what about the consistency of absorption coefficients used with different remote sensing instruments...

1
= = C . l . IBI C . l . d ). ( d . A λ λ σ λ WHAT ABOUT THE CONSISTENCY OF ABSORPTION COEFFICIENTS USED WHAT ABOUT THE CONSISTENCY OF ABSORPTION COEFFICIENTS USED WITH DIFFERENT REMOTE SENSING INSTRUMENTS ? WITH DIFFERENT REMOTE SENSING INSTRUMENTS ? Aline Gratien Aline Gratien (1), Bénédicte Picquet-Varrault (1), Jean-François Doussin (1), Matthew S. Johnson (2), Claus (1), Bénédicte Picquet-Varrault (1), Jean-François Doussin (1), Matthew S. Johnson (2), Claus J. Nielsen (3), Johannes Orphal (1) and Jean-Marie Flaud (1) J. Nielsen (3), Johannes Orphal (1) and Jean-Marie Flaud (1) (1) Laboratoire Inter-universitaire des Systèmes Atmosphériques, Créteil, France (1) Laboratoire Inter-universitaire des Systèmes Atmosphériques, Créteil, France (2) (2) Copenhagen Center for Atmospheric Research Copenhagen Center for Atmospheric Research , , University of Copenhagen University of Copenhagen , , Denmark Denmark (3) (3) Centre for Theoretical and Computational Chemistry, Centre for Theoretical and Computational Chemistry, Department of Chemistry, University of Oslo Department of Chemistry, University of Oslo , , Norway Norway INTRODUCTION Cantrell, C. A., Davidson, J. A., McDaniel, A. H., Shetter, R. E. and Calvert, Cantrell, C. A., Davidson, J. A., McDaniel, A. H., Shetter, R. E. and Calvert, J. G. (1990) J. Phys. Chem., 94, 3902-3908. J. G. (1990) J. Phys. Chem., 94, 3902-3908. Gratien, A.; Picquet-Varrault, B.; Orphal, J.; Perraudin, E.; Doussin, J. F.; Gratien, A.; Picquet-Varrault, B.; Orphal, J.; Perraudin, E.; Doussin, J. F.; Flaud, J.-M. Flaud, J.-M. (2007), (2007), Journal of Geophysical Research Journal of Geophysical Research , 112, D05305 , 112, D05305 Gratien, A., E. Nilsson, L. Bache-Andreassen, , J-F. Doussin, M. S. Johnson, . Gratien, A., E. Nilsson, L. Bache-Andreassen, , J-F. Doussin, M. S. Johnson, . J. Nielsen, Y. Stenstrøm and B. Picquet-Varrault. J. Phys. Chem, soumis J. Nielsen, Y. Stenstrøm and B. Picquet-Varrault. J. Phys. Chem, soumis Herndon, S. C., Nelson, D. D. J., Li, Y. and Zahniser, M. S. (2005) J. Quant. Herndon, S. C., Nelson, D. D. J., Li, Y. and Zahniser, M. S. (2005) J. Quant. Radiat. Transfer, 90, 207-216. Radiat. Transfer, 90, 207-216. Hisatsune, C. and Eggers, D. F. (1955) J. Chem. Phys., 23, 487-492. Hisatsune, C. and Eggers, D. F. (1955) J. Chem. Phys., 23, 487-492. Klotz, B., Barnes, I. and Imamura, T. (2004). Phys. Chem. Chem. Phys., 6, 1725- Klotz, B., Barnes, I. and Imamura, T. (2004). Phys. Chem. Chem. Phys., 6, 1725- 1734. 1734. Meller, R. and Moortgat, G. K. (2000) J. Geophys. Res., 105, 7089-7101. Meller, R. and Moortgat, G. K. (2000) J. Geophys. Res., 105, 7089-7101. Nakanaga, T., Kondo, S. and Saëki, S. (1982) J. Chem. Phys., 76, 3860-3865. Nakanaga, T., Kondo, S. and Saëki, S. (1982) J. Chem. Phys., 76, 3860-3865. Orphal, J. and Chance, K. (2003) J. Quant. Radiat. Transfer, 82, 491-504. Orphal, J. and Chance, K. (2003) J. Quant. Radiat. Transfer, 82, 491-504. Rogers, J. D. (1990) J. Phys. Chem., 94, 4011-4015. Rogers, J. D. (1990) J. Phys. Chem., 94, 4011-4015. Sharpe, S. W., Johnson, T. J., Sams, R. L., Chu, P. M., Rhoderick, G. C. and Sharpe, S. W., Johnson, T. J., Sams, R. L., Chu, P. M., Rhoderick, G. C. and Johnson, P. A. (2004) Appl. Spect., 58, 1452-1461. Johnson, P. A. (2004) Appl. Spect., 58, 1452-1461. Optical measurements of atmospheric minor constituents are performed using spectrometers working in the UV-visible, infrared and microwave spectral ranges. The combined use of nadir viewing UV-visible and thermal infrared spectrometers (such as GOME2 and IASI onboard MetOP) will provide an important improvement of vertical trace gas concentration profiles. The analysis and interpretation of the corresponding atmospheric spectra require good knowledge of the molecular parameters of the species of interest as well as of the interfering species. In particular meaningful comparisons of profiles retrieved by various instruments using different spectral domains require that the spectral parameters are consistent in these spectral domains. To illustrate these points we will focuse on formaldehyde. Formaldehyde (HCHO) is the most abundant carbonyl compound in the atmosphere and plays a key role in atmospheric photochemistry in particular for the production of HOx species. Consequently the aim of the study performed at LISA was to intercalibrate formaldehyde spectra in the infrared and ultraviolet regions. This work has been financed by the French National Program for Atmospheric Chemistry (PN LEFE CHAT). EXPERIMENTAL SECTION IBI (2600-3100 cm IBI (2600-3100 cm -1 -1 ) = (2.9 ) = (2.9 0.1).10 0.1).10 -17 -17 cm/molecule cm/molecule IBI (1660-1820 cm IBI (1660-1820 cm -1 -1 ) = (1.31 ) = (1.31 0.04).10 0.04).10 -17 -17 cm/molecule cm/molecule This study Hisatsune and Eggers, 1955 Nakanaga et al., 1982 Sharpe et al., 2004 Klotz et al., 2004 Herndon et al., 2005 IBI (2600-3100 cm - 1 ) 2.9 ± 0.1 2.1 ± 0.9 2.7 ± 0.1 2.8 ± 0.1 IBI (1660-1820 cm - 1 ) 1.31 ± 0.04 0.96 ± 0.20 1.23 ± 0.04 1.28 ± 0.06 1.25 ± 0.13 1.26 ± 0.08 Beer-Lambert law : : CONCLUSION This study present the first simultaneous measurement of the IR and UV cross sections of the formaldehyde and the improved cross sections calibrated using quantitative conversion to CO and HCOOH. This will help in experiments using spectroscopic data, including remote sensing and laboratory kinetics. The IR cross sections are in agreement with the whole of the data IR except Hitsatsune and Eggers,1955 and the UV cross section confirms the databases JPL 2006 and IUPAC 2004 which recommend to use the cross sections of Meller and Moortgat, 2000. ATMOSPHERIC IMPLICATIONS The underestimation of the UV cross-sections of Cantrell et al., 1990 has important consequences on atmospheric chemistry. The data of Cantrell et al., 1990 are recommended to be used in the HITRAN (Orphal and Chance, 2003). Their use may lead to an overestimation of the formaldehyde concentration in atmospheric measurements. Another important consequence is the underestimation of the atmospheric photolysis rates of formaldehyde in photochemical models, which frequently use the cross-sections Experiments were performed in an evacuable Pyrex photoreactor (6 meters length, volume 977 L) at atmospheric pressure and room temperature. The reactor contains two multiple-reflection optical systems interfaced to a Fourier-transform infrared (IR) spectrometer and to an UV-visible absorption spectrometer. The UV and IR optical path lengths were set to 72 m and 12 m, respectively. REACTOR Interface (C .A .D ) Spectrom eter CCD cam era U V fluorescence tubes A rc lam ps Pyrex tube M ain vacuum line A uxiliary vacuum line U V-visible Source Xenon arc lam p FTIR Source :globbar D etector:M C T FTIR U V visible QUANTIFYING HCHO IN THE CELL USING TITRATION BY BROMINE ATOMS HCHO + HO HCHO + HO 2 2 → HOO-CH → HOO-CH 2 O → HO-CH O → HO-CH 2 -OO -OO HO-CH HO-CH 2 -OO + HO -OO + HO 2 HO-CH HO-CH 2 -OOH+O -OOH+O 2 HCOOH HCOOH + O + O 2 + H + H 2 O O 2 2 HO-CH HO-CH 2 -OO -OO HO-CH HO-CH 2 -OH + -OH + HCOOH HCOOH +O +O 2 2 HO-CH 2 HO-CH 2 -O +O -O +O 2 HO-CH HO-CH 2 -O +O -O +O 2 HCOOH HCOOH + HO2 + HO2 HCO + Br HCO + Br 2 HCOBr + Br HCOBr + Br CO CO + HBr + Br + HBr + Br HCO + Br HCO + Br CO CO + HBr + HBr HCO + HBr HCO + HBr HCHO + Br HCHO + Br HCO + HCO HCO + HCO (CHO) (CHO) 2 HCHO + HCHO + CO CO 2 2 CO CO + H + H 2 HCHO + Br HCHO + Br HCO + HBr HCO + HBr HCO + O 2 CO CO + HO + HO 2 Knowing [CO] and [HCOOH] , one can deduce the amount of reacted HCHO. 0,00E+00 2,00E+13 4,00E+13 6,00E+13 8,00E+13 1,00E+14 1,20E+14 1,40E+14 0 1000 2000 3000 4000 5000 6000 7000 8000 tem ps (s) HCHO CO HC O O H first photolysis Second photolysis Titration by bromine atoms COMPARISON WITH THE IBI FROM LITTERATURE This study Mellerand Moortgat,2000 C antrellet al.,1990 R ogers, 1990 IBI (300-360 nm ) 1.17 ± 0.07 1.11 ± 0.05 0.9 ± 0.1 0.95 ± 0.02 IBI IR in 10 -17 cm/molecule IBI UV in 10 -16 cm/molecule There is an excellent consistency between the infrared data except for the one published by Hisatsune and Eggers,1955 for the two bands (2600-3100 cm -1 and 1660-1820 cm -1 ). The UV absorption coefficients of Meller and Moortgat, 2000 are in good agreement with this study. This study shows that the Cantrell et al. ,1990 and Rogers,1990 cross-sections are underestimated by about 20%. The UV absorption coefficients of Meller and Moortgat, 2000 are in very good agreement with independent sets of IR cross-sections except Hisatsune and Eggers,1955 . agreement < 5% disagreement > 5% The experiments were performed by acquiring simultaneously UV and IR spectra using a common optical cell Gas-phase formaldehyde was generated by sublimating paraformaldehyde in a glass vacuum system and introduced in the reactor by flushing with pure nitrogen. By this method, the concentration of formaldehyde (few mbars) in the reactor is not precisely known. UV and IR absorption spectra of formaldehyde were simultaneously recorded and the absorbances A were obtained by calculating A = ln(I 0 /I) IR spectrum (Résolution : 0,08 cm -1 ) UV spectrum (Résolution : 0,18 nm) IBI UV : ultraviolet integrated band intensities with IBI IR : infrared integrated band intensities with According to the Beer-Lambert law : INTERCALIBRATION IR/UV A d d l C UV UV UV × = × × × ν σ ν σ ν UV UV d IBI × = σ ν IR IR d IBI × = A d d l C IR IR IR × = × × × ν σ ν slope = IBI IR /IBI UV IBI IR /IBI UV = 0.246 0.006 (2600-3100 cm -1 ) IBI IR /IBI UV = 0.113 0.003 (1660-1820 cm - 1 ) Experiments were performed in a 250 L electropolished stainless steel smog chamber equipped with a White type multiple reflection mirror system ( IRTF Bruker) IRTF Bruker) with a 120 m optical path length in Oslo to obtain infrared cross sections and to identify potential artefacts. The UV absorption cross sections of the formaldehyde were then derived from these ratios IBI IR /IBI UV and from the infrared cross sections. LISA, Créteil, France IBI (300-360 nm) = (1.17 IBI (300-360 nm) = (1.17 0.07).10 0.07).10 -16 -16 cm/molecule cm/molecule The infrared cross sections of formaldehyde were determined by quantifying HCHO in the cell using titration by bromine atoms. Complementary experiments in Oslo Examples of formaldehyde spectra acquired simultaneously IR versus UV integrated optical depths of HCHO. Infrared Integrated Band Intensities Contact: [email protected]

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Page 1: WHAT ABOUT THE CONSISTENCY OF ABSORPTION COEFFICIENTS USED WITH DIFFERENT REMOTE SENSING INSTRUMENTS ? Aline Gratien (1), Bénédicte Picquet-Varrault (1),

∫ ∫ == C.l.IBIC.l.d).(d.A λλσλ

WHAT ABOUT THE CONSISTENCY OF ABSORPTION COEFFICIENTS WHAT ABOUT THE CONSISTENCY OF ABSORPTION COEFFICIENTS USED WITH DIFFERENT REMOTE SENSING INSTRUMENTS ?USED WITH DIFFERENT REMOTE SENSING INSTRUMENTS ?

Aline GratienAline Gratien (1), Bénédicte Picquet-Varrault (1), Jean-François Doussin (1), Matthew S. Johnson (2), Claus J. Nielsen (3), Johannes (1), Bénédicte Picquet-Varrault (1), Jean-François Doussin (1), Matthew S. Johnson (2), Claus J. Nielsen (3), Johannes Orphal (1) and Jean-Marie Flaud (1)Orphal (1) and Jean-Marie Flaud (1)

(1) Laboratoire Inter-universitaire des Systèmes Atmosphériques, Créteil, France (1) Laboratoire Inter-universitaire des Systèmes Atmosphériques, Créteil, France (2) (2) Copenhagen Center for Atmospheric ResearchCopenhagen Center for Atmospheric Research , , University of CopenhagenUniversity of Copenhagen , , DenmarkDenmark

(3) (3) Centre for Theoretical and Computational Chemistry, Centre for Theoretical and Computational Chemistry, Department of Chemistry, University of OsloDepartment of Chemistry, University of Oslo , , NorwayNorway

INTRODUCTION

Cantrell, C. A., Davidson, J. A., McDaniel, A. H., Shetter, R. E. and Calvert, J. G. (1990) J. Phys. Chem., Cantrell, C. A., Davidson, J. A., McDaniel, A. H., Shetter, R. E. and Calvert, J. G. (1990) J. Phys. Chem., 94, 3902-3908. 94, 3902-3908. Gratien, A.; Picquet-Varrault, B.; Orphal, J.; Perraudin, E.; Doussin, J. F.; Flaud, J.-M. Gratien, A.; Picquet-Varrault, B.; Orphal, J.; Perraudin, E.; Doussin, J. F.; Flaud, J.-M. (2007),(2007), Journal of Journal of Geophysical ResearchGeophysical Research, 112, D05305, 112, D05305 Gratien, A., E. Nilsson, L. Bache-Andreassen, , J-F. Doussin, M. S.  Johnson, . J.  Nielsen, Y. Stenstrøm Gratien, A., E. Nilsson, L. Bache-Andreassen, , J-F. Doussin, M. S.  Johnson, . J.  Nielsen, Y. Stenstrøm and B. Picquet-Varrault. J. Phys. Chem, soumisand B. Picquet-Varrault. J. Phys. Chem, soumisHerndon, S. C., Nelson, D. D. J., Li, Y. and Zahniser, M. S. (2005) J. Quant. Radiat. Transfer, 90, 207-216.Herndon, S. C., Nelson, D. D. J., Li, Y. and Zahniser, M. S. (2005) J. Quant. Radiat. Transfer, 90, 207-216.Hisatsune, C. and Eggers, D. F. (1955) J. Chem. Phys., 23, 487-492.Hisatsune, C. and Eggers, D. F. (1955) J. Chem. Phys., 23, 487-492.Klotz, B., Barnes, I. and Imamura, T. (2004). Phys. Chem. Chem. Phys., 6, 1725-1734.Klotz, B., Barnes, I. and Imamura, T. (2004). Phys. Chem. Chem. Phys., 6, 1725-1734.Meller, R. and Moortgat, G. K. (2000) J. Geophys. Res., 105, 7089-7101.Meller, R. and Moortgat, G. K. (2000) J. Geophys. Res., 105, 7089-7101.Nakanaga, T., Kondo, S. and Saëki, S. (1982) J. Chem. Phys., 76, 3860-3865.Nakanaga, T., Kondo, S. and Saëki, S. (1982) J. Chem. Phys., 76, 3860-3865.Orphal, J. and Chance, K. (2003) J. Quant. Radiat. Transfer, 82, 491-504.Orphal, J. and Chance, K. (2003) J. Quant. Radiat. Transfer, 82, 491-504.Rogers, J. D. (1990) J. Phys. Chem., 94, 4011-4015.Rogers, J. D. (1990) J. Phys. Chem., 94, 4011-4015.Sharpe, S. W., Johnson, T. J., Sams, R. L., Chu, P. M., Rhoderick, G. C. and Johnson, P. A. (2004) Appl. Sharpe, S. W., Johnson, T. J., Sams, R. L., Chu, P. M., Rhoderick, G. C. and Johnson, P. A. (2004) Appl. Spect., 58, 1452-1461.Spect., 58, 1452-1461.

