Problem Set 3

LAM Chun Ming (58555905)

please find the full version here https://rpubs.com/TCML/1254698

library('TSA')
library('fGarch')
library('parallel')
library('rugarch')
library('quantmod')
library('tseries')
library('forecast')
library('MSwM')

Question 1

1a) download VIX data

getSymbols("VIX", from = '2006-01-01', to = '2024-10-22')
Warning: VIX contains missing values. Some functions will not work if objects contain missing values in the middle of the series. Consider using na.omit(), na.approx(), na.fill(), etc to remove or replace them.
[1] "VIX"
vix = as.numeric(VIX[,6])
vix = na.omit(vix)

dvix = diff(vix)

1b.1) Write down an equivalent AR representation

ARCH(p) model is given as follows \[ h_t=\alpha_0 + \sum_{i=1}^{p}\alpha_i\varepsilon_{t-i}^2 \\ \varepsilon_t =z_t \sqrt{h_t} , \space \space z_t \sim i.i.d(0,1) \] we can use the fact that we can always decompose \(\varepsilon_t^2 = h_t + v_t\) where \(v_t\) is some arbitrary error, and show that this is the same as AR(p) on the squared error (or the de-meaned process) \(\varepsilon_t^2\)

\[ \varepsilon_t^2 = \alpha_0 + \sum_{i=1}^p\alpha_i\varepsilon_{t-i}^2 +v_t \]

1b.2) Explain and show the best order q can be determined

because, this the equivalent to the AR(p) process on the squared error term, we can run PACF on the squared error, as we would determined a AR process, following which we use an MLE method to fit the actual parameters

here we first find the de-meaned process by first fitting an ARIMA model

# uses EACF on the differenced VIX (to remove stationary)
eacf(dvix)
AR/MA
  0 1 2 3 4 5 6 7 8 9 10 11 12 13
0 x o o o x o x o o o o  o  o  o 
1 x x o o x o o o o o o  o  o  o 
2 x o o o x o o o o o o  o  o  o 
3 x x o o o o x x o o o  o  o  o 
4 x x x x o o o o o o o  o  o  o 
5 x x o x x o o o o o o  o  o  o 
6 x x o x x x x o o o o  o  o  o 
7 x x o x x o x o o o o  o  o  o 
m_arima = arima(vix, order = c(3,1,2))

# checking model goodness of fit - cannot reject the Null Hypothesis at 5% level - i.e. there is no serial dependency in the lag 
Box.test(m_arima$residuals,lag = 10)

    Box-Pierce test

data:  m_arima$residuals
X-squared = 13.222, df = 10, p-value = 0.2115
# taking residuals 
res= m_arima$residuals

after fitting the ARIMA process, we fit an ARCH model, by considering it’s AR equivalence

pacf(res^2)

# PACF suggests AR of 3 <=> ARCH(3), 

# fitting model
model_ARCH3 = garchFit(~garch(3,0), data = res , trace = F)

# here all values are significant
summary(model_ARCH3)

Title:
 GARCH Modelling 

Call:
 garchFit(formula = ~garch(3, 0), data = res, trace = F) 

Mean and Variance Equation:
 data ~ garch(3, 0)
<environment: 0x000001bff65eb650>
 [data = res]

Conditional Distribution:
 norm 

Coefficient(s):
         mu        omega       alpha1       alpha2       alpha3  
-2.1084e+01   9.2171e+04   6.9268e-02   1.5041e-01   2.4924e-01  

Std. Errors:
 based on Hessian 

Error Analysis:
         Estimate  Std. Error  t value Pr(>|t|)    
mu     -2.108e+01   1.178e+01   -1.790 0.073387 .  
omega   9.217e+04   5.942e+03   15.512  < 2e-16 ***
alpha1  6.927e-02   3.124e-02    2.217 0.026603 *  
alpha2  1.504e-01   4.881e-02    3.081 0.002060 ** 
alpha3  2.492e-01   6.832e-02    3.648 0.000264 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Log Likelihood:
 -5742.805    normalized:  -7.297083 

Description:
 Fri Dec  6 16:27:06 2024 by user: Toby Lam 


Standardised Residuals Tests:
                                   Statistic   p-Value
 Jarque-Bera Test   R    Chi^2  1.775535e+05 0.0000000
 Shapiro-Wilk Test  R    W      6.888432e-01 0.0000000
 Ljung-Box Test     R    Q(10)  1.193094e+01 0.2897054
 Ljung-Box Test     R    Q(15)  1.381473e+01 0.5396245
 Ljung-Box Test     R    Q(20)  1.664868e+01 0.6756541
 Ljung-Box Test     R^2  Q(10)  7.056540e-01 0.9999660
 Ljung-Box Test     R^2  Q(15)  7.393540e-01 1.0000000
 Ljung-Box Test     R^2  Q(20)  1.106019e+00 1.0000000
 LM Arch Test       R    TR^2   5.042072e-01 0.9999997

