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gateware/dsp: add FIR and test
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artiq/gateware/dsp/fir.py
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artiq/gateware/dsp/fir.py
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from operator import add
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from functools import reduce
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import numpy as np
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from migen import *
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def halfgen4(up, n):
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"""
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http://recycle.lbl.gov/~ldoolitt/halfband
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params:
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* `up` is the stopband width, as a fraction of input sampling rate
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* `n is the order of half-band filter to generate
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returns:
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* `a` is the full set of FIR coefficients, `4*n-1` long.
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implement wisely.
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"""
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npt = n*40
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wmax = 2*np.pi*up
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wfit = (1 - np.linspace(0, 1, npt)[:, None]**2)*wmax
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target = .5*np.ones_like(wfit)
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basis = np.cos(wfit*np.arange(1, 2*n, 2))
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l = np.linalg.pinv(basis)@target
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weight = np.ones_like(wfit)
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for i in range(40):
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err = np.fabs(basis@l - .5)
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weight[err > .99*np.max(err)] *= 1 + 1.5/(i + 11)
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l = np.linalg.pinv(basis*weight)@(target*weight)
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a = np.c_[l, np.zeros_like(l)].ravel()[:-1]
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a = np.r_[a[::-1], 1, a]/2
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return a
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class FIR(Module):
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"""Full-rate finite impulse response filter.
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:param coefficients: integer taps.
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:param width: bit width of input and output.
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:param shift: scale factor (as power of two).
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"""
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def __init__(self, coefficients, width=16, shift=None):
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self.width = width
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self.i = Signal((width, True))
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self.o = Signal((width, True))
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self.latency = (len(coefficients) + 1)//2 + 1
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###
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n = len(coefficients)
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x = [Signal((width, True)) for _ in range(n)]
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self.comb += x[0].eq(self.i)
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self.sync += [x[i + 1].eq(x[i]) for i in range(n - 1)]
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o = []
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for i, c in enumerate(coefficients):
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# simplify for halfband and symmetric filters
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if c == 0 or c in coefficients[:i]:
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continue
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o.append(c*reduce(add, [
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xj for xj, cj in zip(x, coefficients) if cj == c
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]))
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if shift is None:
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shift = width - 1
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self.sync += self.o.eq(reduce(add, o) >> shift)
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78
artiq/test/gateware/test_fir.py
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artiq/test/gateware/test_fir.py
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import numpy as np
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import matplotlib.pyplot as plt
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from migen import *
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from migen.fhdl import verilog
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from artiq.gateware.dsp import fir
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class Transfer(Module):
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def __init__(self, dut):
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self.submodules.dut = dut
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def drive(self, x):
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for xi in x:
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yield self.dut.i.eq(int(xi))
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yield
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def record(self, y):
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for i in range(self.dut.latency):
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yield
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for i in range(len(y)):
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y[i] = (yield self.dut.o)
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yield
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def run(self, samples, amplitude=1.):
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w = 2**(self.dut.width - 1) - 1
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x = np.round(np.random.uniform(
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-amplitude*w, amplitude*w, samples))
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y = np.empty_like(x)
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run_simulation(self, [self.drive(x), self.record(y)],
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vcd_name="fir.vcd")
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x /= w
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y /= w
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return x, y
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def analyze(self, x, y):
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fig, ax = plt.subplots(3)
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ax[0].plot(x, "c-.", label="input")
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ax[0].plot(y, "r-", label="output")
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ax[0].legend(loc="right")
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ax[0].set_xlabel("time (1/fs)")
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ax[0].set_ylabel("signal")
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n = len(x)
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w = np.hanning(n)
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x = (x.reshape(-1, n)*w).sum(0)
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y = (y.reshape(-1, n)*w).sum(0)
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t = (np.fft.rfft(y)/np.fft.rfft(x))
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f = np.fft.rfftfreq(n)*2
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fmin = f[1]
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ax[1].plot(f, 20*np.log10(np.abs(t)), "r-")
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ax[1].set_ylim(-70, 3)
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ax[1].set_xlim(fmin, 1.)
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# ax[1].set_xscale("log")
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ax[1].set_xlabel("frequency (fs/2)")
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ax[1].set_ylabel("magnitude (dB)")
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ax[1].grid(True)
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ax[2].plot(f, np.rad2deg(np.angle(t)), "r-")
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ax[2].set_xlim(fmin, 1.)
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# ax[2].set_xscale("log")
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ax[2].set_xlabel("frequency (fs/2)")
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ax[2].set_ylabel("phase (deg)")
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ax[2].grid(True)
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return fig
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def _main():
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coeff = fir.halfgen4(.4/2, 8)
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coeff_int = [int(round(c * (1 << 16 - 1))) for c in coeff]
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dut = fir.FIR(coeff_int, width=16)
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# print(verilog.convert(dut, ios={dut.i, dut.o}))
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tb = Transfer(dut)
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x, y = tb.run(samples=1 << 10, amplitude=.8)
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tb.analyze(x, y)
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plt.show()
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if __name__ == "__main__":
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_main()
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