surname>
<given-names>G.</given-names>
</name>
<xref ref-type="aff" rid="a8">8</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Chappelle</surname>
<given-names>R. J.</given-names>
</name>
<xref ref-type="aff" rid="a12">12</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Clarke</surname>
<given-names>F.</given-names>
</name>
<xref ref-type="aff" rid="a13">13</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Day-Jones</surname>
<given-names>A. C.</given-names>
</name>
<xref ref-type="aff" rid="a3">3</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Deacon</surname>
<given-names>N. R.</given-names>
</name>
<xref ref-type="aff" rid="a14">14</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Dobbie</surname>
<given-names>P. D.</given-names>
</name>
<xref ref-type="aff" rid="a15">15</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Folkes</surname>
<given-names>S. L.</given-names>
</name>
<xref ref-type="aff" rid="a3">3</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hambly</surname>
<given-names>N. C.</given-names>
</name>
<xref ref-type="aff" rid="a16">16</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hewett</surname>
<given-names>P. C.</given-names>
</name>
<xref ref-type="aff" rid="a8">8</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Hodgkin</surname>
<given-names>S. T.</given-names>
</name>
<xref ref-type="aff" rid="a8">8</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Jones</surname>
<given-names>H. R. A.</given-names>
</name>
<xref ref-type="aff" rid="a3">3</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Kendall</surname>
<given-names>T. R.</given-names>
</name>
<xref ref-type="aff" rid="a3">3</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Magazzù</surname>
<given-names>A.</given-names>
</name>
<xref ref-type="aff" rid="a17">17</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Martín</surname>
<given-names>E. L.</given-names>
</name>
<xref ref-type="aff" rid="a1">1</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>McCaughrean</surname>
<given-names>M. J.</given-names>
</name>
<xref ref-type="aff" rid="a6">6</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Nakajima</surname>
<given-names>T.</given-names>
</name>
<xref ref-type="aff" rid="a18">18</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Pavlenko</surname>
<given-names>Y.</given-names>
</name>
<xref ref-type="aff" rid="a19">19</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Tamura</surname>
<given-names>M.</given-names>
</name>
<xref ref-type="aff" rid="a18">18</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Tinney</surname>
<given-names>C. G.</given-names>
</name>
<xref ref-type="aff" rid="a15">15</xref>
</contrib>
<contrib contrib-type="author">
<name>
<surname>Zapatero Osorio</surname>
<given-names>M. R.</given-names>
</name>
<xref ref-type="aff" rid="a1">1</xref>
</contrib>
</contrib-group>
<aff id="a1">
<label>1</label>
Instituto de Astrofísica de Canarias, Vía Láctea s/n, E-38205 La Laguna, Tenerife, Spain</aff>
<aff id="a2">
<label>2</label>
Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</aff>
<aff id="a3">
<label>3</label>
Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</aff>
<aff id="a4">
<label>4</label>
Gemini Observatory, 670 N. A'ohoku Place, Hilo, HI 96720, USA</aff>
<aff id="a5">
<label>5</label>
Astrophysics Group, Imperial College London, Blackett Laboratory, Prince Consort Road, London SW7 2AZ</aff>
<aff id="a6">
<label>6</label>
School of Physics, University of Exeter, Stocker Road, Exeter, Devon EX4 4QL</aff>
<aff id="a7">
<label>7</label>
Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, USA</aff>
<aff id="a8">
<label>8</label>
Institute of Astronomy, Madingley Road, Cambridge CB3 0HA</aff>
<aff id="a9">
<label>9</label>
CRAL, Ecole Normale Supérieure de Lyon, 46 Allée d'Italie, Université de Lyon, F-69364 Lyon Cédex 7, France</aff>
<aff id="a10">
<label>10</label>
Laboratorio de Astrofísica Espacial y Física Fundamental, INTA, PO Box 50727, E-2808 Madrid, Spain</aff>
<aff id="a11">
<label>11</label>
Departamento de Astronomia, Universidad de Chile, Casilla 36-D, Santiago, Chile</aff>
<aff id="a12">
<label>12</label>
Astronomical Institute, Academy of Sciences of the Czech Republic, Bocni II/1401a, 141 31 Prague, Czech Republic</aff>
<aff id="a13">
<label>13</label>
Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU</aff>
<aff id="a14">
<label>14</label>
Department of Astrophysics, Radboud University Nijmegen, PO Box 9010, 6500 GL Nijmegen, the Netherlands</aff>
<aff id="a15">
<label>15</label>
Anglo-Australian Observatory, PO Box 296, Epping 1710, Australia</aff>
<aff id="a16">
<label>16</label>
Scottish Universities' Physics Alliance (SUPA), Institute for Astronomy, School of Physics, University of Edinburgh, Royal Observatory, Blackford Hill, Edinburgh EH9 3HJ</aff>
<aff id="a17">
<label>17</label>
Fundación Galileo Galilei-INAF, Apartado 565, E-38700 Santa Cruz de La Palma, Spain</aff>
<aff id="a18">
<label>18</label>
National Astronomical Observatory, Mitaka, Tokyo 181-8588, Japan</aff>
<aff id="a19">
<label>19</label>
Main Astronomical Observatory, National Academy of Sciences, Zabolotnoho 27, Kyiv-127 03680, Ukraine</aff>
<author-notes>
<corresp id="c1">†E-mail:
<email>nlodieu@iac.es</email>
</corresp>
<corresp id="c2">‡Alfred P. Sloan Research Fellow.</corresp>
<fn id="fn3">
<label>*</label>
<p>Based on observations made with the United Kingdom Infrared Telescope, operated by the Joint Astronomy Centre on behalf of the UK Particle Physics and Astronomy Research Council.</p>
</fn>
</author-notes>
<pub-date pub-type="ppub">
<day>21</day>
<month>08</month>
<year>2007</year>
</pub-date>
<pub-date pub-type="epub">
<day>26</day>
<month>07</month>
<year>2007</year>
</pub-date>
<volume>379</volume>
<issue>4</issue>
<fpage>1423</fpage>
<lpage>1430</lpage>
<history>
<date date-type="accepted">
<day>23</day>
<month>5</month>
<year>2007</year>
</date>
<date date-type="received">
<day>23</day>
<month>5</month>
<year>2007</year>
</date>
</history>
<copyright-statement>© 2007 The Authors. Journal compilation © 2007 RAS</copyright-statement>
<copyright-year>2007</copyright-year>
<abstract>
<p>We present eight new T4.5–T7.5 dwarfs identified in the UKIRT (United Kingdom Infrared Telescope) Infrared Deep Sky Survey (UKIDSS) Large Area Survey (LAS) Data Release 1 (DR1). In addition we have recovered the T4.5 dwarf SDSS J020742.91+000056.2 and the T8.5 dwarf ULAS J003402.77−005206.7. Photometric candidates were picked up in two-colour diagrams over 190 deg
<sup>2</sup>
(DR1) and selected in at least two filters. All candidates exhibit near-infrared spectra with strong methane and water absorption bands characteristic of T dwarfs and the derived spectral types follow the unified scheme of Burgasser et al.. We have found six new T4.5–T5.5 dwarfs, one T7 dwarf, one T7.5 dwarf and recovered a T4.5 dwarf and a T8.5 dwarf. We provide distance estimates which lie in the 15–85 pc range; the T7.5 and T8.5 dwarfs are probably within 25 pc of the Sun. We conclude with a discussion of the number of T dwarfs expected after completion of the LAS, comparing these initial results to theoretical simulations.</p>
</abstract>
<kwd-group>
<kwd>techniques: photometric</kwd>
<kwd>techniques: spectroscopic</kwd>
<kwd>surveys</kwd>
<kwd>stars: low-mass, brown dwarfs</kwd>
<kwd>infrared: stars</kwd>
</kwd-group>
</article-meta>
</front>
<body>
<sec id="ss1">
<title>1 INTRODUCTION</title>
<p>The advent of large-scale sky surveys has revolutionized our knowledge of ultracool dwarfs (defined here as dwarfs with spectral types later than M7). The first spectroscopic brown dwarfs were confirmed in 1995: GL 229B, a T dwarf orbiting an M dwarf (
<xref ref-type="bibr" rid="b35">Nakajima et al. 1995</xref>
) and Teide 1 in the Pleiades open cluster (
<xref ref-type="bibr" rid="b37">Rebolo, Zapatero-Osorio & Martín 1995</xref>
). 10 yr on, about 500 L dwarfs with effective temperatures (
<italic>T</italic>
<sub>eff</sub>
) between ∼2200 and ∼1400 K (
<xref ref-type="bibr" rid="b4">Basri et al. 2000</xref>
;
<xref ref-type="bibr" rid="b27">Leggett et al. 2000</xref>
) have now been identified, along with around100 T dwarfs with lower temperatures (
<italic>T</italic>
<sub>eff</sub>
≃ 1400–700 K;
<xref ref-type="bibr" rid="b18">Golimowski et al. 2004</xref>
;
<xref ref-type="bibr" rid="b42">Vrba et al. 2004</xref>
). The full catalogue of L and T dwarfs is available on the
<ext-link ext-link-type="uri" xlink:href="DwarfArchives.org">DwarfArchives.org</ext-link>
webpage.
