diff --git a/etc/tests/test_distributions.py b/etc/tests/test_distributions.py
index 9740051..884e8f2 100644
--- a/etc/tests/test_distributions.py
+++ b/etc/tests/test_distributions.py
@@ -7,7 +7,7 @@ import os
 
 sys.path.insert(0, os.path.join(os.path.dirname(__file__), ".."))
 
-from tools.distributions import k_dist, lognakagami, loggamma_dist
+from tools.distributions import k_dist, lognakagami, loggamma_dist, lograyleigh, logrice
 
 
 X = np.linspace(0.01, 10.0, 500)
@@ -340,6 +340,180 @@ class TestLogGamma:
         assert pytest.approx(samples.mean(), rel=5e-2) == expected_mean
 
 
+# ── lograyleigh unit tests ────────────────────────────────────────────────────
+
+
+class TestLogRayleigh:
+    def test_logpdf_is_finite_on_real_line(self):
+        """logpdf must be finite for all real y — tests positivity without float64 underflow."""
+        log_vals = lograyleigh.logpdf(Y, sigma=2.0)
+        assert np.all(np.isfinite(log_vals))
+
+    def test_pdf_integrates_to_one(self):
+        """Numerical integral of PDF over the real line should be ≈ 1."""
+        y_fine = np.linspace(-20, 10, 200_000)
+        integral = np.trapezoid(lograyleigh.pdf(y_fine, sigma=2.0), y_fine)
+        assert pytest.approx(integral, abs=1e-3) == 1.0
+
+    def test_logpdf_equals_log_pdf(self):
+        """logpdf must equal log(pdf) at points where pdf does not underflow."""
+        y_bulk = np.linspace(-5.0, 2.0, 50)
+        log_via_pdf = np.log(lograyleigh.pdf(y_bulk, sigma=2.0))
+        log_direct = lograyleigh.logpdf(y_bulk, sigma=2.0)
+        np.testing.assert_allclose(log_direct, log_via_pdf, rtol=1e-6)
+
+    def test_cdf_is_monotone_increasing(self):
+        """CDF must be strictly non-decreasing."""
+        cdf_vals = lograyleigh.cdf(Y, sigma=2.0)
+        assert np.all(np.diff(cdf_vals) >= 0)
+
+    def test_cdf_and_sf_sum_to_one(self):
+        """CDF + SF must equal 1 at every point."""
+        cdf_vals = lograyleigh.cdf(Y, sigma=2.0)
+        sf_vals = lograyleigh.sf(Y, sigma=2.0)
+        np.testing.assert_allclose(cdf_vals + sf_vals, 1.0, atol=1e-12)
+
+    def test_ppf_inverts_cdf(self):
+        """ppf(cdf(y)) must recover y."""
+        y_test = np.array([-2.0, 0.0, 1.0])
+        cdf_vals = lograyleigh.cdf(y_test, sigma=2.0)
+        np.testing.assert_allclose(lograyleigh.ppf(cdf_vals, sigma=2.0), y_test, atol=1e-8)
+
+    def test_isf_inverts_sf(self):
+        """isf(sf(y)) must recover y."""
+        y_test = np.array([-1.0, 0.5, 1.5])
+        sf_vals = lograyleigh.sf(y_test, sigma=2.0)
+        np.testing.assert_allclose(lograyleigh.isf(sf_vals, sigma=2.0), y_test, atol=1e-8)
+
+    def test_argcheck_rejects_non_positive_sigma(self):
+        """sigma <= 0 must not produce a valid (positive-finite) PDF value."""
+        val = lograyleigh.pdf(0.0, sigma=-1.0)
+        assert not (np.isfinite(val) and val > 0)
+
+    def test_stats_mean(self):
+        """Analytical mean must equal 0.5 * (log(2*sigma^2) + digamma(1))."""
+        sigma = 2.0
+        expected_mean = 0.5 * (np.log(2.0 * sigma**2) + sc.digamma(1))
+        dist_mean = float(lograyleigh.stats(sigma=sigma, moments="m"))
