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latex/Nucleonics.tex

@@ -306,8 +306,8 @@ \subsection{Controlling nuclear transitions with low frequency
 
 For energy applications, it is necessary to have a type of nuclear
 coupling that's both strong and tuneable. For practical purposes such
-tunability more easily achieved via low frequency stimulation because it
-typically requires smaller and less expensive equipment.
+tunability is more easily achieved via low frequency stimulation because
+it typically requires smaller and less expensive equipment.
 
 Peter Hagelstein \href{https://arxiv.org/abs/1201.4377}{first proposed}
 a novel form of relativistic phonon nuclear coupling in 2012. It relies
@@ -323,20 +323,21 @@ \subsection{Controlling nuclear transitions with low frequency
 \href{https://iopscience.iop.org/article/10.1088/1361-6455/acf3be}{peer
 reviewed in 2023}, it has yet to be experimentally verified.
 
-We propose a nuclear excitation transfer experiment in which we seek to
-observe the spreading out of emission of excited \(\rm ^{57}Fe\) as the
-nuclear energy is transferred from the excited \(\rm ^{57}Fe\) to
-neighbouring ground state \(\rm ^{57}Fe\). The excited nuclei are to
-generated from the decay of \(\rm ^{57}Co\) that's deposited on the
-\(\rm ^{57}Fe\) surface and the phonon coupling is generated via
-stimulation of the surface with a \(\rm THz\) laser.
+We propose to verify relativistic phonon nuclear coupling using a
+nuclear excitation transfer experiment. We'll look to observe the
+spreading out of emission of excited \(\rm ^{57}Fe\) as the nuclear
+energy is transferred from the excited \(\rm ^{57}Fe\) to neighbouring
+ground state \(\rm ^{57}Fe\). The excited nuclei are to generated from
+the decay of \(\rm ^{57}Co\) that's deposited on the \(\rm ^{57}Fe\)
+surface and the phonon coupling is generated via stimulation of the
+surface with a \(\rm THz\) laser.
 
 \subsection{Extracting nuclear energy in benign
 forms}\label{extracting-nuclear-energy-in-benign-forms}
 
 Relativistic phonon nuclear coupling is so strong that experiments will
-be in a form of deep strong coupling regime that was first proposed as
-an academic curiosity in 2010 by
+be operating in a regime sometimes called deep strong coupling. This
+regime was first proposed as an academic curiosity in 2010 by
 \href{https://journals.aps.org/prl/abstract/10.1103/PhysRevLett.105.263603}{Casanova
 at.al} and only recently experimentally observed in ``artificial atoms''
 in \href{https://pubs.acs.org/doi/10.1021/acs.nanolett.7b03103}{2017 by
@@ -345,16 +346,16 @@ \subsection{Extracting nuclear energy in benign
 ``perturbation theory''.
 
 Deep strong coupling allows a free exchange of energy between the
-particles and the field. For the phonon-nuclear system this represents a
-free exchange of nuclear and vibrational energy. This presents an
+particles and the field. For the phonon-nuclear system, this represents
+a free exchange of nuclear and vibrational energy. This presents an
 opportunity to ``bleed off'' nuclear energy into vibrational energy and
 ultimately into heat. It also presents the reverse opportunity to turn
 vibrational energy into nuclear energy, e.g.~creating a controllable
 x-ray laser.
 
 Unlike artificial atoms, deep strong coupling for real atoms and nuclei
 requires a minimum field energy. Electromagnetic coupling is too small
-to make deep strong coupling possible for real atoms and nuclear.
+to make deep strong coupling possible for real atoms and nuclei.
 However, relativistic phonon nuclear coupling is so strong that only a
 very modest field energy of \(\sim \rm 10 \ mJ\) is needed.