Generator-offset property: Difference between revisions

Inthar (talk | contribs)
Inthar (talk | contribs)
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# from g<sub>1</sub> (...odd # of gens...) g<sub>1</sub> g<sub>3</sub> g<sub>1</sub> (...odd # of gens...) g<sub>1</sub>, we get a<sub>4</sub> = (''r'' + 1)/2 g<sub>1</sub> + (''r'' &minus; 3)/2 g<sub>2</sub> + g<sub>3</sub> ≡ (''r'' &minus; ''n''/2 &minus; 1/2)g<sub>1</sub> + (''r'' &minus; ''n''/2 &minus; 3/2)g<sub>2</sub> mod e.
# from g<sub>1</sub> (...odd # of gens...) g<sub>1</sub> g<sub>3</sub> g<sub>1</sub> (...odd # of gens...) g<sub>1</sub>, we get a<sub>4</sub> = (''r'' + 1)/2 g<sub>1</sub> + (''r'' &minus; 3)/2 g<sub>2</sub> + g<sub>3</sub> ≡ (''r'' &minus; ''n''/2 &minus; 1/2)g<sub>1</sub> + (''r'' &minus; ''n''/2 &minus; 3/2)g<sub>2</sub> mod e.


Choose a tuning where g<sub>1</sub> and g<sub>2</sub> are both very close to but not exactly 1/2*g<sub>0</sub>, resulting in a scale very close to the mos generated by 1/2*g<sub>0</sub> (i.e. g<sub>1</sub> and g<sub>2</sub> differ from 1/2*g<sub>0</sub> by ε, a quantity much smaller than the chroma of the ''n''/2-note mos generated by g<sub>0</sub>, which is |g<sub>3</sub> &minus; g<sub>2</sub>|). Thus we have 4 distinct sizes for ''k''-steps:
These are all distinct by '''Z'''-linear independence. By applying this argument to 1-steps, we see that there must be 4 step sizes in some tuning, a contradiction. Thus g<sub>1</sub> and g<sub>2</sub> must themselves be step sizes. Thus we see that an even-length, unconditionally SV3, GO scale must be of the form (xy)<sup>''r''</sup>xz. (Note that (xy)<sup>''r''</sup>xz is not SV3, since it has only two kinds of 2-steps, xy and xz.) This proves (1).
# a<sub>1</sub>, a<sub>2</sub> and a<sub>3</sub> are clearly distinct.
# a<sub>4</sub> &minus; a<sub>3</sub> = g<sub>1</sub> &minus; g<sub>2</sub> ≠ 0, since the scale is a non-degenerate GO scale.
# a<sub>4</sub> &minus; a<sub>1</sub> = g<sub>3</sub> &minus; g<sub>2</sub> = (g<sub>3</sub> + g<sub>1</sub>) &minus; (g<sub>2</sub> + g<sub>1</sub>) ≠ 0. This is exactly the chroma of the mos generated by g<sub>0</sub>.
# a<sub>4</sub> &minus; a<sub>2</sub> = g<sub>1</sub> &minus; 2g<sub>2</sub> + g<sub>3</sub> = (g<sub>3</sub> &minus; g<sub>2</sub>) + (g<sub>1</sub> &minus; g<sub>2</sub>) = (chroma ± ε) ≠ 0 by choice of tuning.
 
By applying this argument to 1-steps, we see that there must be 4 step sizes in some tuning, a contradiction. Thus g<sub>1</sub> and g<sub>2</sub> must themselves be step sizes. Thus we see that an even-length, unconditionally SV3, GO scale must be of the form (xy)<sup>''r''</sup>xz. (Note that (xy)<sup>''r''</sup>xz is not SV3, since it has only two kinds of 2-steps, xy and xz.) This proves (1).


In case 2, let (2, 1) &minus; (1, 1) = g<sub>1</sub>, (1, 2) &minus; (2, 1) = g<sub>2</sub> be the two alternants. Let g<sub>3</sub> be the leftover generator after stacking alternating g<sub>1</sub> and g<sub>2</sub>. Then the generator circle looks like g<sub>1</sub> g<sub>2</sub> g<sub>1</sub> g<sub>2</sub> ... g<sub>1</sub> g<sub>2</sub> g<sub>3</sub>. Then the combinations of alternants corresponding to a step come in exactly 3 sizes:
In case 2, let (2, 1) &minus; (1, 1) = g<sub>1</sub>, (1, 2) &minus; (2, 1) = g<sub>2</sub> be the two alternants. Let g<sub>3</sub> be the leftover generator after stacking alternating g<sub>1</sub> and g<sub>2</sub>. Then the generator circle looks like g<sub>1</sub> g<sub>2</sub> g<sub>1</sub> g<sub>2</sub> ... g<sub>1</sub> g<sub>2</sub> g<sub>3</sub>. Then the combinations of alternants corresponding to a step come in exactly 3 sizes: