DATA OF	
Querry M. R., Cary P. G.,  Waring R. C. 1978. Split-pulse laser method for measuring attenuation coefficient of transparent liquids: application to deionized filtered water in the visible region. Appl. Opt. 17, 3587-3592.	

NOTES		
All data have been obtained by the data authors for the following conditions:
water - deionized filtered water
temperature - 26.4 °C
method - the data authors measured the attenuation coefficient, c, with a split-pulse (two-pathlengths) transmission method and subtracted from it the calculated molecular scattering coefficient, bm. Hence, the difference c-bm equals a+bp, where a is the absorption coefficient and bp is the particulate scattering coefficient		
		
Data have been rescaled by Jonasz M. (MJC Optical Technology, www.mjcopticaltech.com) to wavelength in μm and absorption coefficient in 1/m. 

Underscore (_) marks the absence of or incomplete data		
Each column is separated by a TAB - when you import the file into a spreadsheet all column headings should be aligned with the numbers.		

DATA FILE
DATA	DATA	CALC
wave-	bm	a+bp
length		
[um]	[1/m]	[1/m]
		
0.4186	5.015E-03	4.659E-02
0.4219	4.855E-03	4.475E-02
0.4252	4.701E-03	4.420E-02
0.4284	4.557E-03	4.488E-02
0.4317	4.415E-03	4.647E-02
0.4349	4.282E-03	4.547E-02
0.4382	4.150E-03	4.522E-02
0.4415	4.022E-03	4.638E-02
0.4447	3.904E-03	4.656E-02
0.4480	3.786E-03	4.432E-02
0.4504	3.703E-03	3.738E-02
0.4535	3.599E-03	3.993E-02
0.4559	3.521E-03	4.121E-02
0.4583	3.445E-03	3.700E-02
0.4606	3.374E-03	3.503E-02
0.4630	3.302E-03	3.423E-02
0.4654	3.232E-03	3.369E-02
0.4683	3.150E-03	3.761E-02
0.4707	3.084E-03	3.753E-02
0.4730	3.022E-03	3.918E-02
0.4750	2.969E-03	3.592E-02
0.4773	2.910E-03	3.706E-02
0.4796	2.853E-03	3.723E-02
0.4818	2.799E-03	3.701E-02
0.4842	2.742E-03	3.659E-02
0.4866	2.686E-03	3.666E-02
0.4890	2.632E-03	3.656E-02
0.4914	2.578E-03	3.675E-02
0.4938	2.527E-03	3.732E-02
0.4957	2.487E-03	4.125E-02
0.4979	2.441E-03	4.374E-02
0.5003	2.393E-03	4.515E-02
0.5025	2.349E-03	4.796E-02
0.5048	2.305E-03	4.816E-02
0.5072	2.260E-03	5.186E-02
0.5095	2.218E-03	5.440E-02
0.5118	2.177E-03	5.866E-02
0.5142	2.135E-03	5.985E-02
0.5166	2.093E-03	6.490E-02
0.5189	2.055E-03	6.425E-02
0.5212	2.017E-03	6.460E-02
0.5236	1.979E-03	6.524E-02
0.5259	1.943E-03	6.214E-02
0.5282	1.908E-03	6.316E-02
0.5304	1.875E-03	6.365E-02
0.5328	1.840E-03	6.466E-02
0.5350	1.809E-03	6.762E-02
0.5366	1.787E-03	6.672E-02
0.5382	1.764E-03	6.766E-02
0.5397	1.744E-03	7.239E-02
0.5412	1.724E-03	6.962E-02
0.5428	1.703E-03	7.108E-02
0.5443	1.683E-03	7.087E-02
0.5458	1.664E-03	7.013E-02
0.5478	1.639E-03	7.375E-02
0.5501	1.610E-03	7.622E-02
0.5524	1.584E-03	7.836E-02
0.5545	1.560E-03	7.979E-02
0.5568	1.534E-03	8.073E-02
0.5590	1.510E-03	8.163E-02
0.5612	1.487E-03	8.276E-02
0.5634	1.464E-03	8.426E-02
0.5656	1.441E-03	8.604E-02
0.5677	1.420E-03	8.788E-02
0.5700	1.397E-03	8.925E-02
0.5803	1.298E-03	1.072E-01
0.5825	1.278E-03	1.126E-01
0.5846	1.259E-03	1.209E-01
0.5868	1.239E-03	1.311E-01
0.5889	1.220E-03	1.422E-01
0.5910	1.202E-03	1.550E-01
0.5932	1.184E-03	1.686E-01
0.5954	1.166E-03	1.852E-01
0.5975	1.148E-03	2.074E-01
0.5997	1.131E-03	2.361E-01
0.6019	1.114E-03	2.628E-01
0.6040	1.099E-03	2.787E-01
0.6062	1.083E-03	2.854E-01
0.6091	1.063E-03	2.902E-01
0.6112	1.048E-03	2.929E-01
0.6133	1.034E-03	2.949E-01
0.6155	1.019E-03	2.975E-01
0.6176	1.005E-03	3.000E-01
0.6197	9.917E-04	3.018E-01
0.6218	9.784E-04	3.041E-01
0.6239	9.652E-04	3.067E-01
0.6261	9.514E-04	3.101E-01
0.6282	9.381E-04	3.130E-01
0.6303	9.250E-04	3.154E-01
0.6324	9.121E-04	3.191E-01
0.6345	8.995E-04	3.215E-01
0.6367	8.865E-04	3.254E-01
0.6389	8.737E-04	3.274E-01
0.6403	8.657E-04	3.302E-01