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THE ELECTRONIC WORKS OF GYÖRGY LIGETI AND THEIR ...

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course of Event 2 is the effect of the accelerating entrances discussed in the paragraph<br />

above.<br />

The third event is a large glissando rising to over 4300 Hz, which breaks from the<br />

register of the previous events; this is however the resultant texture, made of the previous<br />

material. While the direction of the whole is clearly upwards, elements of the downward<br />

glissandi introduced in event two are still audible, especially in the first half of this event,<br />

up to 34.6 seconds, where the cross-hatching in the spectrograph is still clearly evident.<br />

An increase in reverberation and the density of the texture obscures any individual<br />

entrances, and the whole is perceived as a single entity, one rising aggregate of noise<br />

bands.<br />

Section B.<br />

Section B begins immediately at 40" at the end of Section A and lasts until 1'24".<br />

While Section A was made of homogeneous material–20 Hz. noise–Section B uses a<br />

variety of different materials; and while Section A expanded upwards in register, Section<br />

B begins in this higher register, from approximately 2000-12,000 Hz, and then begins<br />

filling in the lower register with diverse materials growing in density. This accretion of<br />

material and density is defined by a duration scheme which determines the entrances of<br />

individual events. A quasi-serial matrix then assigns a type of material and register to each<br />

event–the spectrograph in Figure 2.4 labels these events according to Ligeti’s matrix,<br />

which will be explained below.<br />

46

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