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Source code for librosa.core.harmonic
#!/usr/bin/env python
# -*- coding: utf-8 -*-
"""Harmonic calculations for frequency representations"""
import warnings
import numpy as np
import scipy.interpolate
import scipy.signal
from ..util.exceptions import ParameterError
from ..util import is_unique
__all__ = ["salience", "interp_harmonics"]
[docs]def salience(
S,
*,
freqs,
harmonics,
weights=None,
aggregate=None,
filter_peaks=True,
fill_value=np.nan,
kind="linear",
axis=-2,
):
"""Harmonic salience function.
Parameters
----------
S : np.ndarray [shape=(..., d, n)]
input time frequency magnitude representation (e.g. STFT or CQT magnitudes).
Must be real-valued and non-negative.
freqs : np.ndarray, shape=(S.shape[axis])
The frequency values corresponding to S's elements along the
chosen axis.
harmonics : list-like, non-negative
Harmonics to include in salience computation. The first harmonic (1)
corresponds to ``S`` itself. Values less than one (e.g., 1/2) correspond
to sub-harmonics.
weights : list-like
The weight to apply to each harmonic in the summation. (default:
uniform weights). Must be the same length as ``harmonics``.
aggregate : function
aggregation function (default: `np.average`)
If ``aggregate=np.average``, then a weighted average is
computed per-harmonic according to the specified weights.
For all other aggregation functions, all harmonics
are treated equally.
filter_peaks : bool
If true, returns harmonic summation only on frequencies of peak
magnitude. Otherwise returns harmonic summation over the full spectrum.
Defaults to True.
fill_value : float
The value to fill non-peaks in the output representation. (default:
`np.nan`) Only used if ``filter_peaks == True``.
kind : str
Interpolation type for harmonic estimation.
See `scipy.interpolate.interp1d`.
axis : int
The axis along which to compute harmonics
Returns
-------
S_sal : np.ndarray
``S_sal`` will have the same shape as ``S``, and measure
the overall harmonic energy at each frequency.
See Also
--------
interp_harmonics
Examples
--------
>>> y, sr = librosa.load(librosa.ex('trumpet'), duration=3)
>>> S = np.abs(librosa.stft(y))
>>> freqs = librosa.fft_frequencies(sr=sr)
>>> harms = [1, 2, 3, 4]
>>> weights = [1.0, 0.5, 0.33, 0.25]
>>> S_sal = librosa.salience(S, freqs=freqs, harmonics=harms, weights=weights, fill_value=0)
>>> print(S_sal.shape)
(1025, 115)
>>> import matplotlib.pyplot as plt
>>> fig, ax = plt.subplots(nrows=2, sharex=True, sharey=True)
>>> librosa.display.specshow(librosa.amplitude_to_db(S, ref=np.max),
... sr=sr, y_axis='log', x_axis='time', ax=ax[0])
>>> ax[0].set(title='Magnitude spectrogram')
>>> ax[0].label_outer()
>>> img = librosa.display.specshow(librosa.amplitude_to_db(S_sal,
... ref=np.max),
... sr=sr, y_axis='log', x_axis='time', ax=ax[1])
>>> ax[1].set(title='Salience spectrogram')
>>> fig.colorbar(img, ax=ax, format="%+2.0f dB")
"""
if aggregate is None:
aggregate = np.average
if weights is None:
weights = np.ones((len(harmonics),))
else:
weights = np.array(weights, dtype=float)
S_harm = interp_harmonics(S, freqs=freqs, harmonics=harmonics, kind=kind, axis=axis)
if aggregate is np.average:
S_sal = aggregate(S_harm, axis=axis - 1, weights=weights)
else:
S_sal = aggregate(S_harm, axis=axis - 1)
if filter_peaks:
S_peaks = scipy.signal.argrelmax(S, axis=axis)
S_out = np.empty(S.shape)
S_out.fill(fill_value)
S_out[S_peaks] = S_sal[S_peaks]
S_sal = S_out
return S_sal
[docs]def interp_harmonics(x, *, freqs, harmonics, kind="linear", fill_value=0, axis=-2):
"""Compute the energy at harmonics of time-frequency representation.
Given a frequency-based energy representation such as a spectrogram
or tempogram, this function computes the energy at the chosen harmonics
of the frequency axis. (See examples below.)
The resulting harmonic array can then be used as input to a salience
computation.
Parameters
----------
x : np.ndarray
The input energy
freqs : np.ndarray, shape=(X.shape[axis])
The frequency values corresponding to X's elements along the
chosen axis.
harmonics : list-like, non-negative
Harmonics to compute as ``harmonics[i] * freqs``.
The first harmonic (1) corresponds to ``freqs``.
