The 2015 edition of the GEISA spectroscopic database

Jonathan Tennyson | Keeyoon Sung | D. Chris Benner | B. A. Voronin | Michael J. Down | Johannes Orphal | Albert A. Ruth | Brian J. Drouin | Shanshan Yu | Holger S. P. Müller | Olga V. Naumenko | E. R. Polovtseva | Robert R. Gamache | Vincent Boudon | Maud Rotger | Jean-Marie Flaud | André Fayt | V. M. Devi | Claus J. Nielsen | Alain Barbe | Nina N. Lavrentieva | Agnes Perrin | A. Chedin | Nicole Jacquinet-Husson | Cyril Crevoisier | Alain Campargue | Antoine Jolly | Andrei V. Nikitin | V. I. Perevalov | Steven T. Massie | Lorenzo Lodi | O. M. Lyulin | D. Jacquemart | L. H. Coudert | Christa Fittschen | Jeremy J. Harrison | R. Armante | J. Vander Auwera | L. Crépeau | Vl.G. Tyuterev | H. Müller | S. Massie | A. Barbe | D. Benner | V. Boudon | L. Brown | L. Coudert | B. Drouin | A. Fayt | J. Harrison | C. Hill | D. Jacquemart | S. Mikhailenko | A. Nikitin | J. Orphal | J. Tennyson | V. Tyuterev | J. Flaud | A. Perrin | A. Chédin | N. Scott | C. Crevoisier | R. Armante | A. Ruth | V. Perevalov | V. Capelle | N. Jacquinet-Husson | J. V. Auwera | L. Lodi | R. R. Gamache | K. Sung | A. Jolly | E. Jiménez | Shanshan Yu | O. Naumenko | C. Fittschen | O. Lyulin | A. Campargue | N. Lavrentieva | J. Buldyreva | A. Predoi‐Cross | An-wen Liu | Shui-Ming Hu | L. Crépeau | C. Boutammine | N. Poulet-Crovisier | M. Rotger | Ø. Hodnebrog | C. Nielsen | Adriana Predoi-Cross | Elena Jiménez | Linda R. Brown | Shui-Ming Hu | Semen Mikhailenko | S. A. Tashkun | Jeanna Buldyreva | An-Wen Liu | Øivind Hodnebrog | S. Tashkun | A. Bouhdaoui | C. Boonne | M. Down | B. Voronin | A. Makie | Christian Hill | N. A. Scott | Cathy Boonne | C. Boutammine | A. Bouhdaoui | V. Capelle | N. Poulet-Crovisier | A. Makie | R. Gamache | E. Polovtseva | M. J. Down | V. Devi | J. Auwera

[1]  J. Pearson,et al.  Modeling the spectrum of the 2ν2 and ν4 states of ammonia to experimental accuracy. , 2016, The Journal of chemical physics.

[2]  J. Pearson,et al.  Far-infrared 14 NH 3 line positions and intensities measured with a FT-IR and AILES beamline, Synchrotron SOLEIL , 2016 .

[3]  A. Chedin,et al.  Evaluation of spectroscopic databases through radiative transfer simulations compared to observations. Application to the validation of GEISA 2015 with IASI and TCCON , 2016 .

[4]  L. Coudert,et al.  Line position and line intensity analyses of the high-resolution spectrum of H218O up to the First Triad and J=17 , 2016 .

[5]  Candice L. Renaud,et al.  A spectral line list for water isotopologues in the 1100–4100 cm−1 region for application to CO2-rich planetary atmospheres , 2016 .

[6]  V. M. Devi,et al.  Spectral line parameters including line shapes in the 2ν3 Q branch of 12CH4 , 2016 .

[7]  J. Tennyson,et al.  A near infrared line list for NH3: Analysis of a Kitt Peak spectrum after 35 years , 2016, 1605.02511.

[8]  S. Tashkun,et al.  A room temperature CO2 line list with ab initio computed intensities , 2016, 1601.05334.

[9]  V. Boudon,et al.  Global analysis of the high temperature infrared emission spectrum of (12)CH4 in the dyad (ν2/ν4) region. , 2016, The Journal of chemical physics.

[10]  R. Acad Institute of Atmospheric Optics , 2016 .

[11]  H. Bouzidi,et al.  Low-Pressure Photolysis of 2,3-Pentanedione in Air: Quantum Yields and Reaction Mechanism. , 2015, The journal of physical chemistry. A.

[12]  A. Campargue,et al.  An empirical line list for methane near 1 µm (9028–10,435 cm−1) , 2015 .

[13]  L. Brown,et al.  The ν17 band of C2H5D from 770 to 880cm−1 , 2015 .

[14]  Vincent Boudon,et al.  Mapping spectroscopic uncertainties into prospective methane retrieval errors from Sentinel-5 and its precursor , 2015 .

[15]  V. M. Devi,et al.  Self- and air-broadened line shapes in the 2ν3 P and R branches of 12CH4 , 2015 .

[16]  P. Bernath,et al.  Relative high-resolution absorption cross sections of C2H6 at low temperatures , 2015 .

[17]  J. Tennyson,et al.  MARVEL analysis of the measured high-resolution spectra of 14NH3 , 2015 .

[18]  D. Jacquemart,et al.  Infrared spectroscopy of 17O- and 18O-enriched carbon dioxide: Line positions and intensities in the 4681–5337 cm−1 region , 2015 .

[19]  J. Hodges,et al.  High accuracy CO2 line intensities determined from theory and experiment , 2015 .

[20]  J. Hodges,et al.  High-Accuracy CO(2) Line Intensities Determined from Theory and Experiment. , 2015, Physical review letters.

[21]  B. Bézard,et al.  Seasonal variations in Titan's middle atmosphere during the northern spring derived from Cassini/CIRS observations , 2015 .

[22]  J. Tennyson,et al.  ExoMol line lists – VIII. A variationally computed line list for hot formaldehyde , 2015, 1506.00172.

[23]  A. Fayt,et al.  Gas phase dicyanoacetylene (C4N2) on Titan: New experimental and theoretical spectroscopy results applied to Cassini CIRS data , 2015 .

[24]  S. Kassi,et al.  An empirical line list for methane in the 1.25 μm transparency window , 2015 .

[25]  J. Lamouroux,et al.  CDSD-296, high resolution carbon dioxide spectroscopic databank: Version for atmospheric applications , 2015 .

[26]  A. Ruth,et al.  The Rotationally-Resolved Absorption Spectrum of Formaldehyde from 6547 to 7051 cm−1 , 2015 .

[27]  V. M. Devi,et al.  An intensity study of the torsional bands of ethane at 35 µm , 2015 .

[28]  B. Drouin,et al.  High resolution spectral analysis of oxygen. IV. Energy levels, partition sums, band constants, RKR potentials, Franck-Condon factors involving the X³Σg⁻, a₁Δg and b¹Σg⁺ states. , 2014, The Journal of chemical physics.

[29]  R. Freedman,et al.  Reliable infrared line lists for 13 CO2 isotopologues up to E′=18,000 cm−1 and 1500 K, with line shape parameters , 2014 .

[30]  D. Jacquemart,et al.  N2-broadening coefficients of methyl chloride: Measurements at room temperature and calculations at atmospheric temperatures , 2014 .

[31]  V. M. Devi,et al.  A cryogenic Herriott cell vacuum-coupled to a Bruker IFS-125HR , 2014 .

[32]  A. Barbe,et al.  Does the "reef structure" at the ozone transition state towards the dissociation exist? New insight from calculations and ultrasensitive spectroscopy experiments. , 2014, Physical review letters.

[33]  L. Coudert,et al.  Analysis of the high-resolution water spectrum up to the Second Triad and to J=30 , 2014 .

[34]  Y. Babikov,et al.  S&MPO – An information system for ozone spectroscopy on the WEB , 2014 .

[35]  L. Manceron,et al.  Revised infrared bending mode intensities for diacetylene (C4H2): Application to Titan , 2014 .

[36]  B. A. Voronin,et al.  Linelist of HD16O for study of atmosphere of terrestrial planets (Earth, Venus and Mars) , 2014 .

[37]  P. Bernath,et al.  IUPAC critical evaluation of the rotational–vibrational spectra of water vapor. Part IV. Energy levels and transition wavenumbers for D216O, D217O, and D218O , 2014 .

[38]  J. Tennyson,et al.  Rotational spectrum of SO3 and theoretical evidence for the formation of sixfold rotational energy-level clusters in its vibrational ground state. , 2014, The Journal of chemical physics.

[39]  V. M. Devi,et al.  Line positions and intensities for the ν12 band of 13C12CH6 , 2014 .

[40]  J. Tennyson,et al.  Rotational Spectrum of SO_3 and Theoretical Evidence for the Formation of Rotational Energy Level Clusters in its Vibrational Ground State , 2014 .

[41]  S. Mikhailenko,et al.  An Accurate and Complete Empirical Line List for Water Vapor Between 5850 and 7920 CM -1 , 2014 .

[42]  Pranay P. Morajkar,et al.  Photolysis of CH₃CHO at 248 nm: evidence of triple fragmentation from primary quantum yield of CH₃ and HCO radicals and H atoms. , 2014, The Journal of chemical physics.

[43]  S. Mikhailenko,et al.  An accurate and complete empirical line list for water vapor between 5850 and 7920 cm−1 , 2014 .

[44]  O. Naumenko,et al.  CW-Cavity Ring Down Spectroscopy of deuterated water in the 1.58 μm atmospheric transparency window , 2014 .

[45]  D. Jacquemart,et al.  Infrared spectroscopy of 17O- and 18O-enriched carbon dioxide: Line positions and intensities in the 3200–4700 cm−1 region. Global modeling of the line positions of 16O12C17O and 17O12C17O , 2014 .

[46]  S. Mikhailenko,et al.  Water vapor line parameters from 6450 to 9400 cm -1 , 2014 .

[47]  S. Tashkun,et al.  High sensitivity Cavity Ring Down spectroscopy of 18O enriched carbon dioxide between 5850 and 7000 cm−1: Part II—Analysis and theoretical modeling of the 12C18O2, 13C18O2 and 16O13C18O spectra , 2014 .

[48]  J. Lamouroux,et al.  An intercomparison of measured pressure-broadening, pressure shifting parameters of carbon dioxide and their temperature dependence , 2014 .

[49]  S. Tashkun,et al.  High sensitivity Cavity Ring Down spectroscopy of 18O enriched carbon dioxide between 5850 and 7000 cm−1: Part III–Analysis and theoretical modeling of the 12C17O2, 16O12C17O, 17O12C18O, 16O13C17O and 17O13C18O spectra , 2014, 1403.5542.

[50]  D. Jacquemart,et al.  Theoretical calculation of self-broadening coefficients for the ν5 band of methyl chloride at various temperatures , 2014 .

[51]  Jonathan Tennyson,et al.  A database of water transitions from experiment and theory (IUPAC Technical Report) , 2014 .

[52]  Jonathan Tennyson,et al.  ExoMol line lists - III. An improved hot rotation-vibration line list for HCN and HNC , 2013, 1311.1328.

[53]  Vincent Guidard,et al.  Towards IASI-New Generation (IASI-NG): impact of improved spectral resolution and radiometric noise on the retrieval of thermodynamic, chemistry and climate variables , 2013 .

[54]  B. Viskolcz,et al.  Absorption spectrum and absolute absorption cross sections of CH3O2 radicals and CH3I molecules in the wavelength range 7473-7497 cm(-1). , 2013, The journal of physical chemistry. A.

[55]  A. Nikitin,et al.  Accurate spectroscopic models for methane polyads derived from a potential energy surface using high-order contact transformations. , 2013, The journal of physical chemistry. A.

[56]  A. A. Azzam,et al.  Terahertz spectroscopy of hydrogen sulfide , 2013 .

[57]  Robert R. Gamache,et al.  Predicting accurate line shape parameters for CO2 transitions , 2013 .

[58]  L. Brown,et al.  Re-analysis of ammonia spectra: Updating the HITRAN 14NH3 database , 2013 .

[59]  J. Buldyreva Air-broadening coefficients of CH335Cl and CH337Cl rovibrational lines and their temperature dependence by a semi-classical approach , 2013 .

[60]  S. Mikhailenko,et al.  An improved line list for water vapor in the 1.5 µm transparency window by highly sensitive CRDS between 5852 and 6607 cm−1 , 2013 .

[61]  A. Barbe,et al.  Ozone spectroscopy in the electronic ground state: high resolution spectra analyses and update of line parameters since 2003 , 2013 .