+        assert pytest.approx(dist_mean, rel=1e-10) == expected_mean
+
+    def test_stats_mean_shifts_with_sigma(self):
+        """Changing sigma shifts the mean by log(sigma2/sigma1) and leaves variance unchanged."""
+        mean1 = float(lograyleigh.stats(sigma=1.0, moments="m"))
+        mean4 = float(lograyleigh.stats(sigma=4.0, moments="m"))
+        assert pytest.approx(mean4 - mean1, rel=1e-10) == np.log(4.0)
+
+    def test_stats_variance_equals_pi_squared_over_24(self):
+        """Variance must equal pi^2/24 and be independent of sigma."""
+        expected_var = np.pi**2 / 24.0
+        for sigma in [0.5, 1.0, 3.0]:
+            _, dist_var, *_ = lograyleigh.stats(sigma=sigma, moments="mv")
+            assert pytest.approx(float(dist_var), rel=1e-10) == expected_var
+
+    def test_log_transform_relation_to_rayleigh(self):
+        """lograyleigh.pdf(y) must equal rayleigh.pdf(exp(y)) * exp(y) (change-of-variable)."""
+        from scipy.stats import rayleigh
+
+        y_test = np.linspace(-3.0, 3.0, 20)
+        sigma = 2.0
+        direct = lograyleigh.pdf(y_test, sigma=sigma)
+        via_rayleigh = rayleigh.pdf(np.exp(y_test), scale=sigma) * np.exp(y_test)
+        np.testing.assert_allclose(direct, via_rayleigh, rtol=1e-6)
+
+    def test_rvs_samples_are_finite(self):
+        """Random samples must be finite real numbers."""
+        rng = np.random.default_rng(42)
+        samples = lograyleigh.rvs(sigma=2.0, size=200, random_state=rng)
+        assert samples.shape == (200,)
+        assert np.all(np.isfinite(samples))
+
+    def test_rvs_sample_mean_near_expected(self):
+        """Sample mean of many RVS should be close to the distribution mean."""
+        sigma = 2.0
+        rng = np.random.default_rng(0)
+        samples = lograyleigh.rvs(sigma=sigma, size=50_000, random_state=rng)
+        expected_mean = float(lograyleigh.stats(sigma=sigma, moments="m"))
+        assert pytest.approx(samples.mean(), rel=5e-2) == expected_mean
+
+
+# ── logrice unit tests ────────────────────────────────────────────────────────
+
+
+class TestLogRice:
+    def test_logpdf_is_finite_on_real_line(self):
+        """logpdf must be finite for all real y — tests positivity without float64 underflow."""
+        log_vals = logrice.logpdf(Y, nu=1.0, sigma=2.0)
+        assert np.all(np.isfinite(log_vals))
+
+    def test_pdf_integrates_to_one(self):
+        """Numerical integral of PDF over the real line should be ≈ 1."""
+        y_fine = np.linspace(-20, 10, 200_000)
+        integral = np.trapezoid(logrice.pdf(y_fine, nu=1.0, sigma=2.0), y_fine)
+        assert pytest.approx(integral, abs=1e-3) == 1.0
+
+    def test_logpdf_equals_log_pdf(self):
+        """logpdf must equal log(pdf) at points where pdf does not underflow."""
+        y_bulk = np.linspace(-5.0, 2.0, 50)
+        log_via_pdf = np.log(logrice.pdf(y_bulk, nu=1.0, sigma=2.0))
+        log_direct = logrice.logpdf(y_bulk, nu=1.0, sigma=2.0)
+        np.testing.assert_allclose(log_direct, log_via_pdf, rtol=1e-6)
+
+    def test_cdf_is_monotone_increasing(self):
+        """CDF must be strictly non-decreasing."""
+        cdf_vals = logrice.cdf(Y, nu=1.0, sigma=2.0)
+        assert np.all(np.diff(cdf_vals) >= 0)
+
+    def test_cdf_and_sf_sum_to_one(self):
+        """CDF + SF must equal 1 at every point."""
+        cdf_vals = logrice.cdf(Y, nu=1.0, sigma=2.0)
+        sf_vals = logrice.sf(Y, nu=1.0, sigma=2.0)
+        np.testing.assert_allclose(cdf_vals + sf_vals, 1.0, atol=1e-12)
+
+    def test_argcheck_rejects_negative_nu(self):
+        """nu < 0 must not produce a valid (positive-finite) PDF value."""
+        val = logrice.pdf(0.0, nu=-1.0, sigma=2.0)
+        assert not (np.isfinite(val) and val > 0)
+
+    def test_argcheck_rejects_non_positive_sigma(self):
+        """sigma <= 0 must not produce a valid (positive-finite) PDF value."""
+        val = logrice.pdf(0.0, nu=1.0, sigma=-1.0)
+        assert not (np.isfinite(val) and val > 0)
+
+    def test_nu_zero_matches_lograyleigh(self):
+        """logrice with nu=0 must match lograyleigh exactly."""
+        sigma = 2.0
+        pdf_rice = logrice.pdf(Y, nu=0.0, sigma=sigma)
+        pdf_rayleigh = lograyleigh.pdf(Y, sigma=sigma)
+        np.testing.assert_allclose(pdf_rice, pdf_rayleigh, rtol=1e-6)
+
+    def test_log_transform_relation_to_rice(self):
+        """logrice.pdf(y) must equal rice.pdf(exp(y)) * exp(y) (change-of-variable)."""
+        from scipy.stats import rice
+
+        y_test = np.linspace(-2.0, 3.0, 20)
+        nu, sigma = 1.0, 2.0
+        direct = logrice.pdf(y_test, nu=nu, sigma=sigma)
+        via_rice = rice.pdf(np.exp(y_test), b=nu / sigma, scale=sigma) * np.exp(y_test)
+        np.testing.assert_allclose(direct, via_rice, rtol=1e-6)
+
+    def test_rvs_samples_are_finite(self):
+        """Random samples must be finite real numbers."""
+        rng = np.random.default_rng(42)
+        samples = logrice.rvs(nu=1.0, sigma=2.0, size=200, random_state=rng)
+        assert samples.shape == (200,)
+        assert np.all(np.isfinite(samples))
+
+    def test_rvs_sample_mean_near_numerical_mean(self):
+        """Sample mean of many RVS should be close to the numerically integrated mean."""
+        nu, sigma = 1.0, 2.0
+        rng = np.random.default_rng(0)
+        samples = logrice.rvs(nu=nu, sigma=sigma, size=50_000, random_state=rng)
+        y_fine = np.linspace(-20, 10, 200_000)
+        pdf_vals = logrice.pdf(y_fine, nu=nu, sigma=sigma)
+        numerical_mean = np.trapezoid(y_fine * pdf_vals, y_fine)
+        assert pytest.approx(samples.mean(), rel=5e-2) == numerical_mean
+
+
 if __name__ == "__main__":
     plot_k_dist_varying_alpha()
     plot_k_dist_varying_mu()
diff --git a/etc/tools/distributions.py b/etc/tools/distributions.py
index 3f7cc58..8c6c488 100644
--- a/etc/tools/distributions.py
+++ b/etc/tools/distributions.py
@@ -1,4 +1,4 @@
-from scipy.stats import rv_continuous
+from scipy.stats import rv_continuous, ncx2
 from scipy.special import kve, gammaln
 from scipy.integrate import quad
 import scipy.special as sc
@@ -9,7 +9,7 @@ import numpy as np
 class k_gen(rv_continuous):
     """Generalized K distribution for radar clutter modeling.
 
