I used to think that all nuclei have fixed intrinsic value of the nuclear spin quantum number, $I$. For example, $\ce{^1H}$ must have a nuclear spin of $\frac{1}{2}$, $\ce{^{14}N}$ must have a nuclear spin of 1 and so on.
Not until I study Mossbauer spectroscopy, in which the transition involved is the excitation from $I = \frac{1}{2}$ to $I = \frac{3}{2}$ of $\ce{^{57}Fe}$ nuclei. It is the $I$ that got changed, not the $m_I$ as in typical NMR!
Source: Wikipedia, Mossbauer Spectroscopy
How can the $I$ of a nuclear species be changed? It was just as weird as changing the mass of a particle, which is an intrinsic property. Any insight will be appreciated.
Since the spin of nuclei can be changed, is it also possible to change the spin, $s = \frac{1}{2}$ of an electron, if given high enough energy?
$\ce{^57Fe}$
$\ce{^57Fe}$ instead of$^{57}$Fe
$^{57}$Fe. The latter looks correct, but the alignment of superscripts might not be entirely correct (depending on e.g. fonts), and (more importantly) if you resize your window the Fe may be shifted to the next line (see example here). Using MathJax to typeset the entire nuclide symbol avoids this issue, and is probably a bit easier to keep track of mentally anyway. $\endgroup$