350 



66 



Table VII. 



Helium, 3203 A (5 3). 



displ. (J = 1 ; 100 000 Volt/cM) = 0,33 Ä 



Transition 







■^2 



■^3 



i Ä 



Ä" 





K'- 





221 





1 







1 



1 

























113 



-^ 003/ 







1 



1 

























212 



-> 102 





1 



1 







.02 







.000 









311 



-> 201 



I 



1 



1 







.03 







.oOl 









221 



-> 021 



6 



2 











.10 







.010 









212 



012 



g 







L 



Q 



Q 



m 

 .10 



Q 



o09 



(1 





311 



iin 



10 





Q 







17 



.10 



.o29 



o09 



1 ai . 



203 



003/ 



10 



2 



Q 







.15 







.o23 



(J 





302 



^ 102 





9 



(J 







.19 



.13 



.o37 



0I8 





401 



-> 201 



14 





Q 







22 



.20 



.o47 







311 



^ 021 



16 





2 



Q 



Ol 





.oOO 









302 



012 



18 



3 



2 



Q 







Q 



Q 



Q 





401 



-> 111 



20 





-j 







Q 



.01 







oOO 





401 



^ 021 



26 



4 



2 



Q 





















122 



021 



1 



1 







1 



.08 







.006 









113 



— * 012 



3 



1 







1 



.12 







.015 









221 



012/ 



3 



2 



1 



—1 



.05 







.003 









212 



^ 111 \ 



5 



1 







1 



.14 



.10 



.019 



.oil 





104 



—>■ 003 [ 



5 



1 







1 



.18 







.033 









212 



^ 003/ 





2 



1 



"i' 



.04 







.0O2 









203 



^ 102^ 



7 



1 









.20 



.20 



.040 



.039 





311 



102/ 



7 



2 



1 





.07 







.005 







I'erp. 



302 



201 



9 



1 









.18 



.16 



.032 



.o27 



212 



-> 02] 



11 





—1 





.02.5 







.oOl 









203 



^ 012 \ 



13 





-1 























311 



^ 012/ 



13 



3 









.02 







.0OO5 









302 



111\ 



15 



2 



—1 









.015 







0.00 





302 



003/ 



15 



3 









.02 







.nOOô 









401 



^ 102 



17 









.02 



.01 



.0OO5 



.oO(t 





302 



^ 021 



21 



3 





1 





















401 



^ 012 



23 



4 



—1 



—1 



















corresponding to the observed parallel components are 1-2/0.24 = 5,0 and 5,i/o,24 = 21,2 

 respectively, and the values of J corresponding to the observed perpendicular 

 components are 3,7/o,24 = 15,4 and respectively; as regards the outer parallel compo- 

 nents these values are, as seen from fig. 9, where again the positions of the compo- 

 nents observed by Stahk are indicated by arrows, in excellent agreement with the 

 positions of the centres of gravity of the strongest components in the theoretical effect. 

 As regards the two inner parallel components, however, we should, on the theory, 

 rather expect the appearance of a single diffuse line in stead of two separate compo- 



