Question

我创建了一个scipy.stats.rv_continuous子类，它似乎正在做我想要的，但它非常慢。代码和测试结果如下。

我使用（断电幂律）的分布函数很容易集成和计算属性，那么是否有另一种内部方法，我应该使用分析值进行子类化以使其更快？文档不清楚rvs是如何实际绘制的，但可能是它找到cdf的倒数。

class Broken_Power_Law(sp.stats.rv_continuous):

    def __init__(self, slopes, breaks, name='Broken_Power_Law'):
        """
        Here `slopes` are the power-law indices for each section, and
        `breaks` are the edges of each section such that `slopes[0]` applies
        between `breaks[0]` and `breaks[1]`, etc.
        """
        super().__init__(a=np.min(breaks), b=np.max(breaks), name=name)
        nums = len(slopes)

        # Calculate the proper normalization of the PDF semi-analytically
        pdf_norms = np.array([np.power(breaks[ii], slopes[ii-1] - slopes[ii]) if ii > 0 else 1.0
                              for ii in range(nums)])
        pdf_norms = np.cumprod(pdf_norms)

        # The additive offsets to calculate CDF values
        cdf_offsets = np.array([(an/(alp+1))*(np.power(breaks[ii+1], alp+1) -
                                              np.power(breaks[ii], alp+1))
                                for ii, (alp, an) in enumerate(zip(slopes, pdf_norms))])

        off_sum = cdf_offsets.sum()
        cdf_offsets = np.cumsum(cdf_offsets)
        pdf_norms /= off_sum
        cdf_offsets /= off_sum

        self.breaks = breaks
        self.slopes = slopes
        self.pdf_norms = pdf_norms
        self.cdf_offsets = cdf_offsets
        self.num_segments = nums
        return

    def _pdf(self, xx):
        mm = np.atleast_1d(xx)
        yy = np.zeros_like(mm)
        # For each power-law, calculate the distribution in that region 
        for ii in range(self.num_segments):
            idx = (self.breaks[ii] < mm) & (mm <= self.breaks[ii+1])
            aa = self.slopes[ii]
            an = self.pdf_norms[ii]
            yy[idx] = an * np.power(mm[idx], aa)

        return yy

    def _cdf(self, xx):
        mm = np.atleast_1d(xx)
        yy = np.zeros_like(mm)
        off = 0.0
        # For each power-law, calculate the cumulative dist in that region
        for ii in range(self.num_segments):
            # incorporate the cumulative offset from previous segments
            off = self.cdf_offsets[ii-1] if ii > 0 else 0.0
            idx = (self.breaks[ii] < mm) & (mm <= self.breaks[ii+1])
            aa = self.slopes[ii]
            an = self.pdf_norms[ii]
            ap1 = aa + 1
            yy[idx] = (an/(ap1)) * (np.power(mm[idx], ap1) - np.power(self.breaks[ii], ap1)) + off

        return yy

测试时：

> test1 = sp.stats.norm()
> %timeit rvs = test1.rvs(size=100)
46.3 µs ± 1.87 µs per loop (mean ± std. dev. of 7 runs, 10000 loops each)

> test2 = Broken_Power_Law([-1.3, -2.2, -2.7], [0.08, 0.5, 1.0, 150.0])
> %timeit rvs = test2.rvs(size=100)
200 ms ± 8.57 ms per loop (mean ± std. dev. of 7 runs, 1 loop each)

即。慢5000倍!!!

Answer 1

一种解决方案是覆盖_rvs方法本身，并使用分析公式使用inverse transform sampling绘制样本：

def _rvs(self, size=None):
    """Invert the CDF (semi)-analytically to draw samples from distribution.
    """
    if size is None:
        size = self._size
    rands = np.random.uniform(size=size)
    samps = np.zeros_like(rands)
    # Go over each segment region, find the region each random-number belongs in based on
    #    the offset values
    for ii in range(self.num_segments):
        lo = self.cdf_offsets[ii]
        hi = self.cdf_offsets[ii+1]
        idx = (lo <= rands) & (rands < hi)

        mlo = self.breaks[ii]
        aa = self.slopes[ii]
        an = self.pdf_norms[ii]
        ap1 = aa + 1

        vals = (ap1/an) * (rands[idx] - lo) + np.power(mlo, ap1)
        samps[idx] = np.power(vals, 1.0/ap1)

    return samps

速度与内置采样几乎相同，

> %timeit rvs = test3.rvs(size=100)
56.8 µs ± 1 µs per loop (mean ± std. dev. of 7 runs, 10000 loops each)

加速scipy自定义连续随机变量

1 个答案: