The New York Stock Exchange in 1909, when money still traveled at the speed of ink. (Scan of a postcard, via Wikimedia Commons, modified to remove captioning.) |
Chaotic oscillator circuit and its response. Component values are as follow: R1 = 46.50 kΩ, R = 14.86 kΩ, R2 = 14.85 kΩ, RE = 14.86 kΩ, RL = 512 Ω, R3 = 14.85 kΩ, C1 = 0.01473 μF, C2 = 0.01483 μF, C3 = 0.01483 μF; D1 and D2 are 1N4148 diodes; the operational amplifiers OP1 and OP2 are LF411CN. The circuit is driven by a four volt, 770 Hz, sine wave. (Image sources: Left, fig. 1, and right, fig. 3, from ref. 6, via arXiv.[7]) |
Power density function for market events. The x-axis is the largest peak value within a burst. (Fig. 2 of ref. 5, via arXiv.[5]) |
"The limitation of our paper is that we haven't shown that our circuit has relevance to the stock market... We aren't yet sure where to look, but for this one simple system, we figured out how to find it."[6]It's hard to publish in Physical Review Letters, and this paper was no exception. Gauthier says that the team needed to allay the concerns of a difficult team of reviewers before it could be published.[6] The research was funded in part by the U.S. Office of Naval Research and the Army Research Office.[6]