D in D2O

 D(D2O)    GA         EVAL-DEC69 KOPPEL,HOUSTON                   
 REF.1 (1978)         DIST-MAY10                       20100309   
----JENDL-4.0         MATERIAL   11                               
-----THERMAL NEUTRON SCATTERING DATA                              
------ENDF-6 FORMAT                                               
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 The data were taken from ENDF/B-VI.8.                            
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 TEMPERATURES = 296 350 400 450 500 600 800 1000 DEG K.           
                                                                  
 HISTORY                                                          
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 THIS EVALUATION WAS PRODUCED AT GENERAL ATOMIC IN 1969 USING     
 THE GA CODE GASKET  (SEE REF.1).  IT WAS CONVERTED               
 TO ENDF-6 FORMAT AT LOS ALAMOS IN 1989.  THE ONLY CHANGES        
 MADE TO THE CONTENTS WERE ADJUSTMENTS OF CROSS SECTIONS          
 TO MATCH THE ENDF/B-VI VALUES.                                   
                                                                  
 THEORY                                                           
 ------                                                           
 WHEREAS HYDROGEN IS NEARLY A COMPLETELY INCOHERENT NEUTRON       
 SCATTERER, THE SCATTERERING FROM DEUTERIUM IS LARGELY COHERENT.  
 ALTHOUGH IT WOULD APPEAR THAT DUE TO THIS FACT A TREATMENT       
 OF D2O ANALOGOUS TO THE ONE USED FOR H2O WOULD BE INADEQUATE,    
 CALCULATIONS (REF. 2) HAVE SHOWN THAT BECAUSE OF A GREAT DEAL    
 OF CANCELLATION BETWEEN INTER AND INTRA-MOLECULAR INTERFERENCE   
 SCATTERING, INTEGRAL QUANTITIES LIKE THE TOTAL CROSS SECTION     
 OR THERMAL NEUTRON SPECTRA CAN ACTUALLY BE PREDICTED QUITE       
 ACCURATELY WITH AN INCOHERENT MODEL.                             
                                                                  
 THEREFORE, THE SCATTERING LAW FOR D2O IS BASED ON A MODEL        
 QUITE SIMILAR TO THE ONE USED FOR THE GA EVALUATION OF H2O;      
 NAMELY, FREELY RECOILING D2O MOLECULES OF MASS 20.  EACH         
 MOLECULE CAN UNDERGO TORSIONAL HARMONIC OSCILLATIONS (HINDERED   
 ROTATIONS) WITH A BROAD SPECTRUM OF DISTRIBUTED MODES.  BETWEEN  
 0.025 AND 0.127 EV, THE ROTATION SPECTRUM IS TAKEN FROM THE      
 WORK OF HAYWOOD (REF. 3) JOINED TO A QUADRATIC LAW BELOW         
 0.025 EV.  IN ADDITION, THERE ARE TWO INTERNAL VIBRATIONS AT     
 FREQUENCIES OF 0.142 AND 0.305 EV (THE FREQUENCIES ARE           
 APPROXIMATELY 1/SQRT(2) TIMES THE CORRESPONDING FREQUENCIES      
 FOR H2O AS EXPECTED FROM THE MASS RATIO) WITH MASSES OF 6 AND    
 3, RESPECTIVELY.  THE TORSIONAL BAND IS NORMALIZED TO A MASS     
 OF 20/9.  THE SCATTERING BY THE OXYGEN ATOMS IS NOT INCLUDED     
 IN THE TABULATED SCATTERING LAW DATA.  IT SHOULD BE TAKEN INTO   
 ACCOUNT BY ADDING THE THE SCATTERING FOR FREE OXYGEN OF          
 MASS 16.                                                         
                                                                  
 REFERENCES                                                       
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 1. J.U.KOPPEL AND D.H.HOUSTON, REFERENCE MANUAL FOR ENDF         
    THERMAL NEUTRON SCATTERING DATA, GENERAL ATOMIC REPORT        
    GA-8774 REVISED AND REISSUED AS ENDF-269 BY THE NATIONAL      
    NUCLEAR DATA CENTER, JULY 1978.                               
 2. J.U.KOPPEL AND J.A.YOUNG, NUKLEONIK 7, 408(1965).             
 3. B.C.HAYWOOD, "PROC. IAEA SYMP. ON PULSED NEUTRON RESEARCH",   
    KARLSRUHE, VOL. i, P.434(1965).