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| 1 | +The data are the singing voice measurements from the [DirPat database](https://opendata.iem.at/projects/dirpat/), specifically from the files |
| 2 | + |
| 3 | +* `IR_a_long_sweep.mat` |
| 4 | + |
| 5 | +* `IR_a_closed_sweep.mat` |
| 6 | + |
| 7 | +* `IR_a_open_sweep.mat` |
| 8 | + |
| 9 | +* `IR_a_wide_sweep.mat`. |
| 10 | + |
| 11 | +The calibration data in file `cal64.mat` were applied to all datasets. All directivity models are far-field models referenced to the direction straight ahead and computed as described in |
| 12 | + |
| 13 | +> J. Ahrens and S. Bilbao, “Interpolation and Range Extrapolation of Sound Source Directivity Based on a Spherical Wave Propagation Model,” in Proc. of IEEE ICASSP, Barcelona, Spain, May 2020 |
| 14 | +
|
| 15 | +and |
| 16 | + |
| 17 | +> J. Ahrens and S. Bilbao, “Computation of Spherical Harmonics Based Sound Source Directivity Models from Sparse Measurement Data,” Forum Acusticum, Lyon, France, May 2020. |
| 18 | +
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| 19 | + |
| 20 | + |
| 21 | +Example balloon plots: |
| 22 | + |
| 23 | +`irs_DirPat_a_closed_sweep_N9_non-reg.mat` |
| 24 | + |
| 25 | + |
| 26 | + |
| 27 | +`irs_DirPat_a_closed_sweep_N9_reg.mat` |
| 28 | + |
| 29 | + |
| 30 | + |
| 31 | +`irs_DirPat_a_long_sweep_N9_non-reg.mat` |
| 32 | + |
| 33 | + |
| 34 | + |
| 35 | +`irs_DirPat_a_long_sweep_N9_reg.mat` |
| 36 | + |
| 37 | + |
| 38 | + |
| 39 | +`irs_DirPat_a_open_sweep_N9_non-reg.mat` |
| 40 | + |
| 41 | + |
| 42 | + |
| 43 | +`irs_DirPat_a_open_sweep_N9_reg.mat` |
| 44 | + |
| 45 | + |
| 46 | + |
| 47 | +`irs_DirPat_a_wide_sweep_N9_non-reg.mat` |
| 48 | + |
| 49 | + |
| 50 | + |
| 51 | +`irs_DirPat_a_wide_sweep_N9_reg.mat` |
| 52 | + |
| 53 | + |
| 54 | + |
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