require(ggplot2)
require(ggExtra)
require(hrbrthemes)
require(extrafont)
require(gridExtra)
require(ggrepel)
require(goftest)
theme_set(theme_ipsum(base_family = "Times New Roman", 
              base_size = 10, axis_title_size = 10))

First, read the data,

HC.BP = data.frame("H" = numeric(16000), 
                   "C" = numeric(16000),
                   "Dist" = numeric(16000),
                   "D" = numeric(16000),
                   "N" = numeric(16000), 
                   stringsAsFactors=FALSE)
filecsv = data.frame(read.csv("../Data/HC_series_fk0_16000.csv"))
HC.BP$H = filecsv[,1]
HC.BP$C = filecsv[,2]
HC.BP$D = as.factor(filecsv[,3])
HC.BP$N = as.factor(rep(c(rep(1e+04, 100), rep(2e+04, 100), rep(3e+04, 100), rep(4e+04, 100), rep(5e+04, 100), rep(6e+04, 100), rep(7e+04, 100), rep(8e+04, 100), rep(9e+04, 100), rep(1e+05, 100)), 16))
summary(HC.BP)
       H                C                  Dist   D              N       
 Min.   :0.9199   Min.   :0.0002271   Min.   :0   3:4000   10000  :1600  
 1st Qu.:0.9869   1st Qu.:0.0041165   1st Qu.:0   4:4000   20000  :1600  
 Median :0.9924   Median :0.0075186   Median :0   5:4000   30000  :1600  
 Mean   :0.9902   Mean   :0.0096574   Mean   :0   6:4000   40000  :1600  
 3rd Qu.:0.9959   3rd Qu.:0.0128926   3rd Qu.:0            50000  :1600  
 Max.   :0.9998   Max.   :0.0745442   Max.   :0            60000  :1600  
                                                           (Other):6400  
ggplot(data = HC.BP, aes(x = H, y = C, color = D)) +
  geom_point(size = 3) +
  labs(title = "Points in the HxC plane",
       x = expression(italic(H)),
       y = expression(italic(C))
  )

Now separated by the embedding dimension \(D\).

ggplot(data=HC.BP, aes(x=H, y=C, color=D)) +
  geom_point(size=2) +
  labs(title="Points in the HxC plane",
       x=expression(italic(H)),
       y=expression(italic(C))) +
  facet_grid(.~D)

We see a seemingly linear trend, but at this point we have to recall that \(C=HD\), in which \(D\) is a distance (in this case, the Jensen-Shannon distance) to an equilibrium distribution (in this case, the Uniform law).

In order to see the relationship between the variables we are studying, let’s look at \(H\times D\).

HC.BP$Dist = HC.BP$C / HC.BP$H
ggplot(data=HC.BP, aes(x=Dist, y=C, color=D)) +
  geom_point(size=2) +
  labs(title="Points in the Dist x C plane",
       x="Dist",
       y=expression(italic(C))) +
  facet_grid(.~D)

ggplot(data=HC.BP, aes(x=H, y=Dist, color=D)) +
  geom_point(size=2) +
  labs(title="Points in the H x Dist plane",
       x=expression(italic(H)),
       y="Dist") +
  facet_grid(.~D)

We will take N out of the data frame, in order to use the default regression in ggplot

HC.BP.regression.data = HC.BP[,-3]
lm.HC = lm(data=HC.BP.regression.data, formula = C ~ H * D)
summary(lm.HC)

Call:
lm(formula = C ~ H * D, data = HC.BP.regression.data)

Residuals:
       Min         1Q     Median         3Q        Max 
-0.0046003 -0.0000673 -0.0000218  0.0000608  0.0037435 

Coefficients:
              Estimate Std. Error   t value Pr(>|t|)    
(Intercept)  0.9778085  0.0005905  1655.768  < 2e-16 ***
H           -0.9777680  0.0005964 -1639.509  < 2e-16 ***
D4          -0.0024713  0.0008190    -3.018  0.00255 ** 
D5          -0.0018136  0.0008318    -2.180  0.02924 *  
D6          -0.0039134  0.0008092    -4.836 1.34e-06 ***
H:D4         0.0024901  0.0008271     3.011  0.00261 ** 
H:D5         0.0018344  0.0008400     2.184  0.02899 *  
H:D6         0.0039479  0.0008173     4.831 1.37e-06 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 0.0002963 on 15992 degrees of freedom
Multiple R-squared:  0.9986,    Adjusted R-squared:  0.9986 
F-statistic: 1.621e+06 on 7 and 15992 DF,  p-value: < 2.2e-16
hist(lm.HC$residuals, breaks = 200)

plot(lm.HC)

The above results suggest that there is no evidence against the use of the embedding dimension \(D\) as a factor in the linear regression model.

ggplot(HC.BP.regression.data, aes(x=H, y=C, colour=D)) +
  geom_point(size=2) +
  geom_smooth(method="lm", formula = y~x) +
  labs(title="Complexity explained by Entropy",
       x=expression(italic(H)),
       y=expression(italic(C)))

Now, let’s see the fitted lines in a semilogarithmic scale.

ggplot(HC.BP.regression.data, aes(x=H, y=C, colour=D)) +
  geom_point(size=2) +
  scale_y_log10() +
  geom_smooth(method="lm", formula = y~x) +
  labs(title="Complexity explained by Entropy",
       x=expression(italic(H)),
       y=expression(italic(C)~"[logarithmic scale]"))

  facet_grid(.~D)
<ggproto object: Class FacetGrid, Facet, gg>
    compute_layout: function
    draw_back: function
    draw_front: function
    draw_labels: function
    draw_panels: function
    finish_data: function
    init_scales: function
    map_data: function
    params: list
    setup_data: function
    setup_params: function
    shrink: TRUE
    train_scales: function
    vars: function
    super:  <ggproto object: Class FacetGrid, Facet, gg>

The model we are fitting is \[ \left\{ \begin{eqnarray*} C^{(3)} &= \beta_0^{(3)} + \beta_1^{(3)} H^{(3)},\\ C^{(4)} &= \beta_0^{(4)} + \beta_1^{(4)} H^{(4)},\\ C^{(5)} &= \beta_0^{(5)} + \beta_1^{(5)} H^{(5)},\\ C^{(6)} &= \beta_0^{(6)} + \beta_1^{(6)} H^{(6)}.\\ \end{eqnarray*} \right. \] in other words, a different linear relationship for each embedding dimension \(D\).

Let’s save the estimates and their confidence intervals.

beta0 <- c(
  lm.HC$coefficients[1],
  lm.HC$coefficients[1] + lm.HC$coefficients[3],
  lm.HC$coefficients[1] + lm.HC$coefficients[4],
  lm.HC$coefficients[1] + lm.HC$coefficients[5])
beta0inf <- c(
  confint(lm.HC)[1,1],
  beta0[2] - confint(lm.HC)[3,1],
  beta0[3] - confint(lm.HC)[4,1],
  beta0[4] - confint(lm.HC)[5,1])
beta0sup <- c(
  confint(lm.HC)[1,2],
  beta0[2] + confint(lm.HC)[3,2],
  beta0[3] + confint(lm.HC)[4,2],
  beta0[4] + confint(lm.HC)[5,2])
beta1 <- c(
  lm.HC$coefficients[2],
  lm.HC$coefficients[2] + lm.HC$coefficients[6],
  lm.HC$coefficients[2] + lm.HC$coefficients[7],
  lm.HC$coefficients[2] + lm.HC$coefficients[8])
beta1inf <-c(
  confint(lm.HC)[2,1],
  beta1[2] - confint(lm.HC)[6,1],
  beta1[3] - confint(lm.HC)[7,1],
  beta1[4] - confint(lm.HC)[8,1])
beta1sup <- c(
  confint(lm.HC)[2,2],
  beta1[2] + confint(lm.HC)[6,2],
  beta1[3] + confint(lm.HC)[7,2],
  beta1[4] + confint(lm.HC)[8,2])
estimates <- data.frame(beta0=beta0, 
                        beta0inf=beta0inf,
                        beta0sup=beta0sup,
                        beta1=beta1, 
                        beta1inf=beta1inf,
                        beta1sup=beta1sup,
                        D=3:6)
estimates

The fitted parameters are: \[ \left\{ \begin{eqnarray*} \widehat{\beta}_0^{(3)} =0.983 ,&\quad \widehat{\beta}_1^{(3)}=-0.983,\\ \widehat{\beta}_0^{(4)} =1.310 ,&\quad \widehat{\beta}_1^{(4)}=-1.310,\\ \widehat{\beta}_0^{(5)} =1.785 ,&\quad \widehat{\beta}_1^{(5)}=-1.785,\\ \widehat{\beta}_0^{(6)} =2.405 ,&\quad \widehat{\beta}_1^{(6)}=-2.405.\\ \end{eqnarray*} \right. \]

Let’s see how they behave.

plot.beta0 <- ggplot(data=estimates, aes(x=D, y=beta0)) +
  geom_point() +
  labs(title="Intercept vs. embedding dimension",
    x=expression(italic(D)),
    y=expression(widehat(beta)[0]))
plot.beta1 <- ggplot(data=estimates, aes(x=D, y=beta1)) +
  geom_point() +
    labs(title="Slope vs embedding dimension",
    x=expression(italic(D)),
    y=expression(widehat(beta)[1]))
grid.arrange(plot.beta0, plot.beta1, nrow=1)

The joint variation:

ggplot(data=estimates, aes(x=beta0, y=beta1)) + 
  geom_smooth(method = "lm", formula = y~x) +
  geom_point(size=2) +
#  geom_errorbar(aes(ymin=beta1inf, ymax=beta1sup)) +
#  geom_errorbarh(aes(xmin=beta0inf, xmax=beta0sup)) +
  geom_label_repel(data=estimates, aes(x=beta0, y=beta1, label=D),
                   direction = "x") +
  labs(title="Intercept vs Slope",
    x=expression(widehat(beta)[0]),
    y=expression(widehat(beta)[1])) +
    coord_fixed()

We verify there is a linear relationship between \(\widehat{\beta}_0\) and \(\widehat{\beta}_1\).

---
title: "Regression Analysis: Report 0"
author: "Alejandro Frery"
date: "Apr 8, 2020"
output:
  html_notebook: default
  pdf_document: default
---
```{r}
require(ggplot2)
require(ggExtra)
require(hrbrthemes)
require(extrafont)
require(gridExtra)
require(ggrepel)
require(goftest)

theme_set(theme_ipsum(base_family = "Times New Roman", 
              base_size = 10, axis_title_size = 10))
```


First, read the data,

```{r}
HC.BP = data.frame("H" = numeric(16000), 
                   "C" = numeric(16000),
                   "Dist" = numeric(16000),
                   "D" = numeric(16000),
                   "N" = numeric(16000), 
                   stringsAsFactors=FALSE)

filecsv = data.frame(read.csv("../Data/HC_series_fk0_16000.csv"))
HC.BP$H = filecsv[,1]
HC.BP$C = filecsv[,2]
HC.BP$D = as.factor(filecsv[,3])
HC.BP$N = as.factor(rep(c(rep(1e+04, 100), rep(2e+04, 100), rep(3e+04, 100), rep(4e+04, 100), rep(5e+04, 100), rep(6e+04, 100), rep(7e+04, 100), rep(8e+04, 100), rep(9e+04, 100), rep(1e+05, 100)), 16))

summary(HC.BP)

ggplot(data = HC.BP, aes(x = H, y = C, color = D)) +
  geom_point(size = 3) +
  labs(title = "Points in the HxC plane",
       x = expression(italic(H)),
       y = expression(italic(C))
  )
```


Now separated by the embedding dimension $D$.

```{r}
ggplot(data=HC.BP, aes(x=H, y=C, color=D)) +
  geom_point(size=2) +
  labs(title="Points in the HxC plane",
       x=expression(italic(H)),
       y=expression(italic(C))) +
  facet_grid(.~D)
```

We see a seemingly linear trend, but at this point we have to recall that $C=HD$, in which $D$ is a distance (in this case, the Jensen-Shannon distance) to an equilibrium distribution (in this case, the Uniform law).

In order to see the relationship between the variables we are studying, let's look at $H\times D$.
```{r}
HC.BP$Dist = HC.BP$C / HC.BP$H

ggplot(data=HC.BP, aes(x=Dist, y=C, color=D)) +
  geom_point(size=2) +
  labs(title="Points in the Dist x C plane",
       x="Dist",
       y=expression(italic(C))) +
  facet_grid(.~D)
```

```{r}
ggplot(data=HC.BP, aes(x=H, y=Dist, color=D)) +
  geom_point(size=2) +
  labs(title="Points in the H x Dist plane",
       x=expression(italic(H)),
       y="Dist") +
  facet_grid(.~D)
```

We will take N out of the data frame, in order to use the default regression in ggplot
```{r}
HC.BP.regression.data = HC.BP[,-3]
lm.HC = lm(data=HC.BP.regression.data, formula = C ~ H * D)
summary(lm.HC)
```

```{r}
hist(lm.HC$residuals, breaks = 200)
plot(lm.HC)
```

The above results suggest that there is no evidence against the use of the embedding dimension $D$ as a factor in the linear regression model.

```{r}
ggplot(HC.BP.regression.data, aes(x=H, y=C, colour=D)) +
  geom_point(size=2) +
  geom_smooth(method="lm", formula = y~x) +
  labs(title="Complexity explained by Entropy",
       x=expression(italic(H)),
       y=expression(italic(C)))
```