[62]  J. Harrison Infrared absorption cross sections for trifluoromethane , 2013 .

[63]  V. Perevalov,et al.  High sensitivity Cavity Ring Down spectroscopy of 18O enriched carbon dioxide between 5850 and 7000 cm−1: I. Analysis and theoretical modeling of the 16O12C18O spectrum , 2013 .

[64]  A. Dudaryonok,et al.  CH3Cl self-broadening coefficients and their temperature dependence , 2013 .

[65]  S. Massie,et al.  HITRAN 2012 refractive indices , 2013 .

[66]  V. M. Devi,et al.  Methane line parameters in the HITRAN2012 database , 2013 .

[67]  Ben M. Elliott,et al.  High resolution spectral analysis of oxygen. III. Laboratory investigation of the airglow bands. , 2013, The Journal of chemical physics.

[68]  S. Tashkun,et al.  New analytical model for the ozone electronic ground state potential surface and accurate ab initio vibrational predictions at high energy range. , 2013, The Journal of chemical physics.

[69]  D. Mondelain,et al.  The WKLMC empirical line lists (5852–7919 cm−1) for methane between 80 K and 296 K: “Final” lists for atmospheric and planetary applications , 2013 .

[70]  T. Carrington,et al.  Analysis of the rovibrational spectrum of 13CH4 in the Octad range , 2013 .

[71]  P. Bernath,et al.  ACE-FTS observations of acetonitrile in the lower stratosphere , 2013 .

[72]  Daniel M. Peters,et al.  Measuring volcanic plume and ash properties from space , 2013 .

[73]  V. Boudon,et al.  High resolution spectroscopy and the first global analysis of the Tetradecad region of methane 12CH4. , 2013, Physical chemistry chemical physics : PCCP.

[74]  D. Jacquemart,et al.  Line positions, intensities and self-broadening coefficients for the ν5 band of methyl chloride , 2013 .

[75]  J. Fuglestvedt,et al.  Global warming potentials and radiative efficiencies of halocarbons and related compounds: A comprehensive review , 2013 .

[76]  A. Coustenis,et al.  An improved empirical line list for methane in the region of the 2ν3 band at 1.66 μm , 2013 .

[77]  J. Lamouroux,et al.  The vibrational dependence of half-widths of CO2 transitions broadened by N2, O2, air, and CO2 , 2013 .

[78]  J. Tennyson,et al.  An ab initio variationally computed room-temperature line list for (32)S(16)O3. , 2013, Physical chemistry chemical physics : PCCP.

[79]  D. Jacquemart,et al.  Analysis of self-broadened pure rotational and rovibrational lines of methyl chloride at room temperature , 2013 .

[80]  M. Herman,et al.  16O12C17O and 18O12C17O spectroscopy in the 1.2–1.25 μm region1 , 2013 .

[81]  V. Perevalov,et al.  Cavity ring down spectroscopy of 18O and 17O enriched carbon dioxide near 795 nm , 2013 .

[82]  E. R. Polovtseva,et al.  The HITRAN2012 molecular spectroscopic database , 2013 .

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[84]  P. Bernath,et al.  IUPAC critical evaluation of the rotational-vibrational spectra of water vapor, Part III: Energy levels and transition , 2013 .

[85]  W. J. Lafferty,et al.  Absolute line intensities for ethylene from 1800 to 2350 cm-1. , 2012 .

[86]  J. Orphal,et al.  Analysis of an 18O and D enhanced water spectrum and new assignments for HD18O and D218O in the near-infrared region (6000–7000 cm−1) using newly calculated variational line lists , 2012 .

[87]  Ilse Aben,et al.  Improved water vapour spectroscopy in the 4174-4300 cm-1 region and its impact on SCIAMACHY HDO/H2O measurements , 2012 .

[88]  S. Tashkun,et al.  High sensitivity cavity ring down spectroscopy of 13C16O2 overtone bands near 806nm , 2012 .

[89]  D. Jacquemart,et al.  Infrared spectroscopy of 17O- and 18O-enriched carbon dioxide in the 1700-8300cm-1 wavenumber region , 2012 .