Optical measurements of atmospheric minor constituents are performed using spectrometers working in the UV-visible, infrared and microwave spectral ranges. The combined use of nadir viewing UV-visible and thermal infrared spectrometers (such as GOME2 and IASI onboard MetOP) will provide an important improvement of vertical trace gas concentration profiles. The analysis and interpretation of the corresponding atmospheric spectra require good knowledge of the molecular parameters of the species of interest as well as of the interfering species. In particular meaningful comparisons of profiles retrieved by various instruments using different spectral domains require that the spectral parameters are consistent in these spectral domains. To illustrate these points we will focuse on formaldehyde. Formaldehyde (HCHO) is the most abundant carbonyl compound in the atmosphere and plays a key role in atmospheric photochemistry in particular for the production of HOx species. Consequently the aim of the study performed at LISA was to intercalibrate formaldehyde spectra in the infrared and ultraviolet regions. This work has been financed by the French National Program for Atmospheric Chemistry (PN LEFE CHAT).

EXPERIMENTAL SECTION

IBI (2600-3100 cmIBI (2600-3100 cm-1-1) = (2.9 ) = (2.9 0.1).10 0.1).10-17-17 cm/molecule cm/molecule

IBI (1660-1820 cmIBI (1660-1820 cm-1-1) = (1.31 ) = (1.31 0.04).10 0.04).10-17-17 cm/molecule cm/molecule

This studyHisatsune

and Eggers, 1955

Nakanaga et al., 1982

Sharpe et al., 2004

Klotz et al., 2004

Herndon et al., 2005

IBI (2600-3100 cm-1) 2.9 ± 0.1 2.1 ± 0.9 2.7 ± 0.1 2.8 ± 0.1    

IBI (1660-1820 cm-1) 1.31 ± 0.04 0.96 ± 0.20 1.23 ± 0.04 1.28 ± 0.06 1.25 ± 0.13 1.26 ± 0.08

Beer-Lambert law ::

CONCLUSIONThis study present the first simultaneous measurement of the IR and UV cross sections of the formaldehyde and the improved cross sections calibrated using quantitative conversion to CO and HCOOH. This will help in experiments using spectroscopic data, including remote sensing and laboratory kinetics.

The IR cross sections are in agreement with the whole of the data IR except Hitsatsune and Eggers,1955 and the UV cross section confirms the databases JPL 2006 and IUPAC 2004 which recommend to use the cross sections of Meller and Moortgat, 2000.

ATMOSPHERIC IMPLICATIONSThe underestimation of the UV cross-sections of Cantrell et al., 1990 has important consequences on atmospheric chemistry.

The data of Cantrell et al., 1990 are recommended to be used in the HITRAN (Orphal and Chance, 2003). Their use may lead to an overestimation of the formaldehyde concentration in atmospheric measurements.

Another important consequence is the underestimation of the atmospheric photolysis rates of formaldehyde in photochemical models, which frequently use the cross-sections published by Cantrell, 1990.

Experiments were performed in an evacuable Pyrex photoreactor (6 meters length, volume 977 L) at atmospheric pressure and room temperature.

The reactor contains two multiple-reflection optical systems interfaced to a Fourier-transform infrared (IR) spectrometer and to an UV-visible absorption spectrometer.

The UV and IR optical path lengths were set to 72 m and 12 m, respectively.

REACTOR

Interface ( C.A.D)

