The Secret Harmony of Primes. Sam Vaseghi
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where
means that
In the early 90s, documentarian George Csicsery created a documentary called ‘N Is a Number’ that captured the life and work of the grand mathematician Paul Erdös. Conversely, when I saw this movie for the first time in 2013, Csicsery’s beautiful title inspired me to look in exactly the opposite direction, to better understand the properties of natural numbers, namely to look at
One crucial difference between a phenomenological mathematical approach and a pure mathematical approach is that a ‘natural phenomenon’ can be mathematically modelled as a phenomenon while a sequence in number theory is, as such, mathematically ‘defined’ by pure mathematics.
One challenge, however, that I encountered in my work was that studying
Figure 1.3: In the early 90s, documentarian George Csicsery created a documentary called ‘N Is a Number’ that captured the life and work of the grand mathematician Erdös.
In the early 90s, when I was a student at the University of Stuttgart and a scholar to Herman Haken, the renowned laser physicist and the founder of the theory of synergetics (the thory of self-organisation), I was fascinated with learning how to translate complex systems of different natural phenomena, independent of their disciplinary origin – physics, biology, sociology etc. – into comprehensive mathematical models. The theory of synergetics provides a fundamental paradigm that helps us to understand how patterns are formed and recognised in nature: the laser.
Synergetics tells us that, similar to laser light that can be regarded as a composition of fundamental waves, many patterns in nature can be scattered into interacting fundamental waves, known as elementary modes. When scattering a system into elementary modes, a spectrum appears that helps us to better understand the elementary structural properties of that pattern or system and how it behaves.
Figure 1.4: Weaving scheme for textile design. A two-dimensional pattern decomposed into vertical and horisontal elementary modes.
However, when we break a system into its elementary modes, like a child decomposing a Lego house into its basic elements, we lose the object as a whole, and we cannot identify a real state of the system as a whole because we have decomposed it: the toy is only present in pieces. This means that, at a certain point in time, we can EITHER have the toy house as decomposed into pieces (and observe/understand how it was composed), OR as one complete house (without an understanding of its details, but observing it as a whole).
Figure 1.5: Position x and momentum p wavefunctions corresponding to quantum particles. The opacity (%) of the particles corresponds to the probability density of finding the particle with position x or momentum component p. Top: If wavelength λ is unknown, so is momentum p, wave-vector k and energy E (de Broglie relations). As the particle is more localised in position space, Δx is smaller than for Δpx. Bottom: If λ is known, so are p, k, and E. As the particle is more localised in momentum space, Δp is smaller than Δx.5
Physicists have identified a general concept of ‘duality’ and ‘uncertainty’ through so called Fourier analysis, which is specifically known in the field of quantum physics as the Heisenberg Uncertainty Principle: when we want to fix the position and state of a specific particle, we cannot have it decomposed into waves – and vice versa: if we like it decomposed into waves, we cannot fix its position and state as a particle.
In physics, a particle can be understood as a probability wave. The amplitude of the wave roughly represents the probability of finding a particle in a given place, while the frequency of the wave roughly represents the particle’s state in terms of momentum (mass × velocity). If we imagine a localised particle as a short pulse, rather than a wave, the reason we cannot know its precise position and momentum is because we can’t make an infinitely short pulse out of a single frequency.
Figure 1.6: Katsushika Hokusai (1760-1849) created this extraordinary picture around 1831. It is known as ‘The Great Wave of Kanagawa.’ It is a fairly small colour woodcut. The foam of the wave is breaking into claws, which grasp for the fishermen.
Bearing in mind that
The more we study
Indeed, as we will show later, one could deduce a similar type of duality as for particles and waves in physics: