By Mott N.F.
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Extra resources for An Outline of Wave Mechanics
22. 23. Experimental arrangement for the measurement of dispersion in atom;c vapors (hook method) sion close to the absorption lines causes interference patterns behind the Mach-Zehnder interferometer, which can be displayed behind a spectrograph as a function of the wavelength A. 4 . 33), which gave the method its name. With simultaneous detection of absorption and dispersion the density Ni of absorbing molecules can be determined. 17]. Such combined techniques have considerably increased the accuracy and relevance of the hook method.
21). 2 Experimental Methods for the Determination of Transition Probabilities The previous section has shown that the spontaneous lifetime of an excited level Ek is determined by the surn of the transition probabilities Akrn of all transitions frorn Ek to lower levels Ern. 39 (V'=17,J'=92)~ -I .. 21. 83) From·measurements of the spontaneous lifetime 'k together with the determination of the relative intensities Ikm/I kO of the different transitions Ek ~ ~ the absoZute transition probabilities Akm can be obtained.
An example for sueh a souree is a hole vlith area dA in a blaekbody radiation eavity. The radiant flux ineident on unit deteetor area is ealled irradianae or flux density [W/m 2] whieh is proportional to the square of the eleetrie field strength. In speetroseopie literature it is often ealled intensity, whieh, however, should not be eonfused with the radiant intensity I * [~J/ster] defined above. 30b) Most deteetors eannot follow the rapid oseillations of the light wave with frequeneies w ~ 10 13 - 10 15 s-l in the visible and ne ar infrared region.