knitr::opts_chunk$set( collapse = TRUE, comment = "#>" )
This document will provide specific details of 2D-Gaussian equations used by
the different method
options within gaussplotR::fit_gaussian_2D()
.
method = "elliptical"
Using method = "elliptical"
fits a two-dimensional, elliptical Gaussian
equation to gridded data.
$$G(x,y) = A_o + A * e^{-U/2}$$
where G is the value of the 2D-Gaussian at each ${(x,y)}$ point, $A_o$ is a constant term, and $A$ is the amplitude (i.e. scale factor).
The elliptical function, $U$, is:
$$U = (x'/a)^{2} + (y'/b)^{2}$$
where $a$ is the spread of Gaussian along the x-axis and $b$ is the spread of Gaussian along the y-axis.
$x'$ and $y'$ are defined as:
$$x' = (x - x_0)cos(\theta) - (y - y_0)sin(\theta)$$ $$y' = (x - x_0)sin(\theta) + (y - y_0)cos(\theta)$$ where $x_0$ is the center (peak) of the Gaussian along the x-axis, $y_0$ is the center (peak) of the Gaussian along the y-axis, and $\theta$ is the rotation of the ellipse from the x-axis in radians, counter-clockwise.
Therefore, all together:
$$G(x,y) = A_o + A * e^{-((((x - x_0)cos(\theta) - (y - y_0)sin(\theta))/a)^{2}+ (((x - x_0)sin(\theta) + (y - y_0)cos(\theta))/b)^{2})/2}$$
Setting the constrain_orientation
argument to a numeric will optionally
constrain the value of $\theta$ to a user-specified value. If a numeric is
supplied here, please note that the value will be interpreted as a value in
radians. Constraining $\theta$ to a user-supplied value can lead to considerably
poorer-fitting Gaussians and/or trouble with converging on a stable solution; in
most cases constrain_orientation
should remain its default: "unconstrained"
.
method = "elliptical_log"
The formula used in method = "elliptical_log"
uses the modification of a 2D
Gaussian fit used by Priebe et al. 2003^[Priebe NJ, Cassanello CR, Lisberger SG.
The neural representation of speed in macaque area MT/V5. J Neurosci. 2003 Jul
2;23(13):5650-61. doi: 10.1523/JNEUROSCI.23-13-05650.2003.].
$$G(x,y) = A * e^{(-(x - x_0)^2)/\sigma_x^2} * e^{(-(y - y'(x)))/\sigma_y^2}$$
and
$$y'(x) = 2^{(Q+1) * (x - x_0) + y_0}$$ where $A$ is the amplitude (i.e. scale factor), $x_0$ is the center (peak) of the Gaussian along the x-axis, $y_0$ is the center (peak) of the Gaussian along the y-axis, $\sigma_x$ is the spread along the x-axis, $\sigma_y$ is the spread along the y-axis and $Q$ is an orientation parameter.
Therefore, all together:
$$G(x,y) = A * e^{(-(x - x_0)^2)/\sigma_x^2} * e^{(-(y - (2^{(Q+1) * (x - x_0) + y_0})))/\sigma_y^2}$$
This formula is intended for use with log2-transformed data.
Setting the constrain_orientation
argument to a numeric will optionally
constrain the value of $Q$ to a user-specified value, which can be useful for
certain kinds of analyses (see Priebe et al. 2003 for more). Keep in mind that
constraining $Q$ to a user-supplied value can lead to considerably
poorer-fitting Gaussians and/or trouble with converging on a stable solution; in
most cases constrain_orientation
should remain its default: "unconstrained"
.
method = "circular"
This method uses a relatively simple formula:
$$G(x,y) = A * e^{(-( ((x-x_0)^2/2\sigma_x^2) + ((y-y_0)^2/2\sigma_y^2)) )}$$
where $A$ is the amplitude (i.e. scale factor), $x_0$ is the center (peak) of the Gaussian along the x-axis, $y_0$ is the center (peak) of the Gaussian along the y-axis, $\sigma_x$ is the spread along the x-axis, and $\sigma_y$ is the spread along the y-axis.
That's all!
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