[90]  Pranay P. Morajkar,et al.  Absolute absorption cross sections for two selected lines of formaldehyde around 6625 cm−1 , 2012 .

[91]  S. Mikhailenko,et al.  CRDS of water vapor at 0.1Torr between 6886 and 7406cm-1 , 2012 .

[92]  Peter F. Bernath,et al.  Infrared absorption cross sections for methanol , 2012 .

[93]  A. Nikitin,et al.  Refinements of the WKMC empirical line lists (5852–7919 cm−1) for methane between 80 K and 296 K , 2012 .

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[95]  Robert R. Gamache,et al.  Semiclassical calculations of half-widths and line shifts for transitions in the 30012←00001 and 30013←00001 bands of CO2. III: Self collisions , 2012 .

[96]  G. Orton,et al.  The application of new methane line absorption data to Gemini-N/NIFS and KPNO/FTS observations of Uranus’ near-infrared spectrum , 2012 .

[97]  H. Müller,et al.  High resolution spectral analysis of oxygen. I. Isotopically invariant Dunham fit for the X(3)Σ(g)(-), a(1)Δ(g), b(1)Σ(g)(+) states. , 2012, The Journal of chemical physics.

[98]  H. Müller,et al.  High resolution spectral analysis of oxygen. II. Rotational spectra of a(1)Δ(g)  O2 isotopologues. , 2012, The Journal of chemical physics.

[99]  Robert R. Gamache,et al.  Semiclassical calculations of half-widths and line shifts for transitions in the 30012←00001 and 30013←00001 bands of CO2 II: Collisions with O2 and air , 2012 .

[100]  D. Jacquemart,et al.  N2-broadening coefficients of methyl chloride at room temperature , 2012 .

[101]  J. Tennyson,et al.  Line lists for H218O and H217O based on empirical line positions and ab initio intensities , 2012 .

[102]  A. Fayt,et al.  Frequency and intensity analyses of the far infrared ν5 band system of cyanogen (C2N2) and applications to Titan , 2012 .

[103]  D. Jacquemart,et al.  Infrared spectroscopy of CO2 isotopologues from 2200 to 7000 cm−1: I—Characterizing experimental uncertainties of positions and intensities , 2012 .

[104]  L. Brown,et al.  Extended line positions, intensities, empirical lower state energies and quantum assignments of NH3 from 6300 to 7000 cm−1 , 2012 .

[105]  S. Eliet,et al.  Experimental studies by complementary terahertz techniques and semi-classical calculations of N2- broadening coefficients of CH335Cl , 2012 .

[106]  S. Mikhailenko,et al.  Fourier transform measurements of H218O and HD18O in the spectral range 1000–2300 cm−1 , 2012 .

[107]  A. Barbe,et al.  FTS high resolution spectra of 16O3 in 3500 and 5500 cm−1 regions. First example of new theoretical modelling for a polyad of strongly coupled states , 2012 .

[108]  M. Birk,et al.  Temperature-dependent air broadening of water in the 1250–1750 cm−1 range , 2012 .

[109]  New progress in spectroscopy of ammonia in the infrared 1.5μm range using evolution of spectra from 300 K down to 122 K , 2012 .

[110]  V. M. Devi,et al.  The quest for ozone intensities in the 9–11 μm region: A retrospective , 2012 .

[111]  J. Orphal,et al.  The near infrared cavity-enhanced absorption spectrum of methyl cyanide , 2012 .

[112]  Attila G. Császár,et al.  MARVEL: Measured active rotational–vibrational energy levels. II. Algorithmic improvements☆ , 2012 .

[113]  S. Mikhailenko,et al.  Absorption spectrum of deuterated water vapor enriched by 18 O between 6000 and 9200 cm 1 , 2012 .

[114]  P. Drossart,et al.  An empirical line list for methane in the 1.26–1.71 μm region for planetary investigations (T = 80–300 K). Application to Titan , 2012 .

[115]  E. R. Polovtseva,et al.  Information system for molecular spectroscopy. 5. Ro-vibrational transitions and energy levels of the hydrogen sulfide molecule , 2012 .

[116]  M. Tolbert,et al.  Optical properties of the products of α-dicarbonyl and amine reactions in simulated cloud droplets. , 2012, Environmental science & technology.