SpectrometerCCD camera

UV fluorescencetubesArc lamps

Pyrex tube

Main vacuum line Auxiliary vacuum line

UV-visible Source Xenon arc lamp

FTIR

Source : globbar

Detector : MCT

FTIRUV visible

QUANTIFYING HCHO IN THE CELL USING TITRATION BY BROMINE ATOMS

HCHO + HOHCHO + HO2 2 → HOO-CH → HOO-CH

22O → HO-CHO → HO-CH22-OO-OO

HO-CHHO-CH

22-OO + HO-OO + HO22 →→ HO-CHHO-CH

22-OOH+O-OOH+O22

→→ HCOOHHCOOH + O + O22 + H + H

22OO

2 2 HO-CHHO-CH22-OO-OO →→ HO-CHHO-CH

22-OH + -OH + HCOOHHCOOH

+O+O22

→→ 2 HO-CH2 HO-CH22-O +O-O +O

22

HO-CHHO-CH22-O +O-O +O

22 →→ HCOOHHCOOH + HO2 + HO2

HCO + BrHCO + Br22 →→ HCOBr + BrHCOBr + Br

   →→ COCO + HBr + Br + HBr + Br

HCO + BrHCO + Br →→ COCO + HBr + HBr

HCO + HBrHCO + HBr →→ HCHO + BrHCHO + Br

HCO + HCOHCO + HCO→→ (CHO)(CHO)22

   →→ HCHO + HCHO + COCO

   →→ 2 2 COCO + H + H22

HCHO + BrHCHO + Br → HCO + HBrHCO + HBr

HCO + O2 COCO + HO + HO22→

Knowing [CO] and [HCOOH] , one can

deduce the amount of reacted HCHO.

0,00E+00

2,00E+13

4,00E+13

6,00E+13

8,00E+13

1,00E+14

1,20E+14

1,40E+14

0 1000 2000 3000 4000 5000 6000 7000 8000

temps (s)

concentration (molecule/cm

3)

HCHO

CO

HCOOH

first photolysis Second photolysis

Titration by bromine atoms

COMPARISON WITH THE IBI FROM LITTERATURE

This studyMeller and

Moortgat, 2000Cantrell et al., 1990

Rogers, 1990

IBI (300-360 nm) 1.17 ± 0.07 1.11 ± 0.05 0.9 ± 0.1 0.95 ± 0.02

IBIIR in 10-17 cm/molecule

IBIUV in 10-16 cm/molecule

There is an excellent consistency between the infrared data except for the one published by Hisatsune and Eggers,1955 for the two bands (2600-3100 cm-1 and 1660-1820 cm-1).

The UV absorption coefficients of Meller and Moortgat, 2000 are in good agreement with this study.

This study shows that the Cantrell et al. ,1990 and Rogers,1990 cross-sections are underestimated by about 20%.

The UV absorption coefficients of Meller and Moortgat, 2000 are in very good agreement with independent sets of IR cross-sections except Hisatsune and Eggers,1955 .

agreement < 5% disagreement > 5%

The experiments were performed by acquiring simultaneously UV and IR spectra using a common optical cell

Gas-phase formaldehyde was generated by sublimating paraformaldehyde in a glass vacuum system and introduced in the reactor by flushing with pure nitrogen. By this method, the concentration of formaldehyde (few mbars) in the reactor is not precisely known. UV and IR absorption spectra of formaldehyde were simultaneously recorded and the absorbances A were obtained by calculating A = ln(I0/I)

IR spectrum (Résolution : 0,08 cm-1) UV spectrum (Résolution : 0,18 nm)

IBIUV : ultraviolet integrated band intensities

with

IBIIR: infrared integrated band intensities

with

According to the Beer-Lambert law :

INTERCALIBRATION IR/UV

A d d l CUV UV UV× = × × ×∫ ∫ν σ ν σ νUV UV d IBI× =∫

σ νIR IR d IBI× =∫A d d l CIR IR IR× = × × ×∫ ∫ν σ ν

slope = IBIIR/IBIUV

IBIIR/IBIUV = 0.246 0.006 (2600-3100 cm-1)

IBIIR/IBIUV = 0.113 0.003 (1660-1820 cm-1)

Experiments were performed in a 250 L electropolished stainless steel smog chamber equipped with a White type multiple reflection mirror system ( IRTF IRTF Bruker)Bruker) with a 120 m optical path length in Oslo to obtain infrared cross sections and to identify potential artefacts.

The UV absorption cross sections of the formaldehyde were then derived from these ratios IBIIR/IBIUV and from the infrared cross sections.

LISA, Créteil, France

IBI (300-360 nm) = (1.17 IBI (300-360 nm) = (1.17 0.07).10 0.07).10-16-16 cm/molecule cm/molecule

The infrared cross sections of formaldehyde were determined by quantifying HCHO in the cell using titration by bromine atoms.

Complementary experiments in Oslo

Examples of formaldehyde spectra acquired simultaneously

IR versus UV integrated optical depths of HCHO.

Infrared Integrated Band Intensities

Contact: [email protected]