Introduction

Libraries

Data

price = tq_get_cafef(symbol = 'VNM', from = '2010-01-01', to = '2022-01-01', src = 'CAFEF')
#VNM from 2010-01-01 to 2022-01-01 already cloned 
glimpse(as.data.frame(price))
Rows: 2,994
Columns: 14
$ date             <date> 2021-12-31, 2021-12-30, 2021-12-29, 2021-12-28, 2021-1…
$ change.percent   <chr> "1.10 (1.29 %)", "0.10 (0.12 %)", "-0.30 (-0.35 %)", "-…
$ open             <dbl> 85.5, 85.3, 85.5, 86.2, 86.0, 84.7, 85.4, 85.7, 85.8, 8…
$ high             <dbl> 87.5, 85.6, 85.6, 86.2, 86.4, 86.0, 85.4, 86.2, 86.0, 8…
$ low              <dbl> 85.3, 85.1, 85.1, 85.2, 85.7, 84.7, 84.5, 85.3, 85.5, 8…
$ close            <dbl> 86.4, 85.3, 85.2, 85.5, 86.1, 86.0, 84.7, 85.4, 85.5, 8…
$ adjusted         <dbl> 84.98, 83.90, 83.80, 84.10, 84.69, 84.59, 83.31, 84.00,…
$ match.volume     <dbl> 2325100, 893100, 945400, 1544400, 1138300, 1148400, 214…
$ reconcile.volume <dbl> 143400, 147400, 20000, 393400, 147400, 280000, 471100, …
$ match.value      <dbl> 200645000000, 76247000000, 80583000000, 132401000000, 9…
$ reconcile.value  <dbl> 13078080000, 13428140000, 1751200000, 34511340000, 1179…
$ volume.round1    <dbl> 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0…
$ volume.round2    <dbl> 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0…
$ volume.round3    <dbl> 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0…

Dataframe: Date & Adjusted Price

df <- price %>%
  arrange(date) %>%
  select(date, adjusted)
tail(df)

Stock Price Plot

ggplot(df, aes(date, adjusted, group = 1, color = adjusted)) + geom_line() +labs(x = "Date", y = "Price", title = "VNM")+ geom_hline(yintercept =mean(df$adjusted) , color = 'red')

Log Return

# Return Plot 
vnm_logret = xts(df$adjusted,as.Date(df$date))

vnm_logret = vnm_logret %>% 
  log %>% 
  diff

vnm_logret= vnm_logret[-1,]

Log Return Plot

qplot(x = 1:length(vnm_logret) , y = vnm_logret , geom = 'line') + geom_line(color = 'darkblue') + 
  geom_hline(yintercept = mean(vnm_logret) , color = 'red' , size = 1) + 
  labs(x = '' , y = 'Daily Returns')
Don't know how to automatically pick scale for object of type xts/zoo. Defaulting to continuous.

To verify the stationarity of the returns, we utilize the Augmented Dickey-Fuller test where null hypothesis indicates non-stationary time series.

adf.test(vnm_logret)

    Augmented Dickey-Fuller Test

data:  vnm_logret
Dickey-Fuller = -14.737, Lag order = 14, p-value = 0.01
alternative hypothesis: stationary

Box-Jenkins Methodology

For time series analysis, Box-Jenkins approach applies ARIMA models to find the best fit of a time series model that represent the stochastic process which generate time series. This method uses a three stage modelling approach: a) identification, b) estimation, c) diagnostic checking. ### Identification

model.arima = auto.arima(vnm_logret , max.order = c(3 , 0 ,3) , stationary = TRUE , trace = T , ic = 'aicc')

 Fitting models using approximations to speed things up...

 ARIMA(2,0,2) with non-zero mean : -16640.05
 ARIMA(0,0,0) with non-zero mean : -16627.37
 ARIMA(1,0,0) with non-zero mean : -16632.69
 ARIMA(0,0,1) with non-zero mean : -16625.63
 ARIMA(0,0,0) with zero mean     : -16621.77
 ARIMA(1,0,2) with non-zero mean : -16629
 ARIMA(2,0,1) with non-zero mean : -16629.1
 ARIMA(3,0,2) with non-zero mean : -16640.76
 ARIMA(3,0,1) with non-zero mean : -16641.24
 ARIMA(3,0,0) with non-zero mean : -16638.24
 ARIMA(4,0,1) with non-zero mean : Inf
 ARIMA(2,0,0) with non-zero mean : -16629.98
 ARIMA(4,0,0) with non-zero mean : -16642.4
 ARIMA(5,0,0) with non-zero mean : -16641.9
 ARIMA(5,0,1) with non-zero mean : -16641.61
 ARIMA(4,0,0) with zero mean     : -16635.79

 Now re-fitting the best model(s) without approximations...

