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rays deflected at certain s have a uniform velocity and how the energy loss is
dependent on the original velocity, the deflection angle, and the ordinal number.
Besides Geiger, Wagner in Munich could probably also be considered for such
Now perhaps I may say something else about the problem, or more correctly, ask
something. If the generated X-rays are defined by the equation
, ought then to be larger, the larger is ; i.e.,
the larger the loss in velocity. Shouldn’t one then expect that be larger, the larger
the deflection s are? That is, that the energy distribution curve of “brems” X-rays
at larger azimuths would have their maxima shifted toward smaller wavelengths?
But Wagner has found precisely the opposite in his
namely, that at
150° the maximum of the bremsstrahlung lies at higher wavelengths than at 90°. Or
else, does this have nothing to do with it because, if one doesn’t calculate classi-
cally, one cannot say anything about the correlation between the orientations of the
deflected cathode rays and the generated X-rays? Additionally, in these cases we
have thick layers again, of course, and therefore summation effects.
Now I beg your forgiveness again for my tardy reply.
I hope you are having a very relaxing time in the countryside and
with best
regards, yours very sincerely,
Lise Meitner.
193. To Lise Meitner
Wustrow, 27 July
Dear Miss Meitner,
Cordial thanks for your kind
I think one should use cathode rays
at high tension, which one generates electrostatically by perhaps using an auto-
matic tension regulator. I have an idea for one. One can certainly obtain
perhaps even more. It must be difficult to get a sufficiently thin diaphragm. If this
is impossible, gas between two diaphragms would have to be used and constantly
= L
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