<xref ref-type="fn" rid="fn1">1</xref>
There are currently 46 T5 or later dwarfs and 17 T7–T8 dwarfs known (two of them are marked as peculiar), at the time of writing. The spectral classification of T dwarfs follows the unified scheme by
<xref ref-type="bibr" rid="b9">Burgasser et al. (2006a)</xref>
and is based on the strength of methane and water absorption bands present in the near-infrared. This sample of ultracool dwarfs is now large enough to characterize the binary properties of brown dwarfs (
<xref ref-type="bibr" rid="b12">Close et al. 2002</xref>
;
<xref ref-type="bibr" rid="b5">Bouy et al. 2003</xref>
;
<xref ref-type="bibr" rid="b8">Burgasser et al. 2003</xref>
,
<xref ref-type="bibr" rid="b10">2006b</xref>
;
<xref ref-type="bibr" rid="b32">Liu et al. 2006</xref>
;
<xref ref-type="bibr" rid="b6">Burgasser 2007</xref>
) and investigate the influence of gravity and metallicity on their spectral energy distributions (
<xref ref-type="bibr" rid="b22">Kirkpatrick 2005</xref>
).</p>
<p>The UKIRT (United Kingdom Infrared Telescope) Infrared Deep Sky Survey (UKIDSS;
<xref ref-type="bibr" rid="b26">Lawrence et al. 2006</xref>
) is a new infrared survey conducted with the UKIRT Wide Field Camera (WFCAM). The survey is now well underway with (at the time of writing) three ESO (European Southern Observatory)-wide releases: the Early Data Release (EDR) in 2006 February (
<xref ref-type="bibr" rid="b14">Dye et al. 2006</xref>
), the Data Release 1 (DR1) in 2006 July (
<xref ref-type="bibr" rid="b44">Warren et al. 2007a</xref>
) and the Data Release 2 (DR2) in 2007 March (
<xref ref-type="bibr" rid="b46">Warren et al. 2007c</xref>
). The Large Area Survey (LAS) will cover 4000 deg
<sup>2</sup>
in
<italic>YJHK</italic>
down to a 5σ sensitivity limit of
<italic>J</italic>
≃ 19.5 mag in each of two epochs (
<italic>J</italic>
≃ 20 mag when the epochs are combined) with a typical baseline of ∼2 yr.</p>
<p>The two major science drivers of the LAS are the discovery of extremely cool brown dwarfs [with spectral types even later than the coolest objects discovered in the Two Micron All Sky Survey (2MASS) and the Sloan Digital Sky Survey (SDSS)], and the discovery of high-redshift quasars (
<italic>z</italic>
≥ 6). New record-breaking low-
<italic>T</italic>
<sub>eff</sub>
dwarfs could require a new spectroscopic class beyond T (e.g.
<xref ref-type="bibr" rid="b11">Burrows, Sudarsky & Lunine 2003</xref>
) which has been pre-emptively called Y (following
<xref ref-type="bibr" rid="b23">Kirkpatrick et al. 1999</xref>
). So far UKIDSS has succeeded on both fronts;
<xref ref-type="bibr" rid="b41">Venemans et al. (2007)</xref>
report the discovery of a
<italic>z</italic>
= 5.9 quasar, and the discovery of two T dwarfs in the EDR (
<xref ref-type="bibr" rid="b21">Kendall et al. 2007</xref>
) has been followed by the identification of the latest T-type brown dwarf yet found (
<xref ref-type="bibr" rid="b45">Warren et al. 2007b</xref>
).</p>
<p>In this paper we report the discovery of eight T4.5–T7.5 dwarfs extracted from 190 deg
<sup>2</sup>
released in the LAS DR1. We also derive kinematics properties for SDSS J020742.91+000056.2 (hereafter SDSS 0207), a T4.5 dwarf discovered by
<xref ref-type="bibr" rid="b16">Geballe et al. (2002)</xref>
and recovered in our search. In
<xref ref-type="sec" rid="ss2">Section 2</xref>
we describe the photometric selection of late-T dwarfs from two-colour diagrams. In
<xref ref-type="sec" rid="ss3">Section 3</xref>
we present the spectroscopic follow-up observations conducted with the Gemini and UKIRT telescopes, and classify each object based on the
<xref ref-type="bibr" rid="b9">Burgasser et al. (2006a)</xref>
scheme. In
<xref ref-type="sec" rid="ss4">Section 4</xref>
we discuss the number of T dwarfs that our study suggests will be discovered in the complete LAS, and compare it with the predictions of
<xref ref-type="bibr" rid="b13">Deacon & Hambly (2006)</xref>
. Finally, we summarize our results and give our conclusions in
<xref ref-type="sec" rid="ss5">Section 5</xref>
.</p>
</sec>
<sec id="ss2">
<title>2 SELECTION OF T DWARF CANDIDATES</title>
<p>This section describes the photometric search carried out for late-T and possible Y dwarf candidates in the LAS, which is based on our current knowledge of the photometric properties of T dwarfs from 2MASS and SDSS, as well as on theoretical models. In addition to the traditional
<italic>JHK</italic>
filters, a new
<italic>Y</italic>
filter centred at 1.03(0.98–1.08) μm was specifically designed and installed in WFCAMto ease the selection and separation of high-redshift quasars and cool brown dwarfs in the LAS colour–colour diagrams (
<xref ref-type="bibr" rid="b43">Warren & Hewett 2002</xref>
).
<xref ref-type="fig" rid="f1">Fig. 1</xref>
shows (
<italic>Y</italic>
<italic>J</italic>
,
<italic>J</italic>
<italic>H</italic>
) for candidate and confirmed L and T dwarfs found in DR1, as well as model-predictedtypical colours, and typical colours of point sources in a WFCAMtile.</p>
<fig position="float" id="f1">
<label>Figure 1</label>
<caption>
<p>(
<italic>J</italic>
<italic>H</italic>
,
<italic>Y</italic>
<italic>J</italic>
) two-colour diagram for point sources (small crosses) in one WFCAM tile centred on (RA, Dec.) = (02
<sup>h</sup>
, 00°). Overplotted are L and T dwarfs candidates extracted from the LAS DR1 whose spectroscopy is currently underway (open triangles). Spectroscopically confirmed T4.0–T7.5 dwarfs from DR1 presented in this paper are displayed as filled circles, and the T4.5 dwarf from the EDR reported by
<xref ref-type="bibr" rid="b21">Kendall et al. (2007)</xref>
is shown as a diamond. Note that two T5.5 dwarfs have the same colours and thus the circles overlap. The T8.5 dwarf marked as an open square was selected from DR1 and is presented in
<xref ref-type="bibr" rid="b45">Warren et al. (2007b)</xref>
. Errors in the colours are typically better than 0.15 mag for the faintest objects. Also shown are the model predictions for the colours of cool brown dwarfs from the Cond (dot-dot-dot-dashed lines;
<xref ref-type="bibr" rid="b1">Allard et al. 2001</xref>
;
<xref ref-type="bibr" rid="b3">Baraffe et al. 2003</xref>
) and Settl models (solid lines; Allard et al., in preparation), and from models by Marley and collaborators (solid lines;
<xref ref-type="bibr" rid="b34">Marley et al. 2002</xref>
),
<xref ref-type="bibr" rid="b11">Burrows et al.</xref>
(2003, dashed lines) and
<xref ref-type="bibr" rid="b40">Tsuji et al.</xref>
(2004, dot–dashed lines).</p>
</caption>
<graphic xlink:href="mnras0379-1423-f1.gif"></graphic>
</fig>
<p>Known T dwarfs found by 2MASS exhibit neutral to blue near-infrared colours with decreasing effective temperature (
<xref ref-type="bibr" rid="b7">Burgasser et al. 2002</xref>
) and a rather constant
<italic>Y</italic>
<italic>J</italic>
∼ 1 (
<xref ref-type="bibr" rid="b20">Hewett et al. 2006</xref>
). SDSS discoveries (e.g.