 ARIMA(4,0,0) with non-zero mean : -16629.58

 Best model: ARIMA(4,0,0) with non-zero mean 

Estimation

model.arima
Series: vnm_logret 
ARIMA(4,0,0) with non-zero mean 

Coefficients:
         ar1     ar2      ar3      ar4    mean
      0.0084  0.0083  -0.0472  -0.0321  0.0008
s.e.  0.0183  0.0183   0.0183   0.0183  0.0003

sigma^2 = 0.0002257:  log likelihood = 8320.81
AIC=-16629.61   AICc=-16629.58   BIC=-16593.59

Diagnostics Checking

The procedure includes observing residual plot and its ACF & PACF diagram, and check Ljung-Box test result. If ACF & PACF of the model residuals show no significant lags, the selected model is appropriate.

model.arima$residuals %>% ggtsdisplay(plot.type = 'hist' , lag.max = 14)

Both ACF and PACF plots are similar and autocorrelations seem to be equal to zero. The lower right corner plot represents the histogram of the residuals compared to a normal distribution N(0 , σ2).

ar.res = model.arima$residuals
Box.test(model.arima$residuals , lag = 14 , fitdf = 2 , type = 'Ljung-Box')

    Box-Ljung test

data:  model.arima$residuals
X-squared = 5.8647, df = 12, p-value = 0.9227

We cannot reject the null hypothesis, therefore the process of the residuals behave like white noise so there is no indication of pattern that might be modeled.

GARCH Implementation

Although ACF & PACF of residuals have no significant lags, the time series plot of residuals shows some cluster volatility. It is important to remember that ARIMA is a method to linearly model the data and the forecast width remains constant because the model does not reflect recent changes or incorporate new information. In order to model volatility we use the Autoregressive Conditional Heteroscedasticity (ARCH) model. ARCH is a statistical model for time series data that describes the variance of the current error term as a function of the actual sizes of the previous time periods’ error terms.

The GARCH process is valid when the squared residuals are correlated. ACF and PACF plots clearly indicate significant correlation.

tsdisplay(ar.res^2 , main = 'Squared Residuals')

Another way to test the Heteroscedasticity of the squared residuals is to perform significance testing on \(\alpha_1\) and \(\beta_1\) parameters.

# Model specification
model.spec = ugarchspec(variance.model = list(model = 'sGARCH' , garchOrder = c(1 , 1)) , 
                        mean.model = list(armaOrder = c(0 , 0)))
model.fit = ugarchfit(spec = model.spec , data = ar.res , solver = 'solnp')

options(scipen = 999)
model.fit@fit$matcoef
             Estimate     Std. Error    t value   Pr(>|t|)
mu     -0.00006781119 0.000225598332 -0.3005837 0.76373195
omega   0.00001562176 0.000006460835  2.4179160 0.01560968
alpha1  0.16338532058 0.018628800583  8.7705765 0.00000000
beta1   0.77278283793 0.046550170076 16.6010744 0.00000000

Both \(\alpha_1\) and \(\beta_1\) are significantly different from zero, therefore it is reasonable to assume time-varying volatility of the residuals. With successive replacement of the \(\sigma_{t-1}^{2}\)

Value at Risk

Value at Risk (VaR) is a statistical measure of downside risk based on current position. It estimates how much a set of investments might lose given normal market conditions in a set time period. A VaR statistic has three components: a) time period, b) confidence level, c) loss ammount (or loss percentage). For 95% confidence level, we can say that the worst daily loss will not exceed VaR estimation. If we use historical data, we can estimate VaR by taking the 5% quantile value. For our data this estimation is:

qplot(vnm_logret , geom = 'histogram') + geom_histogram(fill = 'lightblue' , bins = 30) +
  geom_histogram(aes(vnm_logret[vnm_logret < quantile(vnm_logret , 0.05)]) , fill = 'red' , bins = 30) +
  labs(x = 'Daily Returns')
Don't know how to automatically pick scale for object of type xts/zoo. Defaulting to continuous.
`stat_bin()` using `bins = 30`. Pick better value with `binwidth`.

fitdist(distribution = 'std' , x = vnm_logret)$pars
         mu       sigma       shape 
0.000174047 0.017529840 2.827809536 

Red bars refer to returns lower than 5% quantile.