Values less than one (e.g., 1/2) correspond to sub-harmonics.
kind : str
Interpolation type. See `scipy.interpolate.interp1d`.
fill_value : float
The value to fill when extrapolating beyond the observed
frequency range.
axis : int
The axis along which to compute harmonics
Returns
-------
x_harm : np.ndarray
``x_harm[i]`` will have the same shape as ``x``, and measure
the energy at the ``harmonics[i]`` harmonic of each frequency.
A new dimension indexing harmonics will be inserted immediately
before ``axis``.
See Also
--------
scipy.interpolate.interp1d
Examples
--------
Estimate the harmonics of a time-averaged tempogram
>>> y, sr = librosa.load(librosa.ex('sweetwaltz'))
>>> # Compute the time-varying tempogram and average over time
>>> tempi = np.mean(librosa.feature.tempogram(y=y, sr=sr), axis=1)
>>> # We'll measure the first five harmonics
>>> harmonics = [1, 2, 3, 4, 5]
>>> f_tempo = librosa.tempo_frequencies(len(tempi), sr=sr)
>>> # Build the harmonic tensor; we only have one axis here (tempo)
>>> t_harmonics = librosa.interp_harmonics(tempi, freqs=f_tempo, harmonics=harmonics, axis=0)
>>> print(t_harmonics.shape)
(5, 384)
>>> # And plot the results
>>> import matplotlib.pyplot as plt
>>> fig, ax = plt.subplots()
>>> librosa.display.specshow(t_harmonics, x_axis='tempo', sr=sr, ax=ax)
>>> ax.set(yticks=np.arange(len(harmonics)),
... yticklabels=['{:.3g}'.format(_) for _ in harmonics],
... ylabel='Harmonic', xlabel='Tempo (BPM)')
We can also compute frequency harmonics for spectrograms.
To calculate sub-harmonic energy, use values < 1.
>>> y, sr = librosa.load(librosa.ex('trumpet'), duration=3)
>>> harmonics = [1./3, 1./2, 1, 2, 3, 4]
>>> S = np.abs(librosa.stft(y))
>>> fft_freqs = librosa.fft_frequencies(sr=sr)
>>> S_harm = librosa.interp_harmonics(S, freqs=fft_freqs, harmonics=harmonics, axis=0)
>>> print(S_harm.shape)
(6, 1025, 646)
>>> fig, ax = plt.subplots(nrows=3, ncols=2, sharex=True, sharey=True)
>>> for i, _sh in enumerate(S_harm):
... img = librosa.display.specshow(librosa.amplitude_to_db(_sh,
... ref=S.max()),
... sr=sr, y_axis='log', x_axis='time',
... ax=ax.flat[i])
... ax.flat[i].set(title='h={:.3g}'.format(harmonics[i]))
... ax.flat[i].label_outer()
>>> fig.colorbar(img, ax=ax, format="%+2.f dB")
"""
if freqs.ndim == 1 and len(freqs) == x.shape[axis]:
# Build the 1-D interpolator.
# All frames have a common domain, so we only need one interpolator here.
# First, verify that the input frequencies are unique
if not is_unique(freqs, axis=0):
warnings.warn(
"Frequencies are not unique. This may produce incorrect harmonic interpolations.",
stacklevel=2,
)
f_interp = scipy.interpolate.interp1d(
freqs,
x,
axis=axis,
bounds_error=False,
copy=False,
kind=kind,
fill_value=fill_value,
)
# Set the interpolation points
f_out = np.multiply.outer(harmonics, freqs)
# Interpolate
return f_interp(f_out)
elif freqs.shape == x.shape:
if not np.all(is_unique(freqs, axis=axis)):
warnings.warn(
"Frequencies are not unique. This may produce incorrect harmonic interpolations.",
stacklevel=2,
)
# If we have time-varying frequencies, then it must match exactly the shape of the input
# We'll define a frame-wise interpolator helper function that we will vectorize over
# the entire input array
def _f_interp(_a, _b):
interp = scipy.interpolate.interp1d(
_a, _b, bounds_error=False, copy=False, kind=kind, fill_value=fill_value
)
return interp(np.multiply.outer(_a, harmonics))
# Signature is expanding frequency into a new dimension
xfunc = np.vectorize(_f_interp, signature="(f),(f)->(f,h)")
# Rotate the vectorizing axis to the tail so that we get parallelism over frames
# Afterward, we're swapping (-1, axis-1) instead of (-1,axis)
# because a new dimension has been inserted
return (
xfunc(freqs.swapaxes(axis, -1), x.swapaxes(axis, -1))
.swapaxes(
# Return the original target axis to its place
-2,
axis,
)
.swapaxes(
# Put the new harmonic axis directly in front of the target axis
-1,
axis - 1,
)
)
else:
raise ParameterError(
"freqs.shape={} does not match "
"input shape={}".format(freqs.shape, x.shape)
)