A singly charged ion of a hypothetical element has two lines studied across four even…

PHYSICS · Multi-part · Fermi University Physics · Scientific Practice & Experimental Methods · Atomic, Molecular & Optical Physics · One-electron atoms and the origins of atomic structure

Deriving the Spectrum, Ch Hyperfine structure and isotope shifts

Problem

A singly charged ion of a hypothetical element has two lines studied across four even isotopes, with atomic masses M40=39.9626 uM_{40} = 39.9626\,\mathrm{u}, M42=41.9586 uM_{42} = 41.9586\,\mathrm{u}, M44=43.9555 uM_{44} = 43.9555\,\mathrm{u} and M48=47.9525 uM_{48} = 47.9525\,\mathrm{u}. Line 1 has frequency ν1=755.22 THz\nu_1 = 755.22\,\mathrm{THz} and line 2 has ν2=346.00 THz\nu_2 = 346.00\,\mathrm{THz}. Each isotope shift is δν=ν(M′)−ν(M)\delta\nu = \nu(M') - \nu(M), with M=M40M = M_{40} and M′M' the heavier isotope of the pair: Data: pair (40,42)(40,42) has δν1=450.8 MHz\delta\nu_1=450.8\,\mathrm{MHz} and δν2=242.2 MHz\delta\nu_2=242.2\,\mathrm{MHz}; pair (40,44)(40,44) has δν1=894.6 MHz\delta\nu_1=894.6\,\mathrm{MHz} and δν2=448.1 MHz\delta\nu_2=448.1\,\mathrm{MHz}; pair (40,48)(40,48) has δν1=1756.3 MHz\delta\nu_1=1756.3\,\mathrm{MHz} and δν2=772.4 MHz\delta\nu_2=772.4\,\mathrm{MHz}. Take me=5.4858×10−4 um_e = 5.4858\times10^{-4}\,\mathrm{u}, and use the atomic masses as the masses MM in the normal-mass-shift formula. ((a)) For each pair and each line, subtract the normal mass shift and form the modified shift δνmod\delta\nu^{\rm mod}, in GHz u\mathrm{GHz\,u}. ((b)) Draw the King line through the (40,42)(40, 42) and (40,48)(40, 48) points, with line 1 on the horizontal axis. Give its slope F2/F1\mathcal{F}_2/\mathcal{F}_1 and its intercept in GHz u\mathrm{GHz\,u}, and check whether the (40,44)(40, 44) point lies on it within the rounding of the data. ((c)) An atomic-structure calculation gives line 1 the constants F1=−280 MHz fm−2\mathcal{F}_1 = -280\,\mathrm{MHz\,fm^{-2}} and K1=15.0 GHz u\mathcal{K}_1 = 15.0\,\mathrm{GHz\,u}. Find the change in mean square charge radius, δ⟨r2⟩\delta\langle r^2\rangle, between isotopes 40 and 48.

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