Distributional Properties

To estimate VaR, we need to properly define the corresponding quantile of the assumed distribution. For normal distribution, the quantile corresponding to a = 5% is -1.645. Empirical evidence suggest the assumption of normality often produces weak results. Jarque-Bera test can test the hypothesis that stock returns follow a normal distribution. \[JB = \frac{n+k-1}{6}* (S^2+\frac{1}{4}*(C-3^2))\] where S is skewness and C is kurtosis. A normal distributed sample would return a JB score of zero. The low p-value indicates stock returns are not normally distributed.

jarque.test(vnm_logret)
p2_1 = qplot(vnm_logret , geom = 'density') + geom_density(fill = 'blue' , alpha = 0.4) + 
    geom_density(aes(rnorm(200000 , 0 , sd(vnm_logret))) , fill = 'red' , alpha = 0.25) + 
    labs(x = '')

p2_2 = qplot(vnm_logret , geom = 'density') + geom_density(fill = 'blue' , alpha = 0.4) + 
    geom_density(aes(rnorm(200000 , 0 , sd(vnm_logret))) , fill = 'red' , alpha = 0.25) + 
    coord_cartesian(xlim = c(-0.07 , -0.02) , ylim = c(0 , 10)) + 
    geom_vline(xintercept = c(qnorm(p = c(0.01 , 0.05) , mean = mean(vnm_logret) , sd = sd(vnm_logret))) , 
               color = c('darkgreen' , 'green') , size = 1) + labs(x = 'Daily Returns')

grid.arrange(p2_1 , p2_2 , ncol = 1)

On the figure above, Density plots are shown for stock returns (blue) and normal distributed data (red). Vertical lines of the lower plot represent the normal corresponding quantile for a = 0.05 (light green) and a = 0.01 (dark green). Lower plot indicates that for 95% significance, normal distribution usage may overestimate the value at risk. However, for 99% significance level, a normal distribution would underestimate the risk. Student’s t-distribution

fitdist(distribution = 'std' , x = vnm_logret)$pars
         mu       sigma       shape 
0.000174047 0.017529840 2.827809536 
numnum = fitdist(distribution = 'std' , x = vnm_logret)$pars
numnum[3]
  shape 
2.82781 
cat("For a = 0.05 the quantile value of normal distribution is: " , 
    qnorm(p = 0.05) , "\n" ,
    "For a = 0.05 the quantile value of t-distribution is: " ,
    qdist(distribution = 'std' , shape = 2.9365168555 , p = 0.05) , "\n" , "\n" , 
    'For a = 0.01 the quantile value of normal distribution is: ' , 
    qnorm(p = 0.01) , "\n" , 
    "For a = 0.01 the quantile value of t-distribution is: " , 
    qdist(distribution = 'std' , shape = 2.9365168555 , p = 0.01) , sep = "")
For a = 0.05 the quantile value of normal distribution is: -1.644854
For a = 0.05 the quantile value of t-distribution is: -1.340812

For a = 0.01 the quantile value of normal distribution is: -2.326348
For a = 0.01 the quantile value of t-distribution is: -2.609131

Give some basic statistics

head(vnm_logret)
                   [,1]
2010-01-05  0.043412493
2010-01-06  0.006514681
2010-01-07 -0.030771659
2010-01-08 -0.031748698
2010-01-11 -0.013921339
2010-01-12 -0.033257222
summary(vnm_logret)
     Index              vnm_logret       
 Min.   :2010-01-05   Min.   :-0.072469  
 1st Qu.:2013-01-03   1st Qu.:-0.007086  
 Median :2016-01-08   Median : 0.000000  
 Mean   :2016-01-08   Mean   : 0.000758  
 3rd Qu.:2019-01-07   3rd Qu.: 0.007734  
 Max.   :2021-12-31   Max.   : 0.067646  
sd(vnm_logret)
[1] 0.01503838
skewness(vnm_logret)
[1] 0.14798
attr(,"method")
[1] "moment"
kurtosis(vnm_logret) - 3
[1] 0.1439202
attr(,"method")
[1] "excess"
qqnorm(vnm_logret)
qqline(vnm_logret, col = "blue")


# Calculate ACF
acf(vnm_logret,lag.max=40,plot=F)

Autocorrelations of series ‘vnm_logret’, by lag

     0      1      2      3      4      5      6      7      8      9     10 
 1.000  0.009  0.008 -0.047 -0.033  0.023 -0.001  0.029  0.005 -0.012  0.006 
    11     12     13     14     15     16     17     18     19     20     21 
 0.014 -0.010 -0.007  0.004 -0.041  0.030 -0.017 -0.016  0.002 -0.011  0.034 
    22     23     24     25     26     27     28     29     30     31     32 
-0.002  0.010 -0.002  0.000  0.009  0.000  0.011 -0.013  0.029 -0.006 -0.006 
    33     34     35     36     37     38     39     40 
-0.001 -0.003  0.018  0.017  0.007  0.015 -0.014  0.010 
# Plot ACF
acf(vnm_logret,lag.max=40)

