×ばつ 10<SUP>28</SUP> molecules s<SUP>-1</SUP>) was consistent with that measured during other apparitions of 21P/GZ as retrieved from optical, infrared, and radio observations. Our analysis also provided values for rotational temperature (T <SUB>rot</SUB> = 51 ± 3 K) and the abundance ratio of ortho and para spin populations for water (OPR = 2.99 ± 0.23, implying a spin temperature exceeding 50 K). Six Q-branches in the ν<SUB>7</SUB> band of C<SUB>2</SUB>H<SUB>6</SUB> provided a production rate (5.27 ± 0.90 ×ばつ 10<SUP>25</SUP> s<SUP>-1</SUP>) that corresponded to an abundance ratio of 0.136 ± 0.023 ×ばつ 10<SUP>-2</SUP> relative to H<SUB>2</SUB>O, confirming the previously reported strong depletion of C<SUB>2</SUB>H<SUB>6</SUB> from IR observations during the 1998 apparition, and in qualitative agreement with the depletion of C<SUB>2</SUB> known from optical studies of 21P/GZ. For CH<SUB>3</SUB>OH, we applied our recently published quantum model for the ν<SUB>3</SUB> band to obtain a rotational temperature (48<SUP>+10</SUP>/<SUB>-7</SUB> K) consistent with that obtained for H<SUB>2</SUB>O. In addition, we developed a new empirical model for the CH<SUB>3</SUB>OH ν<SUB>2</SUB> band, based on observations of Comet 8P/Tuttle with NIRSPEC. The application of our ν<SUB>2</SUB> model to 21P/GZ yielded a production rate in agreement with that obtained from the ν<SUB>3</SUB> band. Combining results from both ν<SUB>2</SUB> and ν<SUB>3</SUB> bands provided a production rate (47.5 ± 4.4 ×ばつ10<SUP>25</SUP> s<SUP>-1</SUP>) that corresponded to an abundance ratio of 1.22 ± 0.11 ×ばつ 10<SUP>-2</SUP> relative to H<SUB>2</SUB>O in 21P/GZ, indicating mild depletion of CH<SUB>3</SUB>OH. Together with observations of 21P/GZ in 1998, our study provides a measure of primary volatile production rates for this Jupiter family comet over multiple apparitions using high-resolution IR spectroscopy.">
×ばつ 10<SUP>28</SUP> molecules s<SUP>-1</SUP>) was consistent with that measured during other apparitions of 21P/GZ as retrieved from optical, infrared, and radio observations. Our analysis also provided values for rotational temperature (T <SUB>rot</SUB> = 51 ± 3 K) and the abundance ratio of ortho and para spin populations for water (OPR = 2.99 ± 0.23, implying a spin temperature exceeding 50 K). Six Q-branches in the ν<SUB>7</SUB> band of C<SUB>2</SUB>H<SUB>6</SUB> provided a production rate (5.27 ± 0.90 ×ばつ 10<SUP>25</SUP> s<SUP>-1</SUP>) that corresponded to an abundance ratio of 0.136 ± 0.023 ×ばつ 10<SUP>-2</SUP> relative to H<SUB>2</SUB>O, confirming the previously reported strong depletion of C<SUB>2</SUB>H<SUB>6</SUB> from IR observations during the 1998 apparition, and in qualitative agreement with the depletion of C<SUB>2</SUB> known from optical studies of 21P/GZ. For CH<SUB>3</SUB>OH, we applied our recently published quantum model for the ν<SUB>3</SUB> band to obtain a rotational temperature (48<SUP>+10</SUP>/<SUB>-7</SUB> K) consistent with that obtained for H<SUB>2</SUB>O. In addition, we developed a new empirical model for the CH<SUB>3</SUB>OH ν<SUB>2</SUB> band, based on observations of Comet 8P/Tuttle with NIRSPEC. The application of our ν<SUB>2</SUB> model to 21P/GZ yielded a production rate in agreement with that obtained from the ν<SUB>3</SUB> band. Combining results from both ν<SUB>2</SUB> and ν<SUB>3</SUB> bands provided a production rate (47.5 ± 4.4 ×ばつ10<SUP>25</SUP> s<SUP>-1</SUP>) that corresponded to an abundance ratio of 1.22 ± 0.11 ×ばつ 10<SUP>-2</SUP> relative to H<SUB>2</SUB>O in 21P/GZ, indicating mild depletion of CH<SUB>3</SUB>OH. Together with observations of 21P/GZ in 1998, our study provides a measure of primary volatile production rates for this Jupiter family comet over multiple apparitions using high-resolution IR spectroscopy.">