Information Criterion Statistics:
     AIC      BIC      SIC     HQIC 
14.60687 14.63653 14.60679 14.61828 

1b.3) write down the fitted ARCH & AR model

fitted at the

\[ ARCH: h_t = 91270 + 0.06927 \varepsilon_{t-1}^2 + 0.1504\varepsilon_{t-2}^2 + 0.2492\varepsilon_{t-3}^2\\ AR: \varepsilon_t^2 = 91270 + 0.06927 \varepsilon_{t-1}^2 + 0.1504\varepsilon_{t-2}^2 + 0.2492\varepsilon_{t-3}^2 + v_t \\ \]

1c.1) Write down an ARMA equivalent for GARCH(m,s) GARCH model is given as follows

\[ \varepsilon_t = z_t \sqrt{h_t} \ \ s.t.: z_t \sim i.i.d(0,1)\\ h_t = \alpha_0 + \sum_{i=1}^m \alpha_i\varepsilon_{t-i}^2 + \sum_{j=1}^s \beta_j h_{t-j} \]

again decomposing \(\varepsilon_t^2 = h_t + v_t\),

\[ \varepsilon_t^2 = \alpha_0 + \sum_{i=1}^m \alpha_i \varepsilon_{t-i}^2 + \sum_{j=1}^s \beta_j (\varepsilon_{t-j}^2-v_{t-j}) + v_t \]

by regrouping into \(\varepsilon_{t-j}^2 \ \& \ v_{t-j}\) , note that \(I\{\cdot\}\) is the indicator function

\[ \varepsilon_t^2 = \alpha_0 + \sum_{i=1}^m \tilde\alpha_i \varepsilon_{t-i}^2 + \sum_{j=1}^s \tilde\beta_j v_{t-j} + v_t\\ s.t. : \ \tilde\alpha_i = \alpha_iI\{i\leq m\} + \beta_i I\{i\leq s\}\\ \tilde \beta_j = -\beta_j \]

1c.2) fit and write down the model

model =  garchFit(~garch(1,1), data = res, trace = F)

summary(model)

Title:
 GARCH Modelling 

Call:
 garchFit(formula = ~garch(1, 1), data = res, trace = F) 

Mean and Variance Equation:
 data ~ garch(1, 1)
<environment: 0x000001bff16e69c8>
 [data = res]

Conditional Distribution:
 norm 

Coefficient(s):
         mu        omega       alpha1        beta1  
-1.3696e+01   1.2860e+04   6.8775e-02   8.2912e-01  

Std. Errors:
 based on Hessian 

Error Analysis:
         Estimate  Std. Error  t value Pr(>|t|)    
mu     -1.370e+01   1.131e+01   -1.211 0.226068    
omega   1.286e+04   2.779e+03    4.628 3.69e-06 ***
alpha1  6.878e-02   1.817e-02    3.785 0.000153 ***
beta1   8.291e-01   3.446e-02   24.059  < 2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Log Likelihood:
 -5707.395    normalized:  -7.25209 

Description:
 Fri Dec  6 16:43:44 2024 by user: Toby Lam 


Standardised Residuals Tests:
                                   Statistic   p-Value
 Jarque-Bera Test   R    Chi^2  3.000255e+05 0.0000000
 Shapiro-Wilk Test  R    W      6.927818e-01 0.0000000
 Ljung-Box Test     R    Q(10)  1.143145e+01 0.3249062
 Ljung-Box Test     R    Q(15)  1.325227e+01 0.5828200
 Ljung-Box Test     R    Q(20)  1.599566e+01 0.7168933
 Ljung-Box Test     R^2  Q(10)  5.349208e-02 1.0000000
 Ljung-Box Test     R^2  Q(15)  8.769032e-02 1.0000000
 Ljung-Box Test     R^2  Q(20)  1.235536e-01 1.0000000
 LM Arch Test       R    TR^2   7.811317e-02 1.0000000

Information Criterion Statistics:
     AIC      BIC      SIC     HQIC 
14.51435 14.53807 14.51429 14.52347 

fitted model

\[ h_t = 12860 + 0.06878 \varepsilon_{t-1}^2 + 0.8291 h_{t-1} \]

1d) fit model assuming a student - t distribution

model =  garchFit(~garch(1,1), data = res, cond.dist = 'std', trace = F)

summary(model)

Title:
 GARCH Modelling 

Call:
 garchFit(formula = ~garch(1, 1), data = res, cond.dist = "std", 
    trace = F) 

Mean and Variance Equation:
 data ~ garch(1, 1)
<environment: 0x000001bfe7628170>
 [data = res]

