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THE ELECTRONIC WORKS OF GYÖRGY LIGETI AND THEIR ...

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etrograde of the louder, denser, and more wide ranging F Section, I will mark one such<br />

R<br />

divisions at 4'54.5", the end of Section F . This span also contains anomalous material,<br />

not generated by the schematic form, in two separate areas.<br />

The striking pizzicato glissando which began the initial B Section is filtered out in<br />

R<br />

the reprise, and the end of Section E (which contains the third and final anomaly)<br />

R<br />

transfers clearly to Section D , which, coinciding with the reprise of the D Section,<br />

R<br />

constitutes a substantial change in material. Thus I will define the span of Section E as<br />

the second major division of Stage 1. These divisions are shown below in a spectrograph<br />

(Figure 2.13).<br />

Retrograde of Section F<br />

The retrograde of Section F is largely audible as such, and while fragmented, it<br />

creates a coherent arch around the midpoint of the piece. Two factors facilitate this<br />

perception, first, the decelerating rhythm of the filtered material which mirrors the<br />

R<br />

acceleration towards the midpoint, and second the registral shape of Section F . The<br />

material of Section F was so diverse and spread through such a wide range, that its<br />

2<br />

retrograde overwhelms the shape of Section A with which it runs concurrently; moreover,<br />

since Section A is shorter than Section F, A’s rise in register is swallowed within the shape<br />

R<br />

of Section F ’s arching descent.<br />

The clipping of material which accelerated through Event 6 of Section F, prepares<br />

the abrupt and interruptive filtering which begins the second half of the piece, and<br />

conversely, the slowly lengthening segments of unfiltered material reverse the accretion<br />

70

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