Physalaemus irroratus Cruz, Nascimento & Feio, 2007
publication ID |
https://doi.org/ 10.11646/zootaxa.4725.1.1 |
publication LSID |
lsid:zoobank.org:pub:B137F19A-2C50-476C-8F13-4F049253B361 |
DOI |
https://doi.org/10.5281/zenodo.5583580 |
persistent identifier |
https://treatment.plazi.org/id/D435E640-FFD7-FFEB-BE8B-FE76FEFEFEF5 |
treatment provided by |
Plazi |
scientific name |
Physalaemus irroratus Cruz, Nascimento & Feio, 2007 |
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Physalaemus irroratus Cruz, Nascimento & Feio, 2007
We found a single call type for the species, referred to as call A. The call is composed of a sequence of pulses. There are clear harmonics, and some pulses have PFM, which is synchronic and directly proportional to the slight PAM.
Call A ( Fig. 11 View FIGURE 11 A–F and 4H). We examined two recordings, a total of one minute, with 29 calls from two males. Most of these calls were measured (see Table 2 View TABLE 2 ). Call duration varies from 0.489 to 0.954 s. The call rise and fall durations are similar; both are usually linear-shaped. In some calls, the rise and/or fall can be more abrupt and have a logarithmic shape. The amplitude peak is at around the middle of the call duration, except in calls with very few pulses (e.g., two pulses). Since both rise and fall are similar in slope and duration, the envelope of the call is fairly elliptic ( Fig. 11A, C View FIGURE 11 ). More than 50 % of the call energy is concentrated in 38 % of the call duration around the amplitude peak. The call has a strong PAM (with silence intervals present between pulses; Fig. 11 View FIGURE 11 A–F). The rate of the PAM is ca. 6 Hz, forming ca. four pulses throughout the call. Usually, pulses have an abrupt rise, shorter than fall, which is more gradual, with amplitude peak at the beginning of the pulse ( Fig. 11A, C, D View FIGURE 11 ). However, the first pulses of the longer calls have rises similar to falls and the amplitude peak is at the middle of the pulse. In some calls, the last pulse is clearly shorter than the others. There is a long silence interval between pulses, ca. 5.5 times the pulse duration ( Fig. 11A, C, D View FIGURE 11 ). Some pulses have an internal slight PAM. The call has a harmonic series ( Fig. 4H View FIGURE 4 ). The fundamental frequency is ca. 400 Hz and this band can be present with low energy or absent in the audiospectrograms. The wave periods are regular and then the harmonics are clear throughout the call. However, subharmonics, deterministic chaos, and jumps of the fundamental frequency are observed at the beginning and at the end of the pulses, or even in the entire pulse (usually the last one). Short pulses can be shown as broadband clicks (instantaneously high sound-pressure effect; see Littlejohn 2001) in audiospectrograms at broad filter bandwidth (first pulse in Fig. 11A View FIGURE 11 ). The dominant frequency varies from ca. 1250 to 1720 Hz ( Fig. 11B View FIGURE 11 ). The dominant harmonic varies from the second to the ninth, but it is usually the third or fourth. There is no clear shift in the relative energy among the bands throughout the call. Most of the call energy is between 1300 and 2000 Hz (often, three harmonics). The frequency bands have a general upward FM throughout the call ( Fig. 11B View FIGURE 11 ). There is PFM throughout the call, which is directly proportional to the synchronic pulse-PAM, i.e., each pulse has an up-downward FM ( Fig. 11F View FIGURE 11 ). Additionally, another PFM is present within some pulses and it is directly proportional to the synchronic slight PAM within the pulses.
No known copyright restrictions apply. See Agosti, D., Egloff, W., 2009. Taxonomic information exchange and copyright: the Plazi approach. BMC Research Notes 2009, 2:53 for further explanation.
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