Histogram and fitted normal distribution

h=hist(vnm_logret)
xfit = seq(min(vnm_logret), max(vnm_logret), length = 1000)
yfit = dnorm(xfit, mean = mean(vnm_logret), sd = sd(vnm_logret)) * diff(h$mids[1:2]) * length(vnm_logret)
lines(xfit, yfit, col = "blue", lwd = 2)

Historical Simulation for VaR

Using historical simulation for VaR at 5% with different estimation rolling window (500, 1000) ### (VaR, 0.05, 500)

alpha = 0.05
window = 500
VaR = c()
for (i in 1:(length(vnm_logret) - window)) {
  y = vnm_logret[i:(i + window)]
  ys = sort(y)
  ysta = ys[round(alpha * window)] # 25 is 5% of 500...
  VaR = c(VaR, ysta)
}
plot(df$date[(window+2):length(df$date)], VaR, type = 'l', main = "(VaR, 0.05, 500)", xlab = "Year", col = 'blue')

(VaR, 0.05, 750)

alpha = 0.05
window = 750
VaR = c()
for (i in 1:(length(vnm_logret) - window)) {
  y = vnm_logret[i:(i + window)]
  ys = sort(y)
  ysta = ys[round(alpha * window)] # 5% of 750...
  VaR = c(VaR, ysta)
}

plot(df$date[(window+2):length(df$date)], VaR, type = 'l', main = "(VaR, 0.05, 750)", xlab = "Year", col = 'blue')

(VaR, 0.05, 1000)

alpha = 0.05
window = 1000

VaR = c()
for (i in 1:(length(vnm_logret) - window)) {
  y = vnm_logret[i:(i + window)]
  ys = sort(y)
  ysta = ys[round(alpha * window)] # 5% of 1000...
  VaR = c(VaR, ysta)
}

plot( df$date[(window+2):length(df$date)], VaR, type = 'l', main = "(VaR, 0.05, 1000)", xlab = "Year", col = 'blue')

VaR forecasting

The ugarchroll method allows to perform a rolling estimation and forecasting of a model/dataset combination. It returns the distributional forecast parameters necessary to calculate any required measure on the forecasted density. We set the last 500 observations as test set and we perform a rolling moving 1-step ahead forecast of the conditional standard deviation. We re-estimate GARCH parameters every 50 observations.

var_roll_forecast = function(par_arr) {
  model.spec = ugarchspec(variance.model = list(model = 'sGARCH' , 
                                                garchOrder = par_arr) , 
                          mean.model = list(armaOrder = c(0 , 0)))
  model.fit = ugarchfit(spec = model.spec , data = ar.res , solver = 'solnp')
  
  model.fit@fit$matcoef
  model.roll = ugarchroll(spec = model.spec , data = vnm_logret, 
                          n.start = length(vnm_logret)-500, refit.every = 50,
                          refit.window = 'moving')
  VaR95_td = mean(vnm_logret) + 
    model.roll@forecast$density[,'Sigma'] * qdist(distribution = 'std',
                                                  shape = numnum[3], p = 0.05)
  return(VaR95_td)
}

Garch VaR vs Delta-normal approach

qplot(y = vnm_logret , x = 1:length(vnm_logret) , geom = 'point') + geom_point(colour = 'lightgrey' , size = 2) + 
  geom_line(aes(y = model.fit@fit$sigma*(-1.340812) , x = 1:length(vnm_logret)) , colour = 'red') +
  geom_hline(yintercept = sd(vnm_logret)*qnorm(0.05) , colour = 'darkgreen' , size = 1.2) + theme_light() + 
  labs(x = '' , y = 'Daily Returns' , title = 'Value at Risk Comparison')
Don't know how to automatically pick scale for object of type xts/zoo. Defaulting to continuous.

Red line denotes VaR produced by GARCH model and green line refers to delta-normal VaR.

Backtesting

p = c()
p[1] = pbinom(q = 0 , size = 500 , prob = 0.05)
for(i in 1:50){
    p[i] = (pbinom(q = (i-1) , size = 500 , prob = 0.05) - pbinom(q = (i-2) , size = 500 , prob = 0.05))
}
qplot(y = p , x = 1:50 , geom = 'line') + scale_x_continuous(breaks = seq(0 , 50 , 2)) + 
    annotate('segment' , x = c(16 , 35) , xend = c(16 , 35) , y = c(0 , 0) , yend = p[c(16 , 35)] , color = 'red' , 
             size = 1) + labs(y = 'Probability' , x = 'Number of Exceptions') + theme_light()

The plot above represent the distribution of probabilities for exceptions given by the binomial distribution. The expected number is 25 (=500obs. x 5%). Two red lines denote the 95% confidence level, the lower being 16 and the upper 35. Therefore, when we check the exceptions on the test set, we expect a number between 16 and 35 to state that GARCH model as successfully predictive.

show_VaR = function(VaR) {
  cat('Number of exceptions: ', (sum(vnm_logret[(length(vnm_logret)-499):length(vnm_logret)] < VaR)) , sep = '')
  qplot(y = VaR, x = 1:500, geom = 'line') +
    geom_point(aes(x = 1:500, y = vnm_logret[(length(vnm_logret)-499):length(vnm_logret)],
                   color = as.factor(vnm_logret[(length(vnm_logret)-499):length(vnm_logret)] < VaR)), size = 2) +
    scale_color_manual(values = c('gray', 'red')) +
    labs(y = 'Daily Returns', x = 'Test set Observation') + theme_light() +
    theme(legend.position = 'none')
}

VaR95_Garch = var_roll_forecast(c(1, 1))
show_VaR(VaR95_Garch)
Number of exceptions: 38

Using AR+GARCH (1,1) model to estimate Value at Risk of the returns at 5%

argarch_spec = ugarchspec(mean.model = list(armaOrder = c(1,0), 
                                              include.mean = T),
                            variance.model = list(model = "sGARCH",
                                                  garchOrder = c(1,1)),
                            distribution.model = "norm")
  
argarch_roll = ugarchroll(argarch_spec, 
                        data = vnm_logret, 
                        window.size = 300, 
                        calculate.VaR = TRUE, 
                        VaR.alpha = 0.05)

var_argarch_df = as.data.frame(argarch_roll, which = "VaR")

var_argarch_df = var_argarch_df %>% 
  mutate(date = as.Date(rownames(var_argarch_df)),
         var = `alpha(5%)`)

Plot these estimations for VaR on the same axes

var_argarch_df %>% 
      ggplot(aes(date,var)) + 
      geom_line(color = "red") + 
      scale_y_continuous()

Forecast VaR(5%) for 10 days

ugarchforecast(ugarchfit(argarch_spec, vnm_logret), n.ahead = 5)

*------------------------------------*
*       GARCH Model Forecast         *
*------------------------------------*
Model: sGARCH
Horizon: 5
Roll Steps: 0
Out of Sample: 0

0-roll forecast [T0=2021-12-31]:
       Series   Sigma
T+1 0.0010104 0.01071
T+2 0.0007003 0.01109
T+3 0.0006921 0.01143
T+4 0.0006919 0.01174
T+5 0.0006919 0.01203
---
title: "Project 1- Financial Risk Management 2"
subtitle: "Instructor: Dr. Ta Quoc Bao"
author: "Le Nguyen Dang Khoa"
date: "`r format(Sys.time(), '%d %B, %Y')`"
output: html_notebook
---

<style type = "text/css">

  h1.title {
    font-size: 2em !important;
  }
  
  h1.subtitle {
    font-size: 1.3em !important;
  }
  
</style>

# Introduction
# Libraries
```{r setup, include = FALSE}
knitr::opts_chunk$set(echo = TRUE)
library(ggthemes)
library(stats)
library(quarks)
library(forecast)
library(tseries)
library(gridExtra)
library(rugarch)
library(tidyquant)
library(psych)
library(e1071)
library(zoo)
library(moments)
library(readr)
library(dplyr)
library(nycflights13)
library(fGarch)
library(ggplot2)
library(tidyverse)
library(quadprog)
library(dplyr)
library(VNDS) # https://github.com/phamdinhkhanh/VNDS
```