×ばつ 10<SUP>28</SUP> molecules s<SUP>-1</SUP>) was consistent with that measured during other apparitions of 21P/GZ as retrieved from optical, infrared, and radio observations. Our analysis also provided values for rotational temperature (T <SUB>rot</SUB> = 51 ± 3 K) and the abundance ratio of ortho and para spin populations for water (OPR = 2.99 ± 0.23, implying a spin temperature exceeding 50 K). Six Q-branches in the ν<SUB>7</SUB> band of C<SUB>2</SUB>H<SUB>6</SUB> provided a production rate (5.27 ± 0.90 ×ばつ 10<SUP>25</SUP> s<SUP>-1</SUP>) that corresponded to an abundance ratio of 0.136 ± 0.023 ×ばつ 10<SUP>-2</SUP> relative to H<SUB>2</SUB>O, confirming the previously reported strong depletion of C<SUB>2</SUB>H<SUB>6</SUB> from IR observations during the 1998 apparition, and in qualitative agreement with the depletion of C<SUB>2</SUB> known from optical studies of 21P/GZ. For CH<SUB>3</SUB>OH, we applied our recently published quantum model for the ν<SUB>3</SUB> band to obtain a rotational temperature (48<SUP>+10</SUP>/<SUB>-7</SUB> K) consistent with that obtained for H<SUB>2</SUB>O. In addition, we developed a new empirical model for the CH<SUB>3</SUB>OH ν<SUB>2</SUB> band, based on observations of Comet 8P/Tuttle with NIRSPEC. The application of our ν<SUB>2</SUB> model to 21P/GZ yielded a production rate in agreement with that obtained from the ν<SUB>3</SUB> band. Combining results from both ν<SUB>2</SUB> and ν<SUB>3</SUB> bands provided a production rate (47.5 ± 4.4 ×ばつ10<SUP>25</SUP> s<SUP>-1</SUP>) that corresponded to an abundance ratio of 1.22 ± 0.11 ×ばつ 10<SUP>-2</SUP> relative to H<SUB>2</SUB>O in 21P/GZ, indicating mild depletion of CH<SUB>3</SUB>OH. Together with observations of 21P/GZ in 1998, our study provides a measure of primary volatile production rates for this Jupiter family comet over multiple apparitions using high-resolution IR spectroscopy."/>
We obtained infrared spectra of Comet 21P/Giacobini-Zinner (hereafter 21P/GZ) using NIRSPEC at Keck II on UT 2005 June 3, approximately one month before perihelion, that simultaneously sampled H2O, C2H6, and CH3OH. Our production rate for H2O (3.885 ± 0.074 ×ばつ 1028 molecules s-1) was consistent with that measured during other apparitions of 21P/GZ as retrieved from optical, infrared, and radio observations. Our analysis also provided values for rotational temperature (T rot = 51 ± 3 K) and the abundance ratio of ortho and para spin populations for water (OPR = 2.99 ± 0.23, implying a spin temperature exceeding 50 K). Six Q-branches in the ν7 band of C2H6 provided a production rate (5.27 ± 0.90 ×ばつ 1025 s-1) that corresponded to an abundance ratio of 0.136 ± 0.023 ×ばつ 10-2 relative to H2O, confirming the previously reported strong depletion of C2H6 from IR observations during the 1998 apparition, and in qualitative agreement with the depletion of C2 known from optical studies of 21P/GZ. For CH3OH, we applied our recently published quantum model for the ν3 band to obtain a rotational temperature (48+10/-7 K) consistent with that obtained for H2O. In addition, we developed a new empirical model for the CH3OH ν2 band, based on observations of Comet 8P/Tuttle with NIRSPEC. The application of our ν2 model to 21P/GZ yielded a production rate in agreement with that obtained from the ν3 band. Combining results from both ν2 and ν3 bands provided a production rate (47.5 ± 4.4 ×ばつ1025 s-1) that corresponded to an abundance ratio of 1.22 ± 0.11 ×ばつ 10-2 relative to H2O in 21P/GZ, indicating mild depletion of CH3OH. Together with observations of 21P/GZ in 1998, our study provides a measure of primary volatile production rates for this Jupiter family comet over multiple apparitions using high-resolution IR spectroscopy.