Conditional Distribution:
 std 

Coefficient(s):
      mu     omega    alpha1     beta1     shape  
-1.12649  28.30229   0.63266   0.72633   2.69061  

Std. Errors:
 based on Hessian 

Error Analysis:
        Estimate  Std. Error  t value Pr(>|t|)    
mu      -1.12649     2.41367   -0.467  0.64071    
omega   28.30229   141.73943    0.200  0.84173    
alpha1   0.63266     0.19732    3.206  0.00134 ** 
beta1    0.72633     0.02888   25.152  < 2e-16 ***
shape    2.69061     0.28504    9.439  < 2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Log Likelihood:
 -5404.256    normalized:  -6.866907 

Description:
 Fri Dec  6 16:45:13 2024 by user: Toby Lam 


Standardised Residuals Tests:
                                   Statistic p-Value
 Jarque-Bera Test   R    Chi^2  1.976041e+07       0
 Shapiro-Wilk Test  R    W      3.459989e-02       0
 Ljung-Box Test     R    Q(10)  5.426508e-02       1
 Ljung-Box Test     R    Q(15)  5.818304e-02       1
 Ljung-Box Test     R    Q(20)  8.217111e-02       1
 Ljung-Box Test     R^2  Q(10)  1.324736e-02       1
 Ljung-Box Test     R^2  Q(15)  2.005019e-02       1
 Ljung-Box Test     R^2  Q(20)  2.694674e-02       1
 LM Arch Test       R    TR^2   1.598610e-02       1

Information Criterion Statistics:
     AIC      BIC      SIC     HQIC 
13.74652 13.77618 13.74644 13.75792 

the fitted model \[ h_t = 28.30 + 0.6327\varepsilon_{t-1}^2 + 0.7263 h_{t-1} \]

1e.1) explain how to choose ARMA orders

following work done in part 1a)

# test for stationarity in vix data ; we cannot reject the Null Hypothesis data is non stationary
adf.test(vix)

    Augmented Dickey-Fuller Test

data:  vix
Dickey-Fuller = -1.8035, Lag order = 9, p-value = 0.6615
alternative hypothesis: stationary
# differencing to remove stationarity, test again; we can reject the Null Hypothesis - i.e. the data is stationary
adf.test(dvix)
Warning in adf.test(dvix) : p-value smaller than printed p-value

    Augmented Dickey-Fuller Test

data:  dvix
Dickey-Fuller = -8.9308, Lag order = 9, p-value = 0.01
alternative hypothesis: stationary
# use EACF to select for model - this produces candidate model ARMA(0,1) & ARMA(2,1) 
eacf(dvix)
AR/MA
  0 1 2 3 4 5 6 7 8 9 10 11 12 13
0 x o o o x o x o o o o  o  o  o 
1 x x o o x o o o o o o  o  o  o 
2 x o o o x o o o o o o  o  o  o 
3 x x o o o o x x o o o  o  o  o 
4 x x x x o o o o o o o  o  o  o 
5 x x o x x o o o o o o  o  o  o 
6 x x o x x x x o o o o  o  o  o 
7 x x o x x o x o o o o  o  o  o 
# try to fit for ARMA(0,1)
m1 = arima(vix, order = c(0,1,1))

# test for validity - can reject the null hypothesis at 5% - there is serial dependencies in the residual
Box.test(m1$residuals,lag = 10)

    Box-Pierce test

data:  m1$residuals
X-squared = 18.194, df = 10, p-value = 0.05178
# try second candidate 
m2 = arima(vix, order = c(2,1,1))

# test for validity - can reject the null hypothesis at 5% - there is serial dependencies in the residual  
Box.test(m2$residuals,lag = 10)

    Box-Pierce test

data:  m2$residuals
X-squared = 20.766, df = 10, p-value = 0.02279
# try third candidate 

m3 = arima(vix, order = c(3,1,2))

# test for validity - cannot reject the null hypothesis at 5% - there is no serial dependencies in the residual
Box.test(m3$residuals,lag = 10)

    Box-Pierce test

data:  m3$residuals
X-squared = 13.222, df = 10, p-value = 0.2115
# accept the ARMA(3,2) on the differenced data 

1e.2) write down the fitted model

first fit the model using an MLE method


model =  garchFit(~arma(3,2)+garch(1,1), data = dvix,  trace = F)

summary(model)

Title:
 GARCH Modelling 

Call:
 garchFit(formula = ~arma(3, 2) + garch(1, 1), data = dvix, trace = F) 

Mean and Variance Equation:
 data ~ arma(3, 2) + garch(1, 1)
<environment: 0x000001bff358d200>
 [data = dvix]

