| There are a few questions about an "overview," so I'll give that a shot here. This is some imagery I've been using recently, about how our observed signatures are related to crystals. Sometimes physicists think of phase transitions in terms of "symmetry breaking." Imagine zooming in very close on the molecules in a glass of liquid water, all tumbling quickly into and out of your field of view. The situation is highly "symmetric": if you closed your eyes and I shifted the field of view slightly to the left, you wouldn't know what I'd done when you opened your eyes again. Now suppose the water freezes into a crystal of ice, so that the molecules are arranged on a regular lattice. If I repeat my "shift-slightly-to-the-left" experiment, you'd be able to tell I moved things. That is, somehow the molecules chose a particular location for the lattice, even though any other location of the lattice could have done just as well. In jargon, we say the water "spontaneously broke the continuous translational symmetry": the defining equations of motion are agnostic about the particular location in space, but the state of the system chose a location anyways. In our experiment, we do something similar in time rather than space. We drive the system with pulses once every time period "T", so the equations of motion are identical under this "discrete" shift in time. However, the state of the system (in our case, the direction of the nuclear magnetization) only goes back to itself every time 2T, and so "breaks discrete time translational symmetry." There is one more important feature of the observed signature in this analogy: if you nudge an atom that is in a crystal lattice, it will want to return to its original position. Similarly, the period of the magnetization's direction-reversal is robust to our pulse imperfections, if we allow the quantum interactions long enough to act. So, the "region" of parameter space where you can observe this effect is not confined to perfectly ideal pulses, but is instead robust to our pulse imperfections -- the "robustness" depends on the amount of time we allow the nuclear spin interactions to take place. --- I hope this helps. I recommend the synopses available at prl.aps.org, and searching for the PDF preprints on the Arxiv (not yet quite as good as the published versions), if you don't have Physical Review access. --- [Edit for links] [2012 overview] https://physics.aps.org/articles/v5/116 [2013 overview] https://physics.aps.org/articles/v6/31 [2013 quanta mag.] https://www.quantamagazine.org/perpetual-motion-test-could-a... [2017 overviews: "recipe" and first two results] https://physics.aps.org/articles/v10/5 https://www.nature.com/news/the-quest-to-crystallize-time-1.... [2018 announcement] https://physics.aps.org/synopsis-for/10.1103/PhysRevLett.120... [A different background by (the great) Natalie Wolchover of Quanta Mag., which provides context for the original thrust of one branch of this research. Our first significant involvement was after a talk about "Time Translational Symmetry Breaking" by Chetan Nayak of Microsoft's Station Q.] https://www.quantamagazine.org/physicists-aim-to-classify-al... |