Susanne
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doc#116 Otherwise, we go on endlessly trying to draw the line , color and other, as to which kind of man
doc#118 of these measurements. Thus, the dotted line shown in figure 4 was taken as typical
doc#120 as well as nuclear dipole effects lead to line broadening. The lines are asymmetric and
doc#120 employing a Varian model <formul> broad line spectrometer and the associated 12-inch
doc#120 small enough at all times to prevent obvious line shape distortions by saturation effects
doc#120 derived from the mean value of the resonance line , defined as the field about which the first
doc#120 0.3 wt %) as evidenced by a weak resonance line which was very narrow at room temperature
doc#122 was sublimed into a flask on the vacuum line . Previously purified chlorine was subsequently
doc#122 reaction cells on a manifold on a vacuum line . The desired amounts of inactive chlorine
doc#122 likewise condensed in these cells on the vacuum line following which they were frozen down and
doc#122 electrolysis of a <formul> eutectic on the vacuum line , and by exchange of <formul> with molten
doc#123 is the number of <formul> with electron line -density greater than or equal to <formul>
doc#129 In <sect>1 we investigate a new series of line involutions in a projective space of three
doc#129 transformation of the points in which a general line meets a nonsingular quadric surface bearing
doc#129 <formul>. Then in <sect>2 we show that any line involution with the properties that (a)
doc#129 <formul> curve of order k on Q. A general line l meets Q in two points, <formul> and <formul>
doc#129 the corresponding generator meets g The line <formul> is the image of l. Clearly, the
doc#129 involutorial. </p><p> We observe first that no line , l, can meet its image except at one of
doc#129 clear that the only points of Q at which a line can meets its image are the points of g
doc#129 quadratic complex of tangents to Q, each line of which is transformed into the entire