-    The probability density function is::
+    The probability density function is:
 
         f(x; mu, alpha, beta) = 2 / (Gamma(alpha) * Gamma(beta))
                                 * (alpha*beta/mu)^((alpha+beta)/2)
@@ -103,22 +103,16 @@ k_dist = k_gen(a=0.0, name="k_distribution", shapes="mu, alpha, beta")
 
 
 class lognakagami_gen(rv_continuous):
-    r"""A Log-Nakagami continuous random variable.
+    """Log-Nakagami continuous random variable.
 
-    If X follows a Nakagami distribution with shape parameter m >= 0.5
-    and spread Omega > 0, then Y = ln(X) follows the Log-Nakagami distribution.
-
-    %(before_notes)s
-
-    Notes
-    -----
-    The probability density function for `lognakagami` is:
+    The probability density function is:
 
         f(y; m, Omega) = 2*m^m / (Gamma(m)*Omega^m)
                          * exp(2*m*y) * exp(-(m/Omega)*exp(2*y))
 
-    for y in (-inf, +inf).  Derived via the change of variable Y = ln X,
-    whose Jacobian e^y combines with x^{2m-1} to give the e^{2my} term.
+    for y in (-inf, +inf), m >= 0.5, Omega > 0.  Derived via the change of
+    variable Y = ln X on a Nakagami(m, Omega) variate; the Jacobian e^y
+    combines with x^(2m-1) to give the exp(2*m*y) term.
 
     The mean and variance are:
 
@@ -130,10 +124,6 @@ class lognakagami_gen(rv_continuous):
     unchanged; entropy is also Omega-independent.
 
     `lognakagami` takes ``m`` and ``Omega`` as shape parameters.
-
-    See Also
-    --------
-    nakagami : The Nakagami distribution (before the log transform).
     """
 
     def _shape_info(self):
@@ -145,7 +135,6 @@ class lognakagami_gen(rv_continuous):
     def _argcheck(self, m, Omega):
         return (m >= 0.5) & (Omega > 0)
 
-    # ---------- PDF / log-PDF ----------
 
     def _pdf(self, y, m, Omega):
         return np.exp(self._logpdf(y, m, Omega))
@@ -159,7 +148,6 @@ class lognakagami_gen(rv_continuous):
                 + 2.0 * m * y
                 - (m / Omega) * np.exp(2.0 * y))
 
-    # ---------- CDF / SF / log-CDF / log-SF ----------
 
     def _cdf(self, y, m, Omega):
         # P(Y <= y) = P(X <= e^y) = gammainc(m, (m/Omega) * e^{2y})
@@ -174,7 +162,6 @@ class lognakagami_gen(rv_continuous):
     def _logsf(self, y, m, Omega):
         return np.log(sc.gammaincc(m, (m / Omega) * np.exp(2.0 * y)))
 
-    # ---------- PPF / ISF ----------
 
     def _ppf(self, q, m, Omega):
         # q = gammainc(m, (m/Omega)*e^{2y})
@@ -185,8 +172,6 @@ class lognakagami_gen(rv_continuous):
     def _isf(self, q, m, Omega):
         return 0.5 * np.log(Omega * sc.gammainccinv(m, q) / m)
 
-    # ---------- Moments & statistics ----------
-
     def _stats(self, m, Omega):
         # E[Y]   = 0.5*(psi(m) - ln(m) + ln(Omega))
         mu = 0.5 * (sc.digamma(m) - np.log(m) + np.log(Omega))
@@ -200,9 +185,7 @@ class lognakagami_gen(rv_continuous):
         # H = -E[ln f(Y)] = -ln2 + ln Γ(m) - m*psi(m) + m
         # Omega cancels exactly (translation invariance of differential entropy)
         return -np.log(2.0) + sc.gammaln(m) - m * sc.digamma(m) + m
-
-    # ---------- Random variate generation ----------
-
+    
     def _rvs(self, m, Omega, size=None, random_state=None):
         # X ~ Nakagami(m, Omega)  =>  X^2 ~ Gamma(m, Omega/m)
         g = random_state.gamma(m, Omega / m, size=size)
@@ -212,34 +195,27 @@ class lognakagami_gen(rv_continuous):
 lognakagami = lognakagami_gen(name='lognakagami', shapes="m, Omega")
 
 class loggamma_gen(rv_continuous):
-    r"""A Log-Gamma continuous random variable.
+    """Log-Gamma continuous random variable.
 