<xref ref-type="bibr" rid="b16">Geballe et al. 2002</xref>
) show that T dwarfs are red in the optical (
<italic>i</italic>
<italic>z</italic>
≥ 2.0) and optical-to-infrared (
<italic>z</italic>
<italic>J</italic>
≥ 2.5) colours. The latter also being a good indicator of
<italic>T</italic>
<sub>eff</sub>
(
<xref ref-type="bibr" rid="b24">Knapp et al. 2004</xref>
). Hence the combination of the SDSS and the UKIDSS LAS should produce T and possibly Y dwarfs that are several magnitudes fainter than the 2MASS completeness limit.</p>
<p>Current atmosphere models predict blue near-infrared colours (
<italic>J</italic>
<italic>H</italic>
< 0.0 and
<italic>J</italic>
<italic>K</italic>
< 0.0) for dwarfs cooler than the known T dwarfs, but differ on the
<italic>Y</italic>
<italic>J</italic>
optical-to-infrared colour: the cloud-free Cond models (
<xref ref-type="bibr" rid="b1">Allard et al. 2001</xref>
;
<xref ref-type="bibr" rid="b3">Baraffe et al. 2003</xref>
), the more recent Settl models (Allard et al., in preparation) and the models of
<xref ref-type="bibr" rid="b34">Marley et al. (2002)</xref>
all imply
<italic>Y</italic>
<italic>J</italic>
colours that are bluer than those of the known late-T dwarfs, for
<italic>T</italic>
<sub>eff</sub>
∼ 700 –400 K. However,
<xref ref-type="bibr" rid="b11">Burrows et al. (2003)</xref>
and
<xref ref-type="bibr" rid="b40">Tsuji, Nakajima & Yanagisawa (2004)</xref>
predict redder
<italic>Y</italic>
<italic>J</italic>
colours for these temperatures (
<xref ref-type="bibr" rid="b29">Leggett et al. 2005</xref>
;
<xref ref-type="bibr" rid="b20">Hewett et al. 2006</xref>
). Our initial search focused on the redder
<italic>Y</italic>
<italic>J</italic>
sources, and a subsequent search for bluer objects yielded only one very late T dwarf, presented in a separate paper (
<xref ref-type="bibr" rid="b45">Warren et al. 2007b</xref>
).</p>
<sec id="ss2-1">
<title>2.1 Sample selection</title>
<p>Our basic search methodology was to extract from the UKIDSS LAS DR1 a sample of point sources with the
<italic>YJHK</italic>
colours of late-T dwarfs, guided by the known and modelled colours, and then to cross-match with the SDSS (where possible) to obtain optical-to-infrared colours.</p>
<p>We have constructed a Structured Query Language (
<sc>sql</sc>
) query to extract a list of reliable late-T dwarf candidates from the WFCAM Science Archive
<xref ref-type="fn" rid="fn2">2</xref>
(WSA; Hambly et al., in preparation). Further details regarding the
<sc>sql</sc>
statements are provided in
<xref ref-type="sec" rid="ss8">Appendix A</xref>
. We search for point sources detected in at least
<italic>Y</italic>
and
<italic>J</italic>
, and use other post-processing flags to avoid galaxies and fast moving objects. In addition, we have limited our search to the
<italic>J</italic>
= 14 –19 mag range to avoid saturated sources and maximize the completeness of our sample. Furthermore, we have imposed colour cuts of
<italic>Y</italic>
<italic>J</italic>
≥ 0.5 and
<italic>J</italic>
<italic>H</italic>
≤ 0.0 to focus on late-T dwarfs and potentially cooler objects. Finally, images were checked to insure that the candidates were real and unaffected by artefacts. The location of the new T dwarfs in the (
<italic>J</italic>
<italic>H</italic>
,
<italic>Y</italic>
<italic>J</italic>
) two-colour diagram is displayed in
<xref ref-type="fig" rid="f1">Fig. 1</xref>
.</p>
<p>For the 150 deg
<sup>2</sup>
of the UKIDSS LAS DR1 with SDSS data, only those LAS-selected candidates which had
<italic>z</italic>
<italic>J</italic>
≥ 2.5, or were undetected by SDSS, were retained. Candidates in the second category were also subject to the further requirement that they were not within a few arcsec of a brighter point source – whilst such pairs are almost always separated in UKIDSS, the fainter source often remains unregistered in SDSS, leading to appreciable numbers of false
<italic>z</italic>
-band drop-outs. Having applied all these automated filters, we were left with a total of 19 objects, 10 of which were quickly revealed to be spurious by visual inspection leaving a final list of just nine viable T dwarf candidates. Of these, one (ULAS J022200.43−002410.5) is awaiting further investigation, one is a known T4.5 dwarf (SDSS 0207;
<xref ref-type="bibr" rid="b16">Geballe et al. 2002</xref>
) and one is a new UKIDSS T8.5 dwarf (ULAS J003402.77−005206.7;
<xref ref-type="bibr" rid="b45">Warren et al. 2007b</xref>
). The remaining six have been confirmed as new T dwarfs. Finding charts are shown in
<xref ref-type="fig" rid="f2">Fig. 2</xref>
, their basic observational properties are summarized in
<xref ref-type="table" rid="t1">Table 1</xref>
and a brief statistical analysis of the sample is given in
<xref ref-type="sec" rid="ss4-3">Section 4.3</xref>
.</p>
<fig position="float" id="f2">
<label>Figure 2</label>
<caption>
<p>Finding charts for the eight new T4.5–T7.5 dwarfs extracted from the UKIDSS LAS DR1 and presented in this paper. Charts are
<italic>J</italic>
-band images of 2 arcmin on a side with north up and east left.</p>
</caption>
<graphic xlink:href="mnras0379-1423-f2.gif"></graphic>
</fig>
<table-wrap id="t1">
<label>Table 1</label>
<caption>
<p>List of the coordinates (J2000), infrared magnitudes (
<italic>YJHK</italic>
) on the WFCAM/MKO-system and their associated uncertainties, for 10 T dwarfs identified in the UKIDSS LAS DR1 (ordered by RA), including SDSS J020742.83+000056.2 (
<xref ref-type="bibr" rid="b16">Geballe et al. 2002</xref>
) and ULAS J003402.77−005206.7 (
<xref ref-type="bibr" rid="b45">Warren et al. 2007b</xref>
). The 5σ limits are computed using sky noise following the prescription of
<xref ref-type="bibr" rid="b14">Dye et al. (2006)</xref>
. Two sets of
<italic>JHK</italic>
observations are available for ULAS 2239: the first one originates from the UKIDSS LAS DR1; the second one comes from additional UKIRT/UFTI observations taken 2006 September 3 (
<xref ref-type="sec" rid="ss2-2">Section 2.2</xref>
).
<italic>z</italic>
-band photometry was also obtained for this source with EMMI at the NTT and we measured
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
(AB) = 22.46 ± 0.09 mag. The quoted errors do not include calibration uncertainties; these may be as high as 0.1 mag at
<italic>Y</italic>
, and 0.02 mag at
<italic>JHK</italic>
(
<xref ref-type="bibr" rid="b44">Warren et al. 2007a</xref>
).</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<td>Name</td>
<td>RA</td>
<td>Dec.</td>
<td>
<italic>Y</italic>
</td>
<td>
<italic>J</italic>
</td>
<td>
<italic>H</italic>
</td>
<td>
<italic>K</italic>
</td>
</tr>
</thead>
<tbody>
<tr>
<td>ULAS J002422.94+002247.9</td>
<td>00 24 22.94</td>
<td>+00 22 47.9</td>
<td>19.59 ± 0.15</td>
<td>18.16 ± 0.07</td>
<td>18.24 ± 0.16</td>
<td>>18.05</td>
</tr>
<tr>
<td>ULAS J003402.77−005206.7</td>
<td>00 34 02.77</td>
<td>−00 52 06.7</td>
<td>18.90 ± 0.10</td>
<td>18.14 ± 0.08</td>
<td>18.50 ± 0.22</td>
<td>>17.94</td>
</tr>
<tr>
<td>ULAS J020336.94−010231.1</td>
<td>02 03 36.94</td>
<td>−01 02 31.1</td>
<td>19.06 ± 0.10</td>
<td>18.04 ± 0.05</td>
<td>18.31 ± 0.12</td>
<td>18.13 ± 0.17</td>
</tr>
<tr>
<td>SDSS 0207</td>
<td>02 07 42.91</td>
<td>+00 00 56.2</td>
<td>17.94 ± 0.03</td>
<td>16.75 ± 0.01</td>
<td>16.79 ± 0.04</td>
<td>16.71 ± 0.05</td>
</tr>
<tr>
<td>ULAS J082707.67−020408.2</td>
<td>08 27 07.67</td>
<td>−02 04 08.2</td>
<td>18.29 ± 0.05</td>
<td>17.19 ± 0.02</td>
<td>17.44 ± 0.05</td>
<td>17.52 ± 0.11</td>
</tr>
<tr>
<td>ULAS J090116.23−030635.0</td>
<td>09 01 16.23</td>
<td>−03 06 35.0</td>
<td>18.82 ± 0.05</td>
<td>17.90 ± 0.04</td>
<td>18.46 ± 0.13</td>
<td>>18.21</td>
</tr>
<tr>
<td>ULAS J094806.06+064805.0</td>
<td>09 48 06.06</td>
<td>+06 48 05.0</td>
<td>20.03 ± 0.14</td>
<td>18.85 ± 0.07</td>
<td>19.46 ± 0.22</td>
<td>>18.62</td>
</tr>
<tr>
<td>ULAS J100759.90−010031.1</td>
<td>10 07 59.90</td>
<td>−01 00 31.1</td>
<td>19.82 ± 0.12</td>
<td>18.67 ± 0.07</td>
<td>18.77 ± 0.18</td>
<td>>18.17</td>
</tr>
<tr>
<td>ULAS J101821.78+072547.1</td>
<td>10 18 21.78</td>
<td>+07 25 47.1</td>
<td>18.90 ± 0.08</td>
<td>17.71 ± 0.04</td>
<td>17.87 ± 0.07</td>
<td>18.12 ± 0.17</td>
</tr>
<tr>
<td>ULAS 2239</td>
<td>22 39 55.76</td>
<td>+00 32 52.6</td>
<td>19.94 ± 0.17</td>
<td>18.86 ± 0.09</td>
<td>>18.87</td>
<td>>18.18</td>
</tr>
<tr>
<td colspan="4" align="left"></td>
<td>18.85 ± 0.05
<sup>
<italic>a</italic>
</sup>
</td>
<td>19.10 ± 0.10
<sup>
<italic>a</italic>
</sup>
</td>
<td>18.88 ± 0.06
<sup>
<italic>a</italic>
</sup>
</td>
</tr>
</tbody>
</table>
<table-wrap-foot>
<fn id="t1_note81">
<p>
<sup>
<italic>a</italic>
</sup>
UKIRT/UFTI photometry.</p>
</fn>
</table-wrap-foot>
</table-wrap>
<p>For the 40 deg
<sup>2</sup>
of the UKIDSS LAS DR1 outside the SDSS DR5 footprint, we rejected sources with optical counterparts in the United States Naval Observatory (USNO) catalogues. However, the magnitude limit of these catalogues is so bright that several hundred candidates remained, requiring cross-correlation with other optical catalogues or visual inspection. Not all of these objects have been followed up, but spectra were obtained of two of the most promising, ULAS J082707.67−020408.2 and ULAS J090116.23−030635.0, both of which were confirmed as T dwarfs. Their basic parameters are listed in
<xref ref-type="table" rid="t1">Table 1</xref>
and finding charts are given in
<xref ref-type="fig" rid="f2">Fig. 2</xref>
.</p>
</sec>
<sec id="ss2-2">
<title>2.2 Additional photometry</title>
<p>Additional optical and near-infrared photometry was obtained with UKIRT and the New Technology Telescope (NTT) for one T dwarf, ULAS J223955.76+003252.6 (hereafter ULAS 2239). Details of these observations are given below.</p>
<p>ULAS 2239 was observed at UKIRT on
<sc>ut</sc>
2006 September 3, using the UKIRT Fast-Track Imager (UFTI;
<xref ref-type="bibr" rid="b38">Roche et al. 2003</xref>
