Physalaemus signifer (Girard, 1853)
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.5583588 |
persistent identifier |
https://treatment.plazi.org/id/D435E640-FFDF-FFE3-BE8B-FD94FBA8FE15 |
treatment provided by |
Plazi |
scientific name |
Physalaemus signifer (Girard, 1853) |
status |
|
Physalaemus signifer (Girard, 1853)
We found two different calls, referred to as call A and B. Calls B were recorded in agonistic contexts (M. Bilate, personal communication). Calls A and B are composed of harmonics and a single note each. Call B tends to be longer and with lower fundamental frequency than Call A. Calls B have strong FM segments and nonlinear regimes, such as deterministic chaos and subharmonics.
Call A ( Fig. 17 View FIGURE 17 A–L and 13D). We examined 68 recordings, a total of 213 minutes, with ca. 5800 calls from 135 males. Only some of these calls were measured (see Table 2 View TABLE 2 ). Call duration varies from 0.453 to 0.579 s. Call rise and fall are short and usually similar to each other in duration. In some calls, the rise is longer than the fall ( Fig. 17A, C, D, F View FIGURE 17 ). Both can have a linear or exponential shape. There is a long sustain ( Fig. 17A, C, D, E, F, G View FIGURE 17 ). Usually it has a convex shape it can be quite irregular with periods of concave (amplitude valley) and convex shapes ( Fig. 17E, D View FIGURE 17 , respectively). In some calls the rise and the sustain can be fused. The amplitude peak of the call is at around the end of the first four fifths of the call duration ( Fig. 17A, C, E, F View FIGURE 17 ). The envelope of the call can be classified as elliptic ( Fig. 17D View FIGURE 17 ), rectangular ( Fig. 17F, G View FIGURE 17 ), or triangular (pointed left; Fig. 17A, C, E View FIGURE 17 ) depending on the shape of the sustain and position of the amplitude peak in the call. More than 50 % of the call energy is concentrated in 34 % of the call duration around the amplitude peak. Some calls have a slight PAM (there is no silence interval between the amplitude peaks; Fig. 17 C, E, G View FIGURE 17 ). The rate of the PAM is ca. 50 Hz, forming ca. 22 cycles throughout the call. The cycle rise and fall are similar, with amplitude peak at the middle of the cycle. The call has a harmonic series ( Fig. 13D View FIGURE 13 ). The fundamental frequency is ca. 280 Hz and this band can be present with low energy or absent in the audiospectrograms. The wave periods are regular and the harmonics are clear throughout the call. Subharmonics are present at the very end of some calls. The dominant frequency varies from ca. 860 to 1550 Hz ( Fig. 17B View FIGURE 17 ). The dominant harmonic varies from the third to the fifth harmonic, but it is usually the third. There is no clear shift in the relative energy between the bands throughout the call. Most of the call energy is between 700 and 1000 Hz (two harmonics). Usually, the call has a general upward FM with a short downward FM at the end ( Fig. 17B, H, I, J, K, L View FIGURE 17 ). Some calls have an up-downward FM at the beginning, yielding arc-shaped bands in this part of the call ( Fig. 17L View FIGURE 17 ). Additionally, there is PFM throughout the call, which is directly proportional to the synchronic PAM ( Fig. 17C, E, G, H, J, L View FIGURE 17 ).
Call B ( Fig. 17 View FIGURE 17 M–R and 16B). We examined two recordings, a total of eight minutes, with 64 calls from four males. Only some of these calls were measured (see Table 2 View TABLE 2 ). Call duration varies from 0.883 to 1.355 s. Call rise and fall are short and usually similar in duration. In some calls, the rise is longer than the fall. Both can have a linear or exponential shape. There is a long sustain, usually very irregular, with several amplitude peaks ( Fig. 17M, O, P View FIGURE 17 ). The highest amplitude peak is at around the end of the first nine tenths of the call duration (see below; Fig. 17M, O, P View FIGURE 17 ). The envelope of the call can be classified as elliptic, rectangular, or triangular (pointed left; Fig. 17M, O, P View FIGURE 17 ) depending on the shape of the sustain and position of the amplitude peak in the call. More than 50 % of the call energy is concentrated in 40 % of the call duration around the amplitude peak. The call has an irregular PAM (there is no silence interval between the amplitude peaks; Fig. 17M View FIGURE 17 ). Amplitude peaks are variable in intensity and some of them can show high amplitude. Usually, that is the case of the last peak, where the amplitude peak of the call is. The rate of the PAM is ca. 19 Hz even though highly variable, forming ca. 14 peaks throughout the call. The cycle ride and fall are usually similar, with amplitude peak at the middle of the cycle. The call has a harmonic series ( Fig. 16B View FIGURE 16 ). The fundamental frequency is ca. 230 Hz and this band can be present with low energy or absent in the audiospectrograms. Usually the wave periods are regular and harmonics are clear throughout the call. However, some parts of the call can have poorly distinguished harmonics, with considerably deterministic chaos due to the high irregularity of the wave periods ( Fig. 17Q View FIGURE 17 ). Sudden jumps of the fundamental frequency can be present (usually at the end of the call; Fig. 17Q View FIGURE 17 ). Moreover, some calls show subharmonics, usually at their ends ( Fig. 17N View FIGURE 17 ). The dominant frequency varies from ca. 840 to 950 Hz ( Fig. 17N View FIGURE 17 ). The dominant harmonic varies from the third to the fifth harmonic, but it is usually the fourth. There is no clear shift in the relative energy between the bands throughout the call. Most of the call energy is between 600 and 1200 Hz (two or three harmonics). The call has a general upward FM with a short downward FM at the end ( Fig. 17N, Q, R View FIGURE 17 ). Additionally, there is a remarkable PFM throughout the call, which is directly proportional to the synchronic PAM where the latter is present ( Fig. 17 View FIGURE 17 M–R).
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.
Kingdom |
|
Phylum |
|
Class |
|
Order |
|
Family |
|
Genus |