-    If X follows a Gamma distribution with shape a
-    and unit scale (beta = 1), then Y = ln X follows
-    the Log-Gamma distribution.
+    The probability density function is:
 
-    %(before_notes)s
+        f(y; a) = 1 / Gamma(a) * exp(a*y - exp(y))
 
-    Notes
-    -----
-    The probability density function for `loggamma_dist` is:
+    for y in (-inf, +inf), a > 0.  Derived via the change of variable
+    Y = ln X on a Gamma(a, 1) variate; the Jacobian e^y combines with
+    x^(a-1) to give the exp(a*y) term.
 
-        f(y, a) = 1 / Gamma(a) * exp(a*y - exp(y))
+    The mean and variance are:
 
-    for y in (-inf, +inf), a > 0.
+        E[Y]   = psi(a)
+        Var[Y] = psi_1(a)
 
-    This is the standardised form (scale beta = 1).
+    where psi and psi_1 are the digamma and trigamma functions.
+
+    The non-unit scale beta is recovered through scipy's ``loc`` parameter:
+    loc = ln(beta), since ln(beta * X) = ln(beta) + ln(X).
 
     `loggamma_dist` takes ``a`` as a shape parameter.
-
-    The non-unit scale beta is recovered through scipy's
-    ``loc`` parameter:  loc = ln(beta), since
-    ln(beta * X) = ln(beta) + ln(X).
-
-    See Also
-    --------
-    gamma : The Gamma distribution (before the log transform).
-
     """
  
     def _shape_info(self):
@@ -248,8 +224,6 @@ class loggamma_gen(rv_continuous):
     def _argcheck(self, a):
         return a > 0
  
-    # ---------- PDF / log-PDF ----------
- 
     def _pdf(self, y, a):
         return np.exp(self._logpdf(y, a))
  
@@ -257,8 +231,6 @@ class loggamma_gen(rv_continuous):
         #  ln f = a*y - e^y - ln Γ(a)
         return a * y - np.exp(y) - sc.gammaln(a)
  
-    # ---------- CDF / SF / log-CDF / log-SF ----------
- 
     def _cdf(self, y, a):
         # P(Y <= y) = P(X <= e^y) = gammainc(a, e^y)
         return sc.gammainc(a, np.exp(y))
@@ -272,8 +244,6 @@ class loggamma_gen(rv_continuous):
     def _logsf(self, y, a):
         return np.log(sc.gammaincc(a, np.exp(y)))
  
-    # ---------- PPF / ISF ----------
- 
     def _ppf(self, q, a):
         # Invert CDF:  q = gammainc(a, e^y)
         #   => e^y = gammaincinv(a, q)
@@ -283,8 +253,6 @@ class loggamma_gen(rv_continuous):
     def _isf(self, q, a):
         return np.log(sc.gammainccinv(a, q))
  
-    # ---------- Moments & statistics ----------
- 
     def _stats(self, a):
         # Y = ln(X), X ~ Gamma(a, 1)
         # E[Y] = psi(a)             (digamma)
@@ -303,8 +271,6 @@ class loggamma_gen(rv_continuous):
         # E[e^Y] = E[X] = a  (for Gamma(a, 1))
         return sc.gammaln(a) - a * sc.digamma(a) + a
  
-    # ---------- Random variate generation ----------
- 
     def _rvs(self, a, size=None, random_state=None):
         # Generate Gamma(a, 1) variates, then take log.
         # For small a, use  Gamma(a) ~ Gamma(a+1) * U^(1/a)
@@ -314,4 +280,154 @@ class loggamma_gen(rv_continuous):
                 + np.log(random_state.uniform(size=size)) / a)
  