). The Mauna Kea Observatories (MKO)
<italic>J</italic>
,
<italic>H</italic>
and
<italic>K</italic>
filters were used (
<xref ref-type="bibr" rid="b39">Tokunaga, Simons & Vacca 2002</xref>
), and the data calibrated using UKIRT Faint Standards; the photometric system should be identical to the WFCAM system (
<xref ref-type="bibr" rid="b30">Leggett et al. 2006</xref>
). The night was photometric with 0.6 arcsec seeing. Individual exposure times on target were 1 min, and the total exposure time was 9 min at
<italic>J</italic>
, 18 min at
<italic>H</italic>
and 27 min at
<italic>K</italic>
, dithering the dwarf on a 3 × 3 grid with 10 arcsec offsets. Photometry was measured using a 2-arcsec diameter aperture and is presented in
<xref ref-type="table" rid="t1">Table 1</xref>
.</p>
<p>In addition, we obtained
<italic>z</italic>
-band photometry (filter ♯611) for ULAS 2239 with the ESO Multi-Mode Instrument (EMMI), at the NTT, on the night beginning 2006 August 18. The total exposure time was 15 min. The filter/detector combination is referred to here as
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
and is similar to the SDSS
<italic>z</italic>
. Using the measured CCD sensitivity curve, and the filter transmission curve, we followed the procedure used by
<xref ref-type="bibr" rid="b20">Hewett et al. (2006)</xref>
to establish the colour relation
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
(AB) =
<italic>z</italic>
(AB) − 0.05(
<italic>i</italic>
(AB) −
<italic>z</italic>
(AB)), for O to M dwarf stars. The offset to the Vega system is
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
(AB) =
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
+ 0.54. Photometry in
<italic>i</italic>
and
<italic>z</italic>
of SDSS DR5 sources in the field was converted to
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
, and the brightness of the source was measured by relative photometry using a fixed aperture, with the result
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
(AB) =22.46 ± 0.09. For a T6 dwarf
<italic>z</italic>
(AB) ∼
<italic>z</italic>
<sub>
<italic>N</italic>
</sub>
(AB) + 0.2.</p>
</sec>
</sec>
<sec id="ss3">
<title>3 SPECTROSCOPIC FOLLOW-UP</title>
<sec id="ss3-1">
<title>3.1 Gemini/GNIRS spectroscopy</title>
<p>The Gemini Near-Infrared Spectrograph (GNIRS;
<xref ref-type="bibr" rid="b15">Elias et al. 2006</xref>
) on Gemini South was used to make quick response observations, through programme GS-2006B-Q-36. All photometric candidates were confirmed as T dwarfs with spectral types later than T4. GNIRS was used in cross-dispersed mode with the 32l mm
<sup>−1</sup>
grism, the 1.0-arcsec slit (position angle of 0°) and the short camera, to obtain 0.9–2.5 μm
<italic>R</italic>
∼ 500 (per resolution element) spectra. Triggered observations were made on the nights of 2006 August 26, October 12, 20, 27 and 2007 January 4, 20 with total integration time for each observation of 16 min. In each case the target was nodded 3 arcsec along the slit in an ‘ABBA’ pattern using individual exposure times of 240 s. Calibrations were achieved using lamps in the on-telescope calibration unit. A0 and early F stars were observed as spectroscopic standards, either directly before or after the target observations, at an airmass that closely matched the mid-point airmass of the target in order to remove the effects of telluric absorption. The observing conditions included some patchy cloud (i.e. cloud cover <70 percentile), seeing from 0.5 to 1.4 arcsec, and humidity ranging from 10 to 50 per cent.</p>
<p>Data reduction was initially done using tasks in the Gemini GNIRS
<sc>iraf</sc>
(Image Reduction and Analysis Facility) package. Files were prepared and corrected for offset bias using
<sc>nsprepare</sc>
and
<sc>nvnoise</sc>
, and order separation achieved with
<sc>nscut</sc>
. Each order was then median stacked at the A and B positions, and a difference image obtained using
<sc>gemarith</sc>
. Flat-field correction was not necessary since variations across the 6-arcsec slit are less than 0.1 per cent. S-distortion correction and wavelength calibration were performed interactively using the telluric star spectra and argon arc lamp spectra, with
<sc>nsappwave</sc>
,
<sc>nssdist</sc>
and
<sc>nswave</sc>
. Further reduction was carried out using custom
<sc>idl</sc>
(Interactive Data Language) routines. Apertures (∼1.5-arcsec wide) were centred on the spectra at the A and B positions, and the sky residuals were fit (and subtracted) using a surface constructed via a series of least-squares linear fits across the slit (excluding pixels within the apertures), with one fit for each spatial pixel row. Spectra were then extracted by summing within the A and B position apertures and combining. Noise spectra were also determined using a combination of the sky noise (between the A and B position spectra), and the photon noise associated with the spectra themselves. The target spectra were flux calibrated on a relative scale using the telluric standard spectra (after appropriate interpolation across any hydrogen lines in the standards) with an assumed blackbody function for
<italic>T</italic>
<sub>eff</sub>
= 10000 and 7000 K for A0 and early F tellurics, respectively. The spectral orders were then trimmed of their noisiest portions, and the spectra normalized to unity at 1.27 μm (the average level from 1.265 to 1.275 μm). Although the shape of each spectrum will be correct, the absolute flux calibration is best determined by scaling the spectra to match the WFCAM photometry. We find that a single scaling factor reproduces the observed
<italic>JHK</italic>
magnitudes within the 2–10 per cent WFCAM photometric uncertainties, except for the
<italic>K</italic>
magnitudes of ULAS J020336.94−010231.1 and ULAS J101821.78+072547.1 which the spectra suggest are 1.5σ and 2.5σ brighter than the WFCAM measurements, respectively. The final smoothed spectra of the eight new T dwarfs observed with GNIRS are displayed in
<xref ref-type="fig" rid="f3">Fig. 3</xref>
.</p>
<fig position="float" id="f3">
<label>Figure 3</label>
<caption>
<p>Gemini/GNIRS near-infrared (0.9–2.5 μm) spectra of T4.5–T7.5 dwarfs confirmed spectroscopically. From bottom to top ordered by increasing spectral type are ULAS J002422.94+002247.9 (T4.5), ULAS J020336.94−010231.1 (T5), ULAS J101821.78+072547.1 (T5), ULAS J100759.18−010031.1 (T5.5), ULAS J082707.67−020408.2 (T5.5), ULAS 2239 (T5.5), ULAS J094806.06+064805.0 (T7) and ULAS J090116.23−030635.0 (T7.5). Spectra are smoothed by a boxcar of 10 pixels and shifted up by increments of 1.2 for clarity (zero flux levels are indicated by the horizontal dotted lines). Regions badly affected by telluric features (1.350–1.445 and 1.811–1.942 μm) have been omitted.</p>
</caption>
<graphic xlink:href="mnras0379-1423-f3.gif"></graphic>
</fig>
</sec>
<sec id="ss3-2">
<title>3.2 UKIRT/UIST spectroscopy</title>
<p>SDSS 0207 was observed at UKIRT on
<sc>ut</sc>
2006 September 4, using the UKIRT Imager Spectrometer (UIST;
<xref ref-type="bibr" rid="b36">Ramsay Howat et al. 2004</xref>
). The
<italic>HK</italic>
grism was used with the 4-pixel slit, giving a resolution
<italic>R</italic>
= 550. Individual exposure times on target were 240 s, and the total exposure was 64 min, nodding the target along the slit by 12 arcsec. The instrument calibration lamps were used to provide accurate flat-fielding and wavelength calibration. The F5V star HD 5892 was observed prior to the target to remove the effects of telluric absorption, and to provide an approximate flux calibration. More accurate absolute flux calibration was achieved by scaling the spectra to the
<italic>H</italic>
and
<italic>K</italic>
magnitudes measured in the LAS. The final spectrum of SDSS 0207 is shown in
<xref ref-type="fig" rid="f4">Fig. 4</xref>
.</p>
<fig position="float" id="f4">
<label>Figure 4</label>
<caption>
<p>UKIRT/UIST near-infrared spectrum (
<italic>HK</italic>
grism; 1.4–2.5 μm) of a bright T4.0 dwarf (SDSS 0207) selected photometrically from the UKIDSS LAS DR1 and confirmed spectroscopically. The discovery 1.0–2.5 μmspectrum is presented in
<xref ref-type="bibr" rid="b16">Geballe et al. (2002)</xref>
.</p>
</caption>
<graphic xlink:href="mnras0379-1423-f4.gif"></graphic>
</fig>
</sec>
<sec id="ss3-3">
<title>3.3 Spectral classification</title>
<p>For each spectrum we calculated the five near-infrared spectral indices H
<sub>2</sub>
O-
<italic>J</italic>
, CH
<sub>4</sub>
-
<italic>J</italic>
, H
<sub>2</sub>
O-
<italic>H</italic>
, CH
<sub>4</sub>
-
<italic>H</italic>
and CH
<sub>4</sub>
-
<italic>K</italic>
as defined in
<xref ref-type="bibr" rid="b9">Burgasser et al. (2006a)</xref>
. We also compared the data by eye to template spectra for T dwarfs defined by Burgasser et al. as standards for the T4, T5, T6, T7 and T8 types. The results for the newT dwarfs with GNIRS spectra are given in
<xref ref-type="table" rid="t2">Table 2</xref>
. For the recovered SDSS 0207, we derive a type of T4.0 ± 0.5, in agreement with
<xref ref-type="bibr" rid="b16">Geballe et al. (2002)</xref>
and
<xref ref-type="bibr" rid="b9">Burgasser et al. (2006a)</xref>
who derive T4.5 ± 0.5. Some scatter is present in the spectral indices given in
<xref ref-type="table" rid="t2">Table 2</xref>
. The GNIRS exposures were designed to provide only a rough spectral type for potential late-T dwarfs, and so can yield somewhat noisy spectra, especially in the
<italic>K</italic>
band. Consequentially, the direct comparison with templates has been given more weight than the spectral indices in the assignment of spectral types, and the adopted uncertainty in
<xref ref-type="table" rid="t2">Table 2</xref>
reflects the range in type implied by this comparison.</p>
<table-wrap id="t2">
<label>Table 2</label>
<caption>
<p>List of spectral types derived from indices and from the comparison with T dwarf templates (cf.
<xref ref-type="bibr" rid="b9">Burgasser et al. 2006a</xref>
). The CH
<sub>4</sub>
-
<italic>K</italic>
index derived for the latest T dwarf is very uncertain due to low signal-to-noise ratio in the
<italic>K</italic>
band.</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<td>Name</td>
<td>H
<sub>2</sub>
O-
<italic>J</italic>
</td>
<td>CH
<sub>4</sub>
-
<italic>J</italic>
</td>
<td>H
<sub>2</sub>
O-
<italic>H</italic>
</td>
<td>CH
<sub>4</sub>
-
<italic>H</italic>
</td>
<td>CH
<sub>4</sub>
-
<italic>K</italic>
</td>
<td>Template</td>
<td>Adopted</td>
</tr>
</thead>
<tbody>
<tr>
<td>ULAS J002422.94+002247.9</td>
<td>0.291 (T4.5)</td>
<td>0.382 (T5.5)</td>
<td>0.423 (T3.5)</td>
<td>0.547 (T4)</td>
<td>0.195 (T5.5)</td>
<td>T4.5</td>
<td>T4.5 ± 0.5</td>
</tr>
<tr>
<td>ULAS J003402.77−005206.7</td>
<td>0.012 (T8.5)</td>
<td>0.144 (T8.5)</td>
<td>0.133 (T8.5)</td>
<td>0.096 (T8)</td>
<td>0.091 (≥T7)</td>
<td>T8–T8.5</td>
<td>T8.5 ± 0.5</td>
</tr>
<tr>
<td>ULAS J020336.94−010231.1</td>
<td>0.288 (T4.5)</td>
<td>0.429 (T4.5)</td>
<td>0.328 (T5.5)</td>
<td>0.410 (T5)</td>
<td>0.245 (T4.5)</td>
<td>T4.5–T5</td>
<td>T5.0 ± 0.5</td>
</tr>
<tr>
<td>SDSS 0207</td>
<td>– (–)</td>
<td>– (–)</td>
<td>0.391 (T4)</td>
<td>0.565 (T4)</td>
<td>0.282 (T4)</td>
<td>T4.0</td>
<td>T4.0 ± 0.5</td>
</tr>
<tr>
<td>ULAS J082707.67−020408.2</td>
<td>0.213 (T5.5)</td>
<td>0.384 (T5.5)</td>
<td>0.300 (T6)</td>
<td>0.384 (T5.5)</td>
<td>0.238 (T4.5)</td>
<td>T5–T5.5</td>
<td>T5.5 ± 0.5</td>
</tr>
<tr>
<td>ULAS J090116.23−030635.0</td>
<td>0.075 (T7.5)</td>
<td>0.226 (T7)</td>
<td>0.118 (T8)</td>
<td>0.186 (T7)</td>
<td>0.198 (T5)</td>
<td>T7–T7.5</td>
<td>T7.5 ± 0.5</td>
</tr>
<tr>
<td>ULAS J094806.06+064805.0</td>
<td>0.087 (T7)</td>
<td>0.215 (T7.5)</td>
<td>0.254 (T6.5)</td>
<td>0.222 (T7)</td>
<td>0.115 (T6.5)</td>
<td>T7.0</td>
<td>T7.0 ± 0.5</td>
</tr>
<tr>
<td>ULAS J100759.90−010031.1</td>
<td>0.177 (T5.5)</td>
<td>0.321 (T6)</td>
<td>0.303 (T6)</td>
<td>0.345 (T5.5)</td>
<td>0.191 (T5.5)</td>
<td>T5.5</td>
<td>T5.5 ± 0.5</td>
</tr>
<tr>
<td>ULAS J101821.78+072547.1</td>
<td>0.304 (T4.5)</td>
<td>0.437 (T4.5)</td>
<td>0.376 (T4.5)</td>
<td>0.451 (T4.5)</td>
<td>0.151 (T6)</td>
<td>T5.0</td>
<td>T5.0 ± 0.5</td>
</tr>
<tr>
<td>ULAS 2239</td>
<td>0.195 (T5.5)</td>
<td>0.324 (T6)</td>
<td>0.258 (T6.5)</td>
<td>0.356 (T5.5)</td>
<td>0.187 (T5.5)</td>
<td>T5.5–T6</td>
<td>T5.5 ± 0.5</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>The comparison to the spectral templates, together with modelled trends with gravity and metallicity (as shown for example by
<xref ref-type="bibr" rid="b33">Liu, Leggett & Chiu 2007</xref>
and
<xref ref-type="bibr" rid="b31">Leggett et al. 2007</xref>
, ApJ, submitted)allow us to identify dwarfs that may have a metallicity or a gravity different from the solar-neighbourhood sample that defines the templates.
<xref ref-type="bibr" rid="b31">Leggett et al.</xref>
(2007, ApJ, submitted; their
<xref ref-type="fig" rid="f3">fig. 3</xref>
)show that, for late-T dwarfs, increasing gravity suppresses the
<italic>K</italic>
-band flux due to increased pressure-induced H
<sub>2</sub>
opacity (and vice-versa), while decreasing metallicity also increases the H
<sub>2</sub>
opacity and suppresses
<italic>K</italic>
, but has the additional signature of broadening the 1 μm
<italic>Y</italic>
-band flux peak. Searching for these signatures, we find that most of our sample appear to be typical of the solar neighbourhood, so that metallicity is likely to be solar, and gravity is likely to be given by log 
<italic>g</italic>
= 5.0. The exceptions are (see
<xref ref-type="fig" rid="f3">Fig. 3</xref>
) ULAS J020336.94−010231.1 which appears to be a low-gravity object based on the high
<italic>K</italic>
-band flux, ULAS J090116.23−030635.0 which appears to be a high-gravity object based on the low
<italic>K</italic>
-band flux and ULAS J101821.78+072547.1 which appears to be metal rich based on the high
<italic>K</italic>
-band flux and narrow
<italic>Y</italic>
-band flux peak. ULAS 2239 may have a somewhat low gravity, however, the spectrum is very noisy for this very faint dwarf.
<xref ref-type="fig" rid="f3">Fig. 3</xref>
also suggests that the
<italic>K</italic>
-band flux of ULAS J100759.90−010031.1 is suppressed, but the spectrum is compromised by data spikes at 2.0 and 2.2 μm, and the spectral energy distribution is in fact very similar to the templates if these regions are ignored.</p>
</sec>
</sec>
<sec id="ss4">
<title>4 DISCUSSION</title>
<sec id="ss4-1">
<title>4.1 Properties of SDSS J020742.83+000056.2</title>
<p>Our search criteria recovered one T dwarf found by the SDSS group (SDSS 0207 – T4.5;
<xref ref-type="bibr" rid="b16">Geballe et al. 2002</xref>
).
<xref ref-type="bibr" rid="b16">Geballe et al. (2002)</xref>
reported
<italic>JHK</italic>
magnitudes for SDSS 0207 of 16.63, 16.66 and 16.62, with uncertainties of 0.05 mag. Observations were obtained with UKIRT/UFTI and are described in
<xref ref-type="bibr" rid="b28">Leggett et al. (2002)</xref>
. Although the WFCAM magnitudes (
<xref ref-type="table" rid="t1">Table 1</xref>
) are ∼0.1 mag fainter, the two data sets agree to 2σ and are thus reasonably consistent. The second epoch LAS could be used to investigate photometric variability in the T dwarfs. The derived spectral types (T4.5 in the discovery paper and T4 here) are in agreement within the classification uncertainties.</p>
<p>This object has known proper motion (0.156 ± 0.011 arcsec yr
<sup>−1</sup>
) and parallax (0.035 ± 0.001 arcsec;
<xref ref-type="bibr" rid="b42">Vrba et al. 2004</xref>
). We are able to estimate its proper motion from the ∼3 yr baseline between the SDSS (2002 September 4) and LAS (2005 November 26) observations. We have measured 0.142 and 0.085 arcsec yr
<sup>−1</sup>
in right ascension (RA) and declination (Dec.), respectively, yielding a total proper motion of 0.166 ± 0.020 arcsec yr
<sup>−1</sup>
consistent with the value given in
<xref ref-type="bibr" rid="b42">Vrba et al. (2004)</xref>
. SDSS observations can thus provide a first epoch comparison for UKIDSS, improving the prospects for identifying sources with significant proper motion in the second-epoch
<italic>J</italic>
-band LAS observations.</p>
</sec>
<sec id="ss4-2">
<title>4.2 Distances</title>
<p>To estimate the distances of the new T dwarfs we considered three relationships between spectral type and absolute magnitude: those published by
<xref ref-type="bibr" rid="b42">Vrba et al. (2004)</xref>
,
<xref ref-type="bibr" rid="b24">Knapp et al. (2004)</xref>
and
<xref ref-type="bibr" rid="b32">Liu et al. (2006)</xref>
. The first was derived using 19 T0–T8 dwarfs with measured parallaxes.
<xref ref-type="bibr" rid="b24">Knapp et al. (2004)</xref>
supplied a fifth-order polynomial fit to 42 spectroscopically confirmed T dwarfs.
<xref ref-type="bibr" rid="b32">Liu et al. (2006)</xref>
employed the same procedure as
<xref ref-type="bibr" rid="b24">Knapp et al. (2004)</xref>
but excluded known and possible binaries from the fit to take into account the higher frequency of binary systems among objects with L–T transition colours (e.g.
<xref ref-type="bibr" rid="b10">Burgasser et al. 2006b</xref>
;
<xref ref-type="bibr" rid="b32">Liu et al. 2006</xref>
). The exclusion of binaries results in a relation with fainter absolute magnitudes and smaller inferred distances, for early-mid T dwarfs. The values derived using the three relationships are given in
<xref ref-type="table" rid="t3">Table 3</xref>
.</p>
<table-wrap id="t3">
<label>Table 3</label>
<caption>
<p>Distances (pc) for the eight new late-T dwarfs presented in this paper, based on relationships between absolute magnitude and spectral type from
<xref ref-type="bibr" rid="b42">Vrba et al.</xref>
(2004, V04),
<xref ref-type="bibr" rid="b24">Knapp et al.</xref>
(2004, K04) and
<xref ref-type="bibr" rid="b32">Liu et al.</xref>
(2006, L06). The adopted distances allow for a 0.5 mag uncertainty on the fifth-order polynomial provided in
<xref ref-type="bibr" rid="b32">Liu et al. (2006)</xref>
. The distance for the T8.5 ULAS J003402.77−005206.7 is taken from
<xref ref-type="bibr" rid="b45">Warren et al. (2007b)</xref>
and is based on model spectral fits.</p>
</caption>
<table frame="hsides" rules="groups">
<thead>
<tr>
<td>Name</td>
<td>V04</td>
<td>K04</td>
<td>L06</td>
<td>Adopted</td>
</tr>
</thead>
<tbody>
<tr>
<td>ULAS J002422.94+002247.9</td>
<td>54.4</td>
<td>62.4</td>
<td>53.1</td>
<td>42–67</td>
</tr>
<tr>
<td>ULAS J003402.77−005206.7</td>
<td colspan="3"></td>
<td>14–21</td>
</tr>
<tr>
<td>ULAS J020336.94−010231.1</td>
<td>47.6</td>
<td>54.5</td>
<td>48.3</td>
<td>38–61</td>
</tr>
<tr>
<td>ULAS J082707.67−020408.2</td>
<td>29.2</td>
<td>33.1</td>
<td>30.8</td>
<td>24–39</td>
</tr>
<tr>
<td>ULAS J090116.23−030635.0</td>
<td>22.3</td>
<td>28.3</td>
<td>26.0</td>
<td>21–33</td>
</tr>
<tr>
<td>ULAS J094806.06+064805.0</td>
<td>41.4</td>
<td>41.4</td>
<td>47.7</td>
<td>38–60</td>
</tr>
<tr>
<td>ULAS J100759.90−010031.1</td>
<td>57.9</td>
<td>65.6</td>
<td>60.9</td>
<td>48–77</td>
</tr>
<tr>
<td>ULAS J101821.78+072547.1</td>
<td>40.9</td>
<td>46.6</td>
<td>41.5</td>
<td>33–52</td>
</tr>
<tr>
<td>ULAS 2239</td>
<td>62.8</td>
<td>71.5</td>
<td>66.1</td>
<td>52–83</td>
</tr>
</tbody>
</table>
</table-wrap>
<p>For our final distance estimates we chose those derived using the most recent spectral type–
<italic>M</italic>
<sub>
<italic>J</italic>
</sub>
relation (
<xref ref-type="bibr" rid="b32">Liu et al. 2006</xref>
). The uncertainties in our distance estimates were computed by assuming a dispersion of ±0.5 mag in the spectral type–absolute magnitude relation. The adopted mean distances and their associated intervals are quoted in
<xref ref-type="table" rid="t3">Table 3</xref>
. These distances assume single objects; if any of these sources are in fact multiple systems, they would be more distant by 40 per cent, assuming an unresolved binary with components of comparable brightness.</p>
<p>These spectroscopic distances show that the LAS is detecting late-T dwarfs out to ∼80 pc (see also
<xref ref-type="bibr" rid="b21">Kendall et al. 2007</xref>
, the discovery of ULAS J1452+0655, a T4.5 dwarf at around 80 pc, shown in our
<xref ref-type="fig" rid="f1">Fig. 1</xref>
as a diamond). Furthermore, note that the T7.5 dwarf ULAS J090116.23−030635.0, and the T8.5 dwarf ULAS J003402.77−005206.7 (
<xref ref-type="bibr" rid="b45">Warren et al. 2007b</xref>
), may lie within the 25 pc limit of the catalogue of nearby stars (
<xref ref-type="bibr" rid="b17">Gliese & Jahreiss 1995</xref>
), and thus represent an important addition to the list of nearby cool brown dwarfs.</p>
<p>Assuming the same spectral type–absolute magnitude relationship, we derive a spectroscopic distance of 28 pc (23–36 pc) for SDSS 0207, in good agreement with the parallax distance of 28 ± 0.8 pc (
<xref ref-type="bibr" rid="b42">Vrba et al. 2004</xref>
). This object is of interest as it populates the bump seen for the L–T sequence in the spectral type–
<italic>M</italic>
<sub>
<italic>J</italic>
</sub>
diagram for late-L to mid-T dwarfs (
<xref ref-type="bibr" rid="b10">Burgasser et al. 2006b</xref>
;
<xref ref-type="bibr" rid="b32">Liu et al. 2006</xref>
). Although this bump is known to be partially caused by unresolved binarity, it also appears to be intrinsic to the atmospheric physics of the L–T transition.</p>
</sec>
<sec id="ss4-3">
<title>4.3 Expected numbers of late-T dwarfs in the LAS</title>
<p>In this section we try to estimate the observed number density of late-T (≥T4;
<italic>T</italic>
<sub>eff</sub>
≤ 1300 K) dwarfs from our spectroscopic follow-up and compare it with predictions by
<xref ref-type="bibr" rid="b13">Deacon & Hambly (2006)</xref>
. Quantification of completeness is difficult at this early stage at the faint end of the survey. However, we expect our sample to be complete down to
<italic>J</italic>
= 18.5 mag and possibly
<italic>J</italic>
= 19 mag because all late-T dwarfs will be detected in the
<italic>Y</italic>
passband.</p>
<p>This paper reports 10 T dwarfs, with spectral type T4 and later, extracted from a total area of 190 deg
<sup>2</sup>
(DR1). Of these, seven are brighter than
<italic>J</italic>
= 18.5 mag. To compare directly with the numbers quoted in table 1 of
<xref ref-type="bibr" rid="b13">Deacon & Hambly (2006)</xref>
, we need to scale our numbers to 4000 deg
<sup>2</sup>
(the full LAS coverage after 7 yr of operation) and take into account the final depth of the survey (
<italic>J</italic>
∼ 20 mag) after two epochs. We assume here a uniform and constant distribution of ultracool dwarfs which is reasonable, because an extra magnitude of depth for late-T dwarfs will not probe the scaleheight of the disc.</p>
<p>Consequently, for the bright sample with
<italic>J</italic>
≤ 18.5 mag, we should find 7 × 4000/190 multiplied by a factor of 8 to account for the volume difference, yielding a total of 1179 ± 34 late-T dwarfs. If we take into account all T dwarfs reported here, we estimate a total of (10 × 4000/190) × 4 = 842 ± 29 T dwarfs in the full LAS. These values match the predicted numbers from the simulations of
<xref ref-type="bibr" rid="b13">Deacon & Hambly (2006)</xref>
for a mass function with a slope between α=−1.0 and α=−0.5[in Salpeter units or ξ(log 
<italic>m</italic>
) = d
<italic>n</italic>
/dlog 
<italic>m</italic>
<italic>m</italic>
<sup>−α</sup>
; 676–1060 late-T dwarfs, defined in
<xref ref-type="bibr" rid="b13">Deacon & Hambly 2006</xref>
as dwarfs with 1300 ≥
<italic>T</italic>
<sub>eff</sub>
 (K) ≥ 700]. This result is also in agreement with the derivations of α=−0.7 ± 0.7 for
<italic>M</italic>
≤ 0.08 M
<sub></sub>
by
<xref ref-type="bibr" rid="b25">Kroupa (2001)</xref>
and conclusions drawn by
<xref ref-type="bibr" rid="b2">Allen et al. (2005)</xref>
from their Bayesian approach (α=−0.6 ± 0.7 for
<italic>M</italic>
≤ 0.04 –0.1  M
<sub></sub>
). Similar results are found for the low-mass end of the initial mass function (IMF) in young open clusters (e.g. σ Orionis;
<xref ref-type="bibr" rid="b19">González-García et al. 2006</xref>
).</p>
<p>However, uncertainties in the expected number of T dwarfs and the slope of the mass function remain large on both the observational and theoretical sides. Malmquist related biases have not been taken into consideration for example, but contribute significant uncertainty. For instance, earlier T dwarfs could be detected out to greater distance than some mid-late Ts, and our colour selections are poorly suited for identifying these. Furthermore, there will be a bias favouring unresolved binary systems, as they are brighter than single T dwarfs and detectable at greater distance. The Deacon & Hambly numbers do not account for this bias, but it will be inherent in our sample. A more extensive spectroscopic follow-up of L and T dwarf candidates from the LAS is necessary to disentangle the various possible shapes of the IMF.</p>
</sec>
</sec>
<sec id="ss5">
<title>5 CONCLUSIONS</title>
<p>We have presented the spectroscopic confirmation of eight new T4.5–T7.5 dwarfs identified over the entire LAS area released in the first UKIDSS data release, together with the recovery of a T4.5 dwarf already discovered in the SDSS, and a T8.5 reported by(
<xref ref-type="bibr" rid="b45">Warren et al. 2007b</xref>
). The spectral classification is based on the unified T-dwarf classification scheme of
<xref ref-type="bibr" rid="b9">Burgasser et al. (2006a)</xref>
. In addition, we have estimated distances for all of our sources using recent spectral type–absolute magnitude relationships. The two latest and coolest dwarfs among the new T dwarfs identified in the LAS DR1, the T7.5 and the T8.5, might be within the 25 pc limit of nearby stars. Although our spectroscopic follow-up is limited, our estimates of the number density of T dwarfs agree with other studies.</p>
<p>We have demonstrated the capabilities of the UKIDSS LAS and expect to achieve the main scientific drivers set for the survey. The LAS will be able to detect T dwarfs out to ∼80 pc and L dwarfs much further, enabling the study of the scaleheight of field brown dwarfs. Furthermore, the second-epoch coverage in
<italic>J</italic>
will provide proper motions for a large number of candidate L and T dwarfs identified in the LAS, and allow us to identify fainter and more distant objects.</p>
</sec>
</body>
<back>
<fn-group>
<fn id="fn1">
<label>1</label>
<p>
<ext-link ext-link-type="uri" xlink:href="http://spider.ipac.caltech.edu/staff/davy/ARCHIVE/">http://spider.ipac.caltech.edu/staff/davy/ARCHIVE/</ext-link>
, a webpage dedicated to L and T dwarfs maintained by C. Gelino, D. Kirkpatrick and A. Burgasser.</p>
</fn>
<fn id="fn2">
<label>2</label>
<p>Located at
<ext-link ext-link-type="uri" xlink:href="http://surveys.roe.ac.uk/wsa/">http://surveys.roe.ac.uk/wsa/</ext-link>
</p>
</fn>
</fn-group>
<ack>
<p>NL was a post-doctoral research associate funded by the UK PPARC at the University of Leicester where part of this work was carried out. SKL is supported by the Gemini Observatory, which is operated by the Association of Universities for Research in Astronomy, Inc., on behalf of the International Gemini Partnership. MCL acknowledges support for this work from NSF grants AST-0407441 and AST-0507833 and an Alfred P. Sloan Research Fellowship. This research has made use of the Simbad data base of NASA's Astrophysics Data System Bibliographic Services (ADS). Research has benefited from the M, L and T dwarf compendium housed at
<ext-link ext-link-type="uri" xlink:href="DwarfArchives.org">DwarfArchives.org</ext-link>
and maintained by Chris Gelino, Davy Kirkpatrick and Adam Burgasser. The UKIRT is operated by the Joint Astronomy Centre on behalf of the UK Particle Physics and Astronomy Research Council. Based on observations obtained at the Gemini Observatory (program GS-2006B-Q-36), which is operated by the Association of Universities for Research in Astronomy, Inc., under a cooperative agreement with the NSF on behalf of the Gemini partnership: the National Science Foundation (United States), the Particle Physics and Astronomy Research Council (United Kingdom), the National Research Council (Canada), CONICYT (Chile), the Australian Research Council (Australia), CNPq (Brazil) and CONICET (Argentina). The SDSS is managed by the Astrophysical Research Consortium for the Participating Institutions. The Participating Institutions are the American Museum of Natural History, Astrophysical Institute Potsdam, University of Basel, University of Cambridge, Case Western Reserve University, University of Chicago, Drexel University, Fermilab, the Institute for Advanced Study, the Japan Participation Group, Johns Hopkins University, the Joint Institute for Nuclear Astrophysics, the Kavli Institute for Particle Astrophysics and Cosmology, the Korean Scientist Group, the Chinese Academy of Sciences (LAMOST), Los Alamos National Laboratory, the Max-Planck-Institute for Astronomy (MPIA), the Max-Planck-Institute for Astrophysics (MPA), New Mexico State University, Ohio State University, University of Pittsburgh, University of Portsmouth, Princeton University, the United States Naval Observatory and the University of Washington.</p>
</ack>
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<ref id="b45">
<citation citation-type="journal" id="cit45">
<person-group person-group-type="author">
<name>
<surname>Warren</surname>
<given-names>S. J.</given-names>
</name>
<etal></etal>
</person-group>
<year>2007</year>
,
<source>MNRAS</source>
, submitted</citation>
</ref>
<ref id="b46">
<citation citation-type="other" id="cit46">
<person-group person-group-type="author">
<name>
<surname>Warren</surname>
<given-names>S. J.</given-names>
</name>
<etal></etal>
</person-group>
,
<year>2007</year>
, online-only reference (0703037)</citation>
</ref>
</ref-list>
<app-group id="s3">
<title>Appendix</title>
<app id="ss8">
<title>APPENDIX A: SELECTION PROCEDURE FOR T DWARF CANDIDATES IN THE UKIDSS LARGE AREA SURVEY</title>
<p>The set of
<sc>sql</sc>
statements employed to extract lists of reliable point sources with the colours of late-T dwarfs from the WFCAM Science Archive is detailed here. Sufficient reliability was obtained by demanding detection in at least the
<italic>Y</italic>
and
<italic>J</italic>
bands ({Y,J_1}Class > −10), rejecting sources which were classified as noise in any band ({Y,J_1,H,K}Class¡= 0, note that this is different from a null detection which has Class=−9999) and requiring that interband positional offsets are no more than 0.7 arcsec to preclude asteroids which have moved appreciably between exposures. Point sources were selected by demanding MergedClass =−1, and we rejected bright, potentially saturated sources (J_1AperMag3 > = 14.0 mag), in addition to applying a magnitude cut of
<italic>J</italic>
≤ 19 mag. The principal T dwarf selection was simply a pair of colour cuts:
<italic>Y</italic>
<italic>J</italic>
≥ 0.5 and
<italic>J</italic>
<italic>H</italic>
≤ 0.0 (YAperMag3−J_AperMag3 > = 0.5 and J_1AperMag3−HAperMag3 <= 0.0), where, in the case of non-detections, the
<italic>H</italic>
-band magnitude was replaced with the 5σ
<italic>H</italic>
-band point-source limit calculated using the recipe given by
<xref ref-type="bibr" rid="b14">Dye et al. (2006)</xref>
. The candidate list was further trimmed by removing potential cross-talk artefacts (
<xref ref-type="bibr" rid="b14">Dye et al. 2006</xref>
) by rejecting any object up to seven multiples of 51 arcsec away in RA or Dec. from a 2MASS point source with
<italic>J</italic>
≤ 13.5 mag.</p>
</app>
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<title>Eight new T4.5–T7.5 dwarfs discovered in the UKIDSS Large Area Survey Data Release 1*</title>
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<name type="personal">
<namePart type="given">N.</namePart>
<namePart type="family">Lodieu</namePart>
<affiliation>Instituto de Astrofísica de Canarias, Vía Láctea s/n, E-38205 La Laguna, Tenerife, Spain</affiliation>
<affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</affiliation>
<affiliation>E-mail: nlodieu@iac.es</affiliation>
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<affiliation>E-mail: nlodieu@iac.es</affiliation>
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<name type="personal">
<namePart type="given">D. J.</namePart>
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<affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</affiliation>
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</role>
</name>
<name type="personal">
<namePart type="given">S. K.</namePart>
<namePart type="family">Leggett</namePart>
<affiliation>Gemini Observatory, 670 N. A'ohoku Place, Hilo, HI 96720, USA</affiliation>
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</name>
<name type="personal">
<namePart type="given">R. F.</namePart>
<namePart type="family">Jameson</namePart>
<affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</affiliation>
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<name type="personal">
<namePart type="given">D. J.</namePart>
<namePart type="family">Mortlock</namePart>
<affiliation>Astrophysics Group, Imperial College London, Blackett Laboratory, Prince Consort Road, London SW7 2AZ</affiliation>
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<name type="personal">
<namePart type="given">S. J.</namePart>
<namePart type="family">Warren</namePart>
<affiliation>Astrophysics Group, Imperial College London, Blackett Laboratory, Prince Consort Road, London SW7 2AZ</affiliation>
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<namePart type="given">B.</namePart>
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<affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</affiliation>
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<name type="personal">
<namePart type="given">P. W.</namePart>
<namePart type="family">Lucas</namePart>
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<name type="personal">
<namePart type="given">K.</namePart>
<namePart type="family">Chiu</namePart>
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<name type="personal">
<namePart type="given">M. C.</namePart>
<namePart type="family">Liu</namePart>
<affiliation>Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822, USA</affiliation>
<affiliation>‡Alfred P. Sloan Research Fellow.</affiliation>
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<namePart type="family">Venemans</namePart>
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<namePart type="given">R. G.</namePart>
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<namePart type="given">F.</namePart>
<namePart type="family">Allard</namePart>
<affiliation>CRAL, Ecole Normale Supérieure de Lyon, 46 Allée d'Italie, Université de Lyon, F-69364 Lyon Cédex 7, France</affiliation>
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<name type="personal">
<namePart type="given">I.</namePart>
<namePart type="family">Baraffe</namePart>
<affiliation>CRAL, Ecole Normale Supérieure de Lyon, 46 Allée d'Italie, Université de Lyon, F-69364 Lyon Cédex 7, France</affiliation>
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<name type="personal">
<namePart type="given">D. Barrado</namePart>
<namePart type="family">Y Navascués</namePart>
<affiliation>Laboratorio de Astrofísica Espacial y Física Fundamental, INTA, PO Box 50727, E-2808 Madrid, Spain</affiliation>
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<name type="personal">
<namePart type="given">G.</namePart>
<namePart type="family">Carraro</namePart>
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</name>
<name type="personal">
<namePart type="given">S. L.</namePart>
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<affiliation>Department of Physics and Astronomy, University of Leicester, University Road, Leicester LE1 7RH</affiliation>
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<name type="personal">
<namePart type="given">G.</namePart>
<namePart type="family">Chabrier</namePart>
<affiliation>Institute of Astronomy, Madingley Road, Cambridge CB3 0HA</affiliation>
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<roleTerm type="text">author</roleTerm>
</role>
</name>
<name type="personal">
<namePart type="given">R. J.</namePart>
<namePart type="family">Chappelle</namePart>
<affiliation>Astronomical Institute, Academy of Sciences of the Czech Republic, Bocni II/1401a, 141 31 Prague, Czech Republic</affiliation>
<role>
<roleTerm type="text">author</roleTerm>
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</name>
<name type="personal">
<namePart type="given">F.</namePart>
<namePart type="family">Clarke</namePart>
<affiliation>Department of Physics, University of Oxford, Clarendon Laboratory, Parks Road, Oxford OX1 3PU</affiliation>
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<roleTerm type="text">author</roleTerm>
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</name>
<name type="personal">
<namePart type="given">A. C.</namePart>
<namePart type="family">Day-Jones</namePart>
<affiliation>Centre for Astrophysics Research, Science and Technology Research Institute, University of Hertfordshire, Hatfield AL10 9AB</affiliation>
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</name>
<name type="personal">
<namePart type="given">N. R.</namePart>
<namePart type="family">Deacon</namePart>
<affiliation>Department of Astrophysics, Radboud University Nijmegen, PO Box 9010, 6500 GL Nijmegen, the Netherlands</affiliation>
<role>
<roleTerm type="text">author</roleTerm>
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</name>
<name type="personal">
<namePart type="given">P. D.</namePart>
<namePart type="family">Dobbie</namePart>
<affiliation>Anglo-Australian Observatory, PO Box 296, Epping 1710, Australia</affiliation>
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</role>
</name>
<name type="personal">
<namePart type="given">S. L.</namePart>
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<namePart type="given">N. C.</namePart>
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<namePart type="given">T. R.</namePart>
<namePart type="family">Kendall</namePart>
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<roleTerm type="text">author</roleTerm>
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<name type="personal">
<namePart type="given">A.</namePart>
<namePart type="family">Magazzù</namePart>
<affiliation>Fundación Galileo Galilei-INAF, Apartado 565, E-38700 Santa Cruz de La Palma, Spain</affiliation>
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<name type="personal">
<namePart type="given">E. L.</namePart>
<namePart type="family">Martín</namePart>
<affiliation>Instituto de Astrofísica de Canarias, Vía Láctea s/n, E-38205 La Laguna, Tenerife, Spain</affiliation>
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<namePart type="given">M. J.</namePart>
<namePart type="family">McCaughrean</namePart>
<affiliation>School of Physics, University of Exeter, Stocker Road, Exeter, Devon EX4 4QL</affiliation>
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<namePart type="given">T.</namePart>
<namePart type="family">Nakajima</namePart>
<affiliation>National Astronomical Observatory, Mitaka, Tokyo 181-8588, Japan</affiliation>
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<name type="personal">
<namePart type="given">Y.</namePart>
<namePart type="family">Pavlenko</namePart>
<affiliation>Main Astronomical Observatory, National Academy of Sciences, Zabolotnoho 27, Kyiv-127 03680, Ukraine</affiliation>
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<roleTerm type="text">author</roleTerm>
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<name type="personal">
<namePart type="given">M.</namePart>
<namePart type="family">Tamura</namePart>
<affiliation>National Astronomical Observatory, Mitaka, Tokyo 181-8588, Japan</affiliation>
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<roleTerm type="text">author</roleTerm>
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</name>
<name type="personal">
<namePart type="given">C. G.</namePart>
<namePart type="family">Tinney</namePart>
<affiliation>Anglo-Australian Observatory, PO Box 296, Epping 1710, Australia</affiliation>
<role>
<roleTerm type="text">author</roleTerm>
</role>
</name>
<name type="personal">
<namePart type="given">M. R.</namePart>
<namePart type="family">Zapatero Osorio</namePart>
<affiliation>Instituto de Astrofísica de Canarias, Vía Láctea s/n, E-38205 La Laguna, Tenerife, Spain</affiliation>
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<abstract>We present eight new T4.5–T7.5 dwarfs identified in the UKIRT (United Kingdom Infrared Telescope) Infrared Deep Sky Survey (UKIDSS) Large Area Survey (LAS) Data Release 1 (DR1). In addition we have recovered the T4.5 dwarf SDSS J020742.91+000056.2 and the T8.5 dwarf ULAS J003402.77−005206.7. Photometric candidates were picked up in two-colour diagrams over 190 deg2 (DR1) and selected in at least two filters. All candidates exhibit near-infrared spectra with strong methane and water absorption bands characteristic of T dwarfs and the derived spectral types follow the unified scheme of Burgasser et al.. We have found six new T4.5–T5.5 dwarfs, one T7 dwarf, one T7.5 dwarf and recovered a T4.5 dwarf and a T8.5 dwarf. We provide distance estimates which lie in the 15–85 pc range; the T7.5 and T8.5 dwarfs are probably within 25 pc of the Sun. We conclude with a discussion of the number of T dwarfs expected after completion of the LAS, comparing these initial results to theoretical simulations.</abstract>
<note type="footnotes">Based on observations made with the United Kingdom Infrared Telescope, operated by the Joint Astronomy Centre on behalf of the UK Particle Physics and Astronomy Research Council.</note>
<subject>
<genre>keywords</genre>
<topic>techniques: photometric</topic>
<topic>techniques: spectroscopic</topic>
<topic>surveys</topic>
<topic>stars: low-mass, brown dwarfs</topic>
<topic>infrared: stars</topic>
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<identifier type="eISSN">1365-2966</identifier>
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<date>2007</date>
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<caption>vol.</caption>
<number>379</number>
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<caption>no.</caption>
<number>4</number>
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<start>1423</start>
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