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Nakagami distribution
Statistical distribution
Statistical distribution
name =Nakagami| type =density| pdf_image =[[Image:Nakagami pdf.svg|325px]]| cdf_image =[[Image:Nakagami cdf.svg|325px]]| parameters = m\text{ or } \mu \geq 0.5 shape (real) \Omega \text{ or } \omega 0 scale (real)| support =x 0!| pdf =\frac{2m^m}{\Gamma(m)\Omega^m} x^{2m-1} \exp\left(-\frac{m}{\Omega}x^2 \right)| cdf =\frac{\gamma \left(m,\frac{m}{\Omega} x^2\right)}{\Gamma(m)}| mean =\frac{\Gamma(m+\frac{1}{2})}{\Gamma(m)}\left(\frac{\Omega}{m}\right)^{1/2}| median =No simple closed form| mode =\left(\frac{(2m-1)\Omega}{2m}\right)^{1/2}| variance =\Omega\left(1-\frac{1}{m}\left(\frac{\Gamma(m+\frac{1}{2})}{\Gamma(m)}\right)^2\right)| skewness =| kurtosis =| entropy =| mgf =| char =| The Nakagami distribution or the Nakagami-m distribution is a probability distribution related to the gamma distribution. The family of Nakagami distributions has two parameters: a shape parameter m\geq 1/2 and a scale parameter \Omega 0. It is used to model physical phenomena such as those found in medical ultrasound imaging, communications engineering, meteorology, hydrology, multimedia, and seismology.
Characterization
Its probability density function (pdf) is{{cite web | access-date = 2007-08-04 }}
: f(x;,m,\Omega) = \frac{2m^m}{\Gamma(m)\Omega^m}x^{2m-1}\exp\left(-\frac{m}{\Omega}x^2\right) \text{ for } x\geq 0. where m\geq 1/2 and \Omega0.
Its cumulative distribution function (CDF) is
: F(x;,m,\Omega) = \frac{\gamma\left(m, \frac{m}{\Omega}x^2\right)}{\Gamma(m)} = P\left(m, \frac{m}{\Omega}x^2\right)
where P is the regularized (lower) incomplete gamma function.
Parameterization
The parameters m and \Omega are
: m = \frac{\left( \operatorname{E} [X^2] \right)^2 } {\operatorname{Var} [X^2]}, and : \Omega = \operatorname{E} [X^2].
No closed form solution exists for the median of this distribution, although special cases do exist, such as \sqrt{\Omega \ln(2)} when m = 1. For practical purposes the median would have to be calculated as the 50th-percentile of the observations.
Parameter estimation
An alternative way of fitting the distribution is to re-parametrize \Omega as σ = Ω/m.
Given independent observations X_1=x_1,\ldots,X_n=x_n from the Nakagami distribution, the likelihood function is
: L( \sigma, m) = \left( \frac{2}{\Gamma(m)\sigma^m} \right)^n \left( \prod_{i=1}^n x_i\right)^{2m-1} \exp\left(-\frac{\sum_{i=1}^n x_i^2} \sigma \right).
Its logarithm is
: \ell(\sigma, m) = \log L(\sigma,m) = -n \log \Gamma(m) - nm\log\sigma + (2m-1) \sum_{i=1}^n \log x_i - \frac{ \sum_{i=1}^n x_i^2} \sigma.
Therefore
: \begin{align} \frac{\partial\ell}{\partial\sigma} = \frac{-nm\sigma+\sum_{i=1}^n x_i^2}{\sigma^2} \quad \text{and} \quad \frac{\partial\ell}{\partial m} = -n\frac{\Gamma'(m)}{\Gamma(m)} -n \log\sigma + 2\sum_{i=1}^n \log x_i. \end{align} These derivatives vanish only when : \sigma= \frac{\sum_{i=1}^n x_i^2}{nm} and the value of m for which the derivative with respect to m vanishes is found by numerical methods including the Newton–Raphson method.
It can be shown that at the critical point a global maximum is attained, so the critical point is the maximum-likelihood estimate of (m,σ). Because of the equivariance of maximum-likelihood estimation, a maximum likelihood estimate for Ω is obtained as well. Here one could add something about the probability distribution of the MLE as a function of the n observed random variables. --
Random variate generation
The Nakagami distribution is related to the gamma distribution. In particular, given a random variable Y , \sim \textrm{Gamma}(k, \theta), it is possible to obtain a random variable X , \sim \textrm{Nakagami} (m, \Omega), by setting k=m, \theta=\Omega / m , and taking the square root of Y:
: X = \sqrt{Y}. ,
Alternatively, the Nakagami distribution f(y; ,m,\Omega) can be generated from the chi distribution with parameter k set to 2m and then following it by a scaling transformation of random variables. That is, a Nakagami random variable X is generated by a simple scaling transformation on a chi-distributed random variable Y \sim \chi(2m) as below.
: X = \sqrt{(\Omega / 2 m)}Y .
For a chi-distribution, the degrees of freedom 2m must be an integer, but for Nakagami the m can be any real number greater than 1/2. This is the critical difference and accordingly, Nakagami-m is viewed as a generalization of chi-distribution, similar to a gamma distribution being considered as a generalization of chi-squared distributions.
History and applications
The Nakagami distribution is relatively new, being first proposed in 1960 by Minoru Nakagami as a mathematical model for small-scale fading in long-distance high-frequency radio wave propagation. It has been used to model attenuation of wireless signals traversing multiple paths and to study the impact of fading channels on wireless communications.
References
References
- R. Kolar, R. Jirik, J. Jan (2004) [http://www.radioeng.cz/fulltexts/2004/04_01_08_12.pdf "Estimator Comparison of the Nakagami-m Parameter and Its Application in Echocardiography"], ''Radioengineering'', 13 (1), 8–12
- Mitra, Rangeet. (2012). "Maximum Likelihood Estimate of Parameters of Nakagami-m Distribution". International Conference on Communications, Devices and Intelligent Systems (CODIS), 2012.
- Nakagami, M. (1960) "The m-Distribution, a general formula of intensity of rapid fading". In William C. Hoffman, editor, ''Statistical Methods in Radio Wave Propagation: Proceedings of a Symposium held June 18–20, 1958'', pp. 3–36. Pergamon Press., {{doi. 10.1016/B978-0-08-009306-2.50005-4
- Parsons, J. D. (1992) ''The Mobile Radio Propagation Channel''. New York: Wiley.
- (2013). "2013 World Congress on Computer and Information Technology (WCCIT)".
- (2009). "Nakagami-q (Hoyt) distribution function with applications". Electronics Letters.
- "HoytDistribution".
- "NakagamiDistribution".
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