  
-loggamma_dist = loggamma_gen(name='loggamma_dist')
\ No newline at end of file
+loggamma_dist = loggamma_gen(name='loggamma_dist')
+
+
+class lograyleigh_gen(rv_continuous):
+    """Log-Rayleigh continuous random variable.
+
+    The probability density function is:
+
+        f(y; sigma) = (e^{2y} / sigma^2) * exp(-e^{2y} / (2*sigma^2))
+
+    for y in (-inf, +inf), sigma > 0.  Derived via the change of variable
+    Y = ln X on a Rayleigh(sigma) variate; the Jacobian e^y combines with
+    x to give the e^{2y} term.
+
+    The mean and variance are:
+
+        E[Y]   = 0.5 * (ln(2*sigma^2) + psi(1))
+        Var[Y] = pi^2 / 24
+
+    where psi is the digamma function.  The scale sigma shifts the mean by
+    ln(sigma) but leaves all higher central moments unchanged; entropy is
+    also sigma-independent.
+
+    `lograyleigh` takes ``sigma`` as a shape parameter.
+    """
+
+    def _shape_info(self):
+        return [_ShapeInfo("sigma", False, (0, np.inf), (False, False))]
+
+    def _argcheck(self, sigma):
+        return sigma > 0
+
+    def _pdf(self, y, sigma):
+        return np.exp(self._logpdf(y, sigma))
+
+    def _logpdf(self, y, sigma):
+        # ln f = 2y - 2*ln(sigma) - e^{2y} / (2*sigma^2)
+        return 2.0 * y - 2.0 * np.log(sigma) - np.exp(2.0 * y) / (2.0 * sigma**2)
+
+    def _cdf(self, y, sigma):
+        return 1.0 - np.exp(-np.exp(2.0 * y) / (2.0 * sigma**2))
+
+    def _sf(self, y, sigma):
+        return np.exp(-np.exp(2.0 * y) / (2.0 * sigma**2))
+
+    def _logcdf(self, y, sigma):
+        return np.log1p(-np.exp(-np.exp(2.0 * y) / (2.0 * sigma**2)))
+
+    def _logsf(self, y, sigma):
+        return -np.exp(2.0 * y) / (2.0 * sigma**2)
+
+    def _ppf(self, q, sigma):
+        # q = 1 - exp(-e^{2y}/(2*sigma^2))
+        #   => e^{2y} = -2*sigma^2 * ln(1-q)
+        #   => y = 0.5 * ln(-2*sigma^2 * ln(1-q))
+        return 0.5 * np.log(-2.0 * sigma**2 * np.log1p(-q))
+
+    def _isf(self, q, sigma):
+        # q = exp(-e^{2y}/(2*sigma^2))
+        #   => y = 0.5 * ln(-2*sigma^2 * ln(q))
+        return 0.5 * np.log(-2.0 * sigma**2 * np.log(q))
+
+    def _stats(self, sigma):
+        # Y = 0.5*ln(2) + 0.5*ln(W) + ln(sigma), W ~ Exp(1) = Gamma(1, 1)
+        # E[Y] = 0.5*(ln(2*sigma^2) + psi(1))
+        # Var[Y] = 0.25*psi_1(1) = pi^2/24
+        # Standardised skewness/kurtosis are sigma-independent (pure shift)
+        mu = 0.5 * (np.log(2.0 * sigma**2) + sc.digamma(1))
+        mu2 = 0.25 * sc.polygamma(1, 1)
+        g1 = sc.polygamma(2, 1) / sc.polygamma(1, 1)**1.5
+        g2 = sc.polygamma(3, 1) / sc.polygamma(1, 1)**2
+        return mu, mu2, g1, g2
+
+    def _entropy(self, sigma):
+        # H(Y) = 1 - ln(2) - psi(1)  (sigma-independent; derived via H(X) - E[ln X])
+        return 1.0 - np.log(2.0) - sc.digamma(1)
+
+    def _rvs(self, sigma, size=None, random_state=None):
+        # X ~ Rayleigh(sigma) = sigma*sqrt(-2*ln(U)), U ~ Uniform(0,1)
+        u = random_state.uniform(size=size)
+        return np.log(sigma) + 0.5 * np.log(-2.0 * np.log(u))
+
+
+lograyleigh = lograyleigh_gen(name='lograyleigh', shapes="sigma")
+
+
+class logrice_gen(rv_continuous):
+    """Log-Rice continuous random variable.
+
+    The probability density function is:
+
+        f(y; nu, sigma) = (e^{2y} / sigma^2)
+                          * exp(-(e^{2y} + nu^2) / (2*sigma^2))
+                          * I_0(e^y * nu / sigma^2)
+
+    for y in (-inf, +inf), nu >= 0, sigma > 0.  Derived via the change of
+    variable Y = ln X on a Rice(nu, sigma) variate; the Jacobian e^y
+    combines with x to give the e^{2y} factor.  I_0 is the modified Bessel
+    function of the first kind of order zero.
+
+    The CDF involves the Marcum Q-function of order 1:
+
+        F(y; nu, sigma) = 1 - Q_1(nu/sigma, e^y/sigma)
+
+    When nu = 0, the distribution reduces to Log-Rayleigh.
+
+    `logrice` takes ``nu`` and ``sigma`` as shape parameters.
+    """
+
+    def _shape_info(self):
+        return [
+            _ShapeInfo("nu", False, (0, np.inf), (True, False)),
+            _ShapeInfo("sigma", False, (0, np.inf), (False, False)),
+        ]
+
+    def _argcheck(self, nu, sigma):
+        return (nu >= 0) & (sigma > 0)
+
+    def _pdf(self, y, nu, sigma):
+        return np.exp(self._logpdf(y, nu, sigma))
+
+    def _logpdf(self, y, nu, sigma):
+        # ln f = 2y - 2*ln(sigma) - (e^{2y} + nu^2)/(2*sigma^2) + ln(I_0(z))
+        # Use ive(0, z)*exp(z) = I_0(z) for stability: ln(I_0(z)) = ln(ive(0,z)) + z
+        z = np.exp(y) * nu / sigma**2
+        return (2.0 * y
+                - 2.0 * np.log(sigma)
+                - (np.exp(2.0 * y) + nu**2) / (2.0 * sigma**2)
+                + np.log(sc.ive(0, z)) + z)
+
+    def _cdf(self, y, nu, sigma):
+        # P(Y <= y) = 1 - Q_1(nu/sigma, e^y/sigma) = ncx2.cdf(e^{2y}/sigma^2, 2, nu^2/sigma^2)
+        return ncx2.cdf(np.exp(2.0 * y) / sigma**2, 2, (nu / sigma)**2)
+
+    def _sf(self, y, nu, sigma):
+        return ncx2.sf(np.exp(2.0 * y) / sigma**2, 2, (nu / sigma)**2)
+
+    def _logcdf(self, y, nu, sigma):
+        return ncx2.logcdf(np.exp(2.0 * y) / sigma**2, 2, (nu / sigma)**2)
+
+    def _logsf(self, y, nu, sigma):
+        return ncx2.logsf(np.exp(2.0 * y) / sigma**2, 2, (nu / sigma)**2)
+
+    def _rvs(self, nu, sigma, size=None, random_state=None):
+        # X ~ Rice(nu, sigma): norm of 2D Gaussian with mean (nu, 0) and std sigma
+        z1 = random_state.normal(nu, sigma, size=size)
+        z2 = random_state.normal(0.0, sigma, size=size)
+        return np.log(np.hypot(z1, z2))
+
+
+logrice = logrice_gen(name='logrice', shapes="nu, sigma")
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