# Data
```{r message=FALSE, warning=FALSE}
price = tq_get_cafef(symbol = 'VNM', from = '2010-01-01', to = '2022-01-01', src = 'CAFEF')
glimpse(as.data.frame(price))
```
## Dataframe: Date & Adjusted Price
```{r}
df <- price %>%
  arrange(date) %>%
  select(date, adjusted)
tail(df)
```
## Stock Price Plot
```{r}
ggplot(df, aes(date, adjusted, group = 1, color = adjusted)) + geom_line() +labs(x = "Date", y = "Price", title = "VNM")+ geom_hline(yintercept =mean(df$adjusted) , color = 'red')
```
## Log Return
```{r}
# Return Plot 
vnm_logret = xts(df$adjusted,as.Date(df$date))

vnm_logret = vnm_logret %>% 
  log %>% 
  diff

vnm_logret= vnm_logret[-1,]
```
### Log Return Plot
```{r}
qplot(x = 1:length(vnm_logret) , y = vnm_logret , geom = 'line') + geom_line(color = 'darkblue') + 
  geom_hline(yintercept = mean(vnm_logret) , color = 'red' , size = 1) + 
  labs(x = '' , y = 'Daily Returns')
```
To verify the stationarity of the returns, we utilize the Augmented Dickey-Fuller test where null hypothesis indicates non-stationary time series.
```{r warning=FALSE}
adf.test(vnm_logret)
```
## Box-Jenkins Methodology
For time series analysis, Box-Jenkins approach applies ARIMA models to find the best fit of a time series model that represent the stochastic process which generate time series. This method uses a three stage modelling approach: a) identification, b) estimation, c) diagnostic checking.
### Identification
```{r}
model.arima = auto.arima(vnm_logret , max.order = c(3 , 0 ,3) , stationary = TRUE , trace = T , ic = 'aicc')
```
### Estimation
```{r}
model.arima
```
### Diagnostics Checking
The procedure includes observing residual plot and its ACF & PACF diagram, and check Ljung-Box test result. If ACF & PACF of the model residuals show no significant lags, the selected model is appropriate.
```{r}
model.arima$residuals %>% ggtsdisplay(plot.type = 'hist' , lag.max = 14)
```
Both ACF and PACF plots are similar and autocorrelations seem to be equal to zero. The lower right corner plot represents the histogram of the residuals compared to a normal distribution N(0 , σ2).

```{r}
ar.res = model.arima$residuals
Box.test(model.arima$residuals , lag = 14 , fitdf = 2 , type = 'Ljung-Box')
```
We cannot reject the null hypothesis, therefore the process of the residuals behave like white noise so there is no indication of pattern that might be modeled.

## GARCH Implementation
Although ACF & PACF of residuals have no significant lags, the time series plot of residuals shows some cluster volatility. It is important to remember that ARIMA is a method to linearly model the data and the forecast width remains constant because the model does not reflect recent changes or incorporate new information. In order to model volatility we use the Autoregressive Conditional Heteroscedasticity (ARCH) model. ARCH is a statistical model for time series data that describes the variance of the current error term as a function of the actual sizes of the previous time periods’ error terms.

The GARCH process is valid when the squared residuals are correlated. ACF and PACF plots clearly indicate significant correlation.
```{r}
tsdisplay(ar.res^2 , main = 'Squared Residuals')
```
Another way to test the Heteroscedasticity of the squared residuals is to perform significance testing on $\alpha_1$ and $\beta_1$ parameters.
```{r}
# Model specification
model.spec = ugarchspec(variance.model = list(model = 'sGARCH' , garchOrder = c(1 , 1)) , 
                        mean.model = list(armaOrder = c(0 , 0)))
model.fit = ugarchfit(spec = model.spec , data = ar.res , solver = 'solnp')

options(scipen = 999)
model.fit@fit$matcoef
```
Both $\alpha_1$ and $\beta_1$ are significantly different from zero, therefore it is reasonable to assume time-varying volatility of the residuals.
With successive replacement of the $\sigma_{t-1}^{2}$ 

## Value at Risk
Value at Risk (VaR) is a statistical measure of downside risk based on current position. It estimates how much a set of investments might lose given normal market conditions in a set time period. A VaR statistic has three components: a) time period, b) confidence level, c) loss ammount (or loss percentage). For 95% confidence level, we can say that the worst daily loss will not exceed VaR estimation. If we use historical data, we can estimate VaR by taking the 5% quantile value. For our data this estimation is:

```{r}
qplot(vnm_logret , geom = 'histogram') + geom_histogram(fill = 'lightblue' , bins = 30) +
  geom_histogram(aes(vnm_logret[vnm_logret < quantile(vnm_logret , 0.05)]) , fill = 'red' , bins = 30) +
  labs(x = 'Daily Returns')

fitdist(distribution = 'std' , x = vnm_logret)$pars
```
Red bars refer to returns lower than 5% quantile.

## Distributional Properties
To estimate VaR, we need to properly define the corresponding quantile of the assumed distribution. For normal distribution, the quantile corresponding to a = 5% is -1.645. Empirical evidence suggest the assumption of normality often produces weak results. Jarque-Bera test can test the hypothesis that stock returns follow a normal distribution.
$$JB = \frac{n+k-1}{6}* (S^2+\frac{1}{4}*(C-3^2))$$
where S is skewness and C is kurtosis. A normal distributed sample would return a JB score of zero. The low p-value indicates stock returns are not normally distributed.
```{r}
jarque.test(vnm_logret)
p2_1 = qplot(vnm_logret , geom = 'density') + geom_density(fill = 'blue' , alpha = 0.4) + 
    geom_density(aes(rnorm(200000 , 0 , sd(vnm_logret))) , fill = 'red' , alpha = 0.25) + 
    labs(x = '')

p2_2 = qplot(vnm_logret , geom = 'density') + geom_density(fill = 'blue' , alpha = 0.4) + 
    geom_density(aes(rnorm(200000 , 0 , sd(vnm_logret))) , fill = 'red' , alpha = 0.25) + 
    coord_cartesian(xlim = c(-0.07 , -0.02) , ylim = c(0 , 10)) + 
    geom_vline(xintercept = c(qnorm(p = c(0.01 , 0.05) , mean = mean(vnm_logret) , sd = sd(vnm_logret))) , 
               color = c('darkgreen' , 'green') , size = 1) + labs(x = 'Daily Returns')

grid.arrange(p2_1 , p2_2 , ncol = 1)
```
On the figure above, Density plots are shown for stock returns (blue) and normal distributed data (red). Vertical lines of the lower plot represent the normal corresponding quantile for a = 0.05 (light green) and a = 0.01 (dark green). Lower plot indicates that for 95% significance, normal distribution usage may overestimate the value at risk. However, for 99% significance level, a normal distribution would underestimate the risk.
**Student’s t-distribution**
```{r}
fitdist(distribution = 'std' , x = vnm_logret)$pars

numnum = fitdist(distribution = 'std' , x = vnm_logret)$pars
numnum[3]
cat("For a = 0.05 the quantile value of normal distribution is: " , 
    qnorm(p = 0.05) , "\n" ,
    "For a = 0.05 the quantile value of t-distribution is: " ,
    qdist(distribution = 'std' , shape = 2.9365168555 , p = 0.05) , "\n" , "\n" , 
    'For a = 0.01 the quantile value of normal distribution is: ' , 
    qnorm(p = 0.01) , "\n" , 
    "For a = 0.01 the quantile value of t-distribution is: " , 
    qdist(distribution = 'std' , shape = 2.9365168555 , p = 0.01) , sep = "")
```
### Give some basic statistics
```{r}
head(vnm_logret)
```
```{r}
summary(vnm_logret)
```
```{r}
sd(vnm_logret)
```
```{r}
skewness(vnm_logret)
```
```{r}
kurtosis(vnm_logret) - 3
```
```{r}
qqnorm(vnm_logret)
qqline(vnm_logret, col = "blue")
```
```{r}

# Calculate ACF
acf(vnm_logret,lag.max=40,plot=F)

# Plot ACF
acf(vnm_logret,lag.max=40)
```
### Histogram and fitted normal distribution
```{r}
h=hist(vnm_logret)
xfit = seq(min(vnm_logret), max(vnm_logret), length = 1000)
yfit = dnorm(xfit, mean = mean(vnm_logret), sd = sd(vnm_logret)) * diff(h$mids[1:2]) * length(vnm_logret)
lines(xfit, yfit, col = "blue", lwd = 2)
```

# Historical Simulation for VaR
Using historical simulation for VaR at 5% with different estimation rolling window (500, 1000)
### (VaR, 0.05, 500)
```{r}
alpha = 0.05
window = 500
VaR = c()
for (i in 1:(length(vnm_logret) - window)) {
  y = vnm_logret[i:(i + window)]
  ys = sort(y)
  ysta = ys[round(alpha * window)] # 25 is 5% of 500...
  VaR = c(VaR, ysta)
}
plot(df$date[(window+2):length(df$date)], VaR, type = 'l', main = "(VaR, 0.05, 500)", xlab = "Year", col = 'blue')
```
### (VaR, 0.05, 750)
```{r}
alpha = 0.05
window = 750
VaR = c()
for (i in 1:(length(vnm_logret) - window)) {
  y = vnm_logret[i:(i + window)]
  ys = sort(y)
  ysta = ys[round(alpha * window)] # 5% of 750...
  VaR = c(VaR, ysta)
}

plot(df$date[(window+2):length(df$date)], VaR, type = 'l', main = "(VaR, 0.05, 750)", xlab = "Year", col = 'blue')
```
### (VaR, 0.05, 1000)
```{r}
alpha = 0.05
window = 1000

VaR = c()
for (i in 1:(length(vnm_logret) - window)) {
  y = vnm_logret[i:(i + window)]
  ys = sort(y)
  ysta = ys[round(alpha * window)] # 5% of 1000...
  VaR = c(VaR, ysta)
}

plot( df$date[(window+2):length(df$date)], VaR, type = 'l', main = "(VaR, 0.05, 1000)", xlab = "Year", col = 'blue')
```

