2002
DOI: 10.1002/qua.10351
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Rosetta Stone of the genetic language

Abstract: ABSTRACT:The paper begins with a guided tour through the history of several major deciphering events in modern science, going from the determination of the wave nature of visible light in the early 19th century, via the discovery of X-rays and their electromagnetic nature around the turn of the 19th century, and onward to the great decipherments of molecular biology of recent times. The central piece of the latter decoding efforts, i.e., the measurement of the X-ray diffraction diagram of DNA, occurred in the … Show more

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Cited by 6 publications
(8 citation statements)
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References 15 publications
(22 reference statements)
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“…The angle of the lines of the X shape (about 40° in Figure 7) equals the angle between the zigzagging, edge on base pairs in A-DNA. In addition, the intensity of the X shape is weak along the lower-order layer lines (3-5) and strong along the higher-order layer lines (6)(7)(8). The reason for this is that the intensity of the X shape is modulated by the envelope of the Thomas Young diffraction of each double slit.…”
Section: Optical Simulationsmentioning
confidence: 99%
“…The angle of the lines of the X shape (about 40° in Figure 7) equals the angle between the zigzagging, edge on base pairs in A-DNA. In addition, the intensity of the X shape is weak along the lower-order layer lines (3-5) and strong along the higher-order layer lines (6)(7)(8). The reason for this is that the intensity of the X shape is modulated by the envelope of the Thomas Young diffraction of each double slit.…”
Section: Optical Simulationsmentioning
confidence: 99%
“…On the other hand, from the same argument, one might expect a nonzero intensity on the meridian of the l = 9 layer-line where x ≈ 3.5, but this happens to be close to the first zero of J 1 (x) at x = 3.8; so, fortuitously, there is no or very weak intensity there for the particular parameters of the phosphorus helix illustrated in figure 6(b). The diffraction pattern is quite sensitive not only to the helix parameters but also to the angular orientation of the atomic helix around its axis [32]. In the numerical simulation of figure 6(b), the intensities have been averaged over the helix angular orientation (as in a gel fibre).…”
Section: Atomic Helixmentioning
confidence: 99%
“…In the simulation of figure 6(c), the layer-lines are projected from the centre of the Ewald sphere corresponding to Cu K α x-rays and indeed they do appear hyperbolic and chirped, as in the real x-ray patterns. A more detailed discussion of the CCV analytical formulae can be found in the original CCV paper [23] and in [32].…”
Section: Atomic Helixmentioning
confidence: 99%
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“…There are several works by A. A. Lucas, Phillipe Lambin, and others that provide complementary historical accounts of these events with less emphasis on the mathematical details of the X-ray diffraction analysis compared to the current work (5)(6)(7). Also, techniques to experimentally demonstrate in the classroom the X-ray diffraction of double helixes or other periodic patterns is outside the scope of this work but can be obtained from the Institute for Chemical Education and their excellent DNA Optical Transform Kit (8).…”
mentioning
confidence: 99%