[117]  P. Bernath,et al.  First remote sensing observations of trifluoromethane (HFC-23) in the upper troposphere and lower stratosphere , 2012 .

[118]  V. Boudon,et al.  Comparison of line-by-line and band models of near-IR methane absorption applied to outer planet atmospheres , 2012 .

[119]  Sergio A. González,et al.  Laboratory studies of CHF2CF2CH2OH and CF3CF2CH2OH: UV and IR absorption cross sections and OH rate coefficients between 263 and 358 K. , 2012, The journal of physical chemistry. A.

[120]  P. Bernath,et al.  Mid- and long-wave infrared absorption cross sections for acetonitrile , 2012 .

[121]  J. Tennyson,et al.  ExoMol: molecular line lists for exoplanet and other atmospheres , 2012, 1204.0124.

[122]  P. Drossart,et al.  Applications of a new set of methane line parameters to the modeling of Titan’s spectrum in the 1.58 μm window , 2012 .

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[124]  J. Tennyson,et al.  Line lists for H 2 18 O and H 2 17 O based on empirical line positions and ab initio intensities , 2012 .

[125]  D. Mondelain,et al.  The absorption spectrum of methane at 80 and 294 K in the icosad (6717–7589 cm−1): Improved empirical line lists, isotopologue identification and temperature dependence , 2012 .

[126]  L. Brown,et al.  High resolution investigation of the 7 μm region of the ethane spectrum , 2012 .

[127]  L. R. Brown,et al.  PRELIMINARY MODELING OF CH$_3$D FROM 4000 TO 4550 cm$^{-1}$ , 2012 .

[128]  W. J. Lafferty,et al.  The high-resolution infrared spectrum of ethylene in the 1800–2350 cm−1 spectral region , 2011 .

[129]  Shanshan Yu,et al.  O2 A-band line parameters to support atmospheric remote sensing. Part II: The rare isotopologues , 2011 .

[130]  D. Mondelain,et al.  The CH3D absorption spectrum in the 1.58 μm transparency window of methane: Empirical line lists at 81 K and 294 K and temperature dependence , 2011 .

[131]  D. Jacquemart,et al.  The ν1, ν4 and 3ν6 bands of methyl chloride in the 3.4-μm region: Line positions and intensities , 2011 .

[132]  V. M. Devi,et al.  The 2009 edition of the GEISA spectroscopic database , 2011 .

[133]  B. Viskolcz,et al.  Measurement of absolute absorption cross sections for nitrous acid (HONO) in the near-infrared region by the continuous wave cavity ring-down spectroscopy (cw-CRDS) technique coupled to laser photolysis. , 2011, The journal of physical chemistry. A.

[134]  G. Mellau Highly excited rovibrational states of HNC , 2011 .

[135]  I. Gordon,et al.  Revision of spectral parameters for the B- and γ-bands of oxygen and their validation against atmospheric spectra , 2011 .

[136]  S. Mikhailenko,et al.  The absorption spectrum of water in the 1.25 μm transparency window (7408–7920 cm−1) , 2011 .

[137]  P. Bernath,et al.  Acetonitrile (CH3CN) infrared absorption cross sections in the 3 μm region , 2011 .

[138]  G. Villanueva,et al.  Ethane in planetary and cometary atmospheres: Transmittance and fluorescence models of the ν7 band at 3.3 μm , 2011 .

[139]  C. Linke,et al.  Complex refractive indices of Saharan dust samples at visible and near UV wavelengths: a laboratory study , 2011 .

[140]  J. Tennyson,et al.  A global, high accuracy ab initio dipole moment surface for the electronic ground state of the water molecule. , 2011, The Journal of chemical physics.

[141]  G. Mellau Rovibrational eigenenergy structure of the [H,C,N] molecular system. , 2011, The Journal of chemical physics.

[142]  V. M. Devi,et al.  Absolute line intensities and self-broadened half-width coefficients in the ethylene-1- 13 C bands in the 700-1190 cm -1 region , 2011 .

[143]  J. V. Auwera,et al.  Toward the understanding of the high resolution infrared spectrum of C2H6 near 3.3 μm , 2011 .

[144]  I. Gordon,et al.  The a1Δg−X3Σg− band of 16O17O, 17O18O and 17O2 by high sensitivity CRDS near 1.27 μm , 2011 .

[145]  D. Mondelain,et al.  The 1.28 μm transparency window of methane (7541-7919 cm⁻¹): empirical line lists and temperature dependence (80 K-300 K). , 2011, Physical chemistry chemical physics : PCCP.

[146]  S. Kassi,et al.  The 1.58 μm transparency window of methane (6165–6750 cm−1): Empirical line list and temperature dependence between 80 and 296 K , 2011 .

[147]  P. Bernath,et al.  Infrared absorption cross-sections for acetaldehyde (CH3CHO) in the 3 μm region , 2011 .

[148]  Shui-Ming Hu,et al.  High sensitivity cavity ring down spectroscopy of CO2 overtone bands near 790 nm , 2011 .

[149]  P. Bernath,et al.  Mid-infrared absorption cross sections for acetone (propanone) , 2011 .

[150]  S. Mikhailenko,et al.  0 0 0) and (0 1 0) energy levels of the HD18O and D218O molecules from analysis of their ν2 bands , 2011 .

[151]  J. Tennyson,et al.  A variationally computed line list for hot NH3 , 2010, 1011.1569.

[152]  G. Mellau Complete experimental rovibrational eigenenergies of HCN up to 6880 cm(-1) above the ground state. , 2010, The Journal of chemical physics.

[153]  A. Nikitin,et al.  First assignment of the 5ν4 and ν2+4ν4 band systems of 12CH4 in the 6287–6550 cm−1 region , 2011 .

[154]  P. Bernath,et al.  Infrared absorption cross sections for acetone (propanone) in the 3 μm region , 2011 .

[155]  J. Burrows,et al.  The remote sensing of tropospheric composition from space , 2011 .

[156]  M. Antiñolo,et al.  Atmospheric lifetimes and global warming potentials of CF3CH2CH2OH and CF3(CH2)2CH2OH. , 2010, Chemphyschem : a European journal of chemical physics and physical chemistry.

[157]  V. M. Devi,et al.  Multispectrum measurements of spectral line parameters including temperature dependences of N2- and self-broadened half-width coefficients in the region of the ν9 band of 12C2H6 , 2010 .

[158]  Mellau GCh Complete experimental rovibrational eigenenergies of HNC up to 3743 cm(-1) above the ground state. , 2010 .

[159]  S. Mikhailenko,et al.  GOSAT-2009 methane spectral line list in the 5550–6236 cm−1 range , 2010 .

[160]  P. Bernath,et al.  IUPAC Critical Evaluation of the Rotational-Vibrational Spectra of Water Vapor. Part II. Energy Levels and Transition Wavenumbers for HD16O, HD17O, and HD18O , 2010 .

[161]  S. Mikhailenko,et al.  Line positions and energy levels of the 18O substitutions from the HDO/D2O spectra between 5600 and 8800 cm―1 , 2010 .

[162]  I. Gordon,et al.  High sensitivity CRDS of the a1Δg−X3Σg− band of oxygen near 1.27 μm: Extended observations, quadrupole transitions, hot bands and minor isotopologues , 2010 .

[163]  New line intensity measurements for 12C2H2 around 7.7 μm and HITRAN format line list for applications , 2010 .

[164]  Jonathan Tennyson,et al.  HITEMP, the high-temperature molecular spectroscopic database , 2010 .

[165]  V. Tyuterev,et al.  Toward an improved ground state potential energy surface of ozone. , 2010, The journal of physical chemistry. A.

[166]  David A. Long,et al.  O2 A-band line parameters to support atmospheric remote sensing , 2010 .

[167]  S. Kassi,et al.  Empirical line parameters of methane in the 1.63-1.48 μm transparency window by high sensitivity Cavity Ring Down Spectroscopy , 2010 .

[168]  Sara Seager,et al.  Exoplanet Atmospheres: Physical Processes , 2010 .

[169]  Claus Nielsen,et al.  Global Warming Potential of Inhaled Anesthetics: Application to Clinical Use , 2010, Anesthesia and analgesia.

[170]  H. Müller,et al.  Introduction to submillimeter, millimeter and microwave spectral line catalog , 2010 .

[171]  P. Bernath,et al.  Infrared absorption cross sections for propane (C3H8) in the 3 μm region , 2010 .

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