Now, let's see the fitted lines in a semilogarithmic scale.

```{r}
ggplot(HC.BP.regression.data, aes(x=H, y=C, colour=D)) +
  geom_point(size=2) +
  scale_y_log10() +
  geom_smooth(method="lm", formula = y~x) +
  labs(title="Complexity explained by Entropy",
       x=expression(italic(H)),
       y=expression(italic(C)~"[logarithmic scale]"))
  facet_grid(.~D)
```
The model we are fitting is
$$
\left\{
  \begin{eqnarray*}
    C^{(3)} &= \beta_0^{(3)} + \beta_1^{(3)} H^{(3)},\\ 
    C^{(4)} &= \beta_0^{(4)} + \beta_1^{(4)} H^{(4)},\\ 
    C^{(5)} &= \beta_0^{(5)} + \beta_1^{(5)} H^{(5)},\\ 
    C^{(6)} &= \beta_0^{(6)} + \beta_1^{(6)} H^{(6)}.\\ 
  \end{eqnarray*}
\right.
$$
in other words, a different linear relationship for each embedding dimension $D$.

Let's save the estimates and their confidence intervals.
```{r}
beta0 <- c(
  lm.HC$coefficients[1],
  lm.HC$coefficients[1] + lm.HC$coefficients[3],
  lm.HC$coefficients[1] + lm.HC$coefficients[4],
  lm.HC$coefficients[1] + lm.HC$coefficients[5])

beta0inf <- c(
  confint(lm.HC)[1,1],
  beta0[2] - confint(lm.HC)[3,1],
  beta0[3] - confint(lm.HC)[4,1],
  beta0[4] - confint(lm.HC)[5,1])

beta0sup <- c(
  confint(lm.HC)[1,2],
  beta0[2] + confint(lm.HC)[3,2],
  beta0[3] + confint(lm.HC)[4,2],
  beta0[4] + confint(lm.HC)[5,2])

beta1 <- c(
  lm.HC$coefficients[2],
  lm.HC$coefficients[2] + lm.HC$coefficients[6],
  lm.HC$coefficients[2] + lm.HC$coefficients[7],
  lm.HC$coefficients[2] + lm.HC$coefficients[8])

beta1inf <-c(
  confint(lm.HC)[2,1],
  beta1[2] - confint(lm.HC)[6,1],
  beta1[3] - confint(lm.HC)[7,1],
  beta1[4] - confint(lm.HC)[8,1])

beta1sup <- c(
  confint(lm.HC)[2,2],
  beta1[2] + confint(lm.HC)[6,2],
  beta1[3] + confint(lm.HC)[7,2],
  beta1[4] + confint(lm.HC)[8,2])

estimates <- data.frame(beta0=beta0, 
                        beta0inf=beta0inf,
                        beta0sup=beta0sup,
                        beta1=beta1, 
                        beta1inf=beta1inf,
                        beta1sup=beta1sup,
                        D=3:6)

estimates
```


The fitted parameters are:
$$
\left\{
  \begin{eqnarray*}
    \widehat{\beta}_0^{(3)} =0.983 ,&\quad \widehat{\beta}_1^{(3)}=-0.983,\\ 
    \widehat{\beta}_0^{(4)} =1.310  ,&\quad \widehat{\beta}_1^{(4)}=-1.310,\\ 
    \widehat{\beta}_0^{(5)} =1.785 ,&\quad \widehat{\beta}_1^{(5)}=-1.785,\\ 
    \widehat{\beta}_0^{(6)} =2.405 ,&\quad \widehat{\beta}_1^{(6)}=-2.405.\\ 
  \end{eqnarray*}
\right. 
$$

Let's see how they behave.
```{r}
plot.beta0 <- ggplot(data=estimates, aes(x=D, y=beta0)) +
  geom_point() +
  labs(title="Intercept vs. embedding dimension",
    x=expression(italic(D)),
    y=expression(widehat(beta)[0]))
plot.beta1 <- ggplot(data=estimates, aes(x=D, y=beta1)) +
  geom_point() +
    labs(title="Slope vs embedding dimension",
    x=expression(italic(D)),
    y=expression(widehat(beta)[1]))
grid.arrange(plot.beta0, plot.beta1, nrow=1)
```

The joint variation:
```{r}
ggplot(data=estimates, aes(x=beta0, y=beta1)) + 
  geom_smooth(method = "lm", formula = y~x) +
  geom_point(size=2) +
#  geom_errorbar(aes(ymin=beta1inf, ymax=beta1sup)) +
#  geom_errorbarh(aes(xmin=beta0inf, xmax=beta0sup)) +
  geom_label_repel(data=estimates, aes(x=beta0, y=beta1, label=D),
                   direction = "x") +
  labs(title="Intercept vs Slope",
    x=expression(widehat(beta)[0]),
    y=expression(widehat(beta)[1])) +
    coord_fixed()
```
We verify there is a linear relationship between $\widehat{\beta}_0$ and $\widehat{\beta}_1$.