## VaR forecasting
The ugarchroll method allows to perform a rolling estimation and forecasting of a model/dataset combination. It returns the distributional forecast parameters necessary to calculate any required measure on the forecasted density. We set the last 500 observations as test set and we perform a rolling moving 1-step ahead forecast of the conditional standard deviation. We re-estimate GARCH parameters every 50 observations.
```{r}
var_roll_forecast = function(par_arr) {
  model.spec = ugarchspec(variance.model = list(model = 'sGARCH' , 
                                                garchOrder = par_arr) , 
                          mean.model = list(armaOrder = c(0 , 0)))
  model.fit = ugarchfit(spec = model.spec , data = ar.res , solver = 'solnp')
  
  model.fit@fit$matcoef
  model.roll = ugarchroll(spec = model.spec , data = vnm_logret, 
                          n.start = length(vnm_logret)-500, refit.every = 50,
                          refit.window = 'moving')
  VaR95_td = mean(vnm_logret) + 
    model.roll@forecast$density[,'Sigma'] * qdist(distribution = 'std',
                                                  shape = numnum[3], p = 0.05)
  return(VaR95_td)
}
```
## Garch VaR vs Delta-normal approach
```{r}
qplot(y = vnm_logret , x = 1:length(vnm_logret) , geom = 'point') + geom_point(colour = 'lightgrey' , size = 2) + 
  geom_line(aes(y = model.fit@fit$sigma*(-1.340812) , x = 1:length(vnm_logret)) , colour = 'red') +
  geom_hline(yintercept = sd(vnm_logret)*qnorm(0.05) , colour = 'darkgreen' , size = 1.2) + theme_light() + 
  labs(x = '' , y = 'Daily Returns' , title = 'Value at Risk Comparison')
```
Red line denotes VaR produced by GARCH model and green line refers to delta-normal VaR.

## Backtesting
```{r}
p = c()
p[1] = pbinom(q = 0 , size = 500 , prob = 0.05)
for(i in 1:50){
    p[i] = (pbinom(q = (i-1) , size = 500 , prob = 0.05) - pbinom(q = (i-2) , size = 500 , prob = 0.05))
}
qplot(y = p , x = 1:50 , geom = 'line') + scale_x_continuous(breaks = seq(0 , 50 , 2)) + 
    annotate('segment' , x = c(16 , 35) , xend = c(16 , 35) , y = c(0 , 0) , yend = p[c(16 , 35)] , color = 'red' , 
             size = 1) + labs(y = 'Probability' , x = 'Number of Exceptions') + theme_light()
```
The plot above represent the distribution of probabilities for exceptions given by the binomial distribution. The expected number is 25 (=500obs. x 5%). Two red lines denote the 95% confidence level, the lower being 16 and the upper 35. Therefore, when we check the exceptions on the test set, we expect a number between 16 and 35 to state that GARCH model as successfully predictive.
```{r}
show_VaR = function(VaR) {
  cat('Number of exceptions: ', (sum(vnm_logret[(length(vnm_logret)-499):length(vnm_logret)] < VaR)) , sep = '')
  qplot(y = VaR, x = 1:500, geom = 'line') +
    geom_point(aes(x = 1:500, y = vnm_logret[(length(vnm_logret)-499):length(vnm_logret)],
                   color = as.factor(vnm_logret[(length(vnm_logret)-499):length(vnm_logret)] < VaR)), size = 2) +
    scale_color_manual(values = c('gray', 'red')) +
    labs(y = 'Daily Returns', x = 'Test set Observation') + theme_light() +
    theme(legend.position = 'none')
}

VaR95_Garch = var_roll_forecast(c(1, 1))
show_VaR(VaR95_Garch)
```

# Using AR+GARCH (1,1) model to estimate Value at Risk of the returns at 5%
```{r,warning = F,message = T}
argarch_spec = ugarchspec(mean.model = list(armaOrder = c(1,0), 
                                              include.mean = T),
                            variance.model = list(model = "sGARCH",
                                                  garchOrder = c(1,1)),
                            distribution.model = "norm")
  
argarch_roll = ugarchroll(argarch_spec, 
                        data = vnm_logret, 
                        window.size = 300, 
                        calculate.VaR = TRUE, 
                        VaR.alpha = 0.05)

var_argarch_df = as.data.frame(argarch_roll, which = "VaR")

var_argarch_df = var_argarch_df %>% 
  mutate(date = as.Date(rownames(var_argarch_df)),
         var = `alpha(5%)`)
```

# Plot these estimations for VaR on the same axes
```{r,warning = F,message = T}
var_argarch_df %>% 
      ggplot(aes(date,var)) + 
      geom_line(color = "red") + 
      scale_y_continuous()
```

# Forecast VaR(5%) for 10 days

```{r,warning = F,message = T}
ugarchforecast(ugarchfit(argarch_spec, vnm_logret), n.ahead = 5)
```