Conditional Distribution:
 norm 

Coefficient(s):
         mu          ar1          ar2          ar3          ma1          ma2        omega       alpha1        beta1  
-4.6882e+00   9.6053e-01  -4.1495e-01   7.9452e-02  -1.0000e+00   3.4651e-01   1.5574e+04   9.4341e-02   7.8623e-01  

Std. Errors:
 based on Hessian 

Error Analysis:
         Estimate  Std. Error  t value Pr(>|t|)    
mu     -4.688e+00   4.010e+00   -1.169   0.2423    
ar1     9.605e-01   2.276e-01    4.220 2.44e-05 ***
ar2    -4.149e-01   1.951e-01   -2.127   0.0334 *  
ar3     7.945e-02   5.023e-02    1.582   0.1137    
ma1    -1.000e+00   2.258e-01   -4.428 9.49e-06 ***
ma2     3.465e-01   1.849e-01    1.874   0.0610 .  
omega   1.557e+04   2.951e+03    5.277 1.31e-07 ***
alpha1  9.434e-02   2.328e-02    4.053 5.05e-05 ***
beta1   7.862e-01   3.796e-02   20.714  < 2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Log Likelihood:
 -5672.15    normalized:  -7.216475 

Description:
 Fri Dec  6 16:45:58 2024 by user: Toby Lam 


Standardised Residuals Tests:
                                   Statistic   p-Value
 Jarque-Bera Test   R    Chi^2  3.863743e+05 0.0000000
 Shapiro-Wilk Test  R    W      6.770924e-01 0.0000000
 Ljung-Box Test     R    Q(10)  7.165589e+00 0.7097254
 Ljung-Box Test     R    Q(15)  9.637014e+00 0.8419305
 Ljung-Box Test     R    Q(20)  1.156437e+01 0.9302548
 Ljung-Box Test     R^2  Q(10)  7.277833e-02 1.0000000
 Ljung-Box Test     R^2  Q(15)  1.149614e-01 1.0000000
 Ljung-Box Test     R^2  Q(20)  2.076563e-01 1.0000000
 LM Arch Test       R    TR^2   1.078846e-01 1.0000000

Information Criterion Statistics:
     AIC      BIC      SIC     HQIC 
14.45585 14.50929 14.45559 14.47640 

fitted model

\[ X_t = 0.9605 X_{t-1} -0.4149 X_{t-2} + 0.07945 X_{t-3} - \varepsilon_{t-1} + 0.3465 \varepsilon_{t-2}+\varepsilon_t\\ h_t = 15570 + 0.09434 \varepsilon_{t-1}^2 + 0.7862 h_{t-1} \]

Question 2

2a) expected value of returns the Null hypothesis states that the mean of the daily log percentage returns is 0, whilst the alternative is that it is not 0.

here the p value is 0.1105, the sample statistic has a 11.05% probability to be observed given an assumed Null Hypothesis. therefore we cannot reject the Null Hypothesis at the 5% level. That is to say, given our sample, we do not see sufficient statistical evidence that the population daily log percentage return is different from 0.

getSymbols("WMT",from = "2018-01-02", to = "2024-11-01")
[1] "WMT"
# find the log percentage returns 
wmt = WMT$WMT.Close
lret_wmt = log(wmt/lag(wmt))*100

# format data
lret_wmt = na.omit(lret_wmt)
lret_wmt = as.numeric(lret_wmt)

# find the mean
mean(lret_wmt)
[1] 0.053156
# conduct t test
t.test(lret_wmt)

    One Sample t-test

data:  lret_wmt
t = 1.5966, df = 1718, p-value = 0.1105
alternative hypothesis: true mean is not equal to 0
95 percent confidence interval:
 -0.01214204  0.11845404
sample estimates:
mean of x 
 0.053156 

2b) are there serial correlation in the return and squared return

Taking the Ljung Box test shows that, we can reject the Null Hypothesis for both the log returns and the log squared returns. that is, there is serial dependencies in both time series


Box.test(lret_wmt, lag = 10, type = "Ljung")

    Box-Ljung test

data:  lret_wmt
X-squared = 39.364, df = 10, p-value = 2.192e-05
Box.test(lret_wmt^2, lag = 10, type = "Ljung")

    Box-Ljung test

data:  lret_wmt^2
X-squared = 278.83, df = 10, p-value < 2.2e-16

2c) fit an ARCH - GARCH model to the rt series

the model seems adequate - the QQ plot shows reasonable good fit for most of the central quantile data points, Ljung Box test on the residuals also shows no serial dependencies in the residual


# use EACF
eacf(lret_wmt)
AR/MA
  0 1 2 3 4 5 6 7 8 9 10 11 12 13
0 x o o x o o o x x o o  o  o  o 
1 o o o x o o o o x o o  o  o  o 
2 x o o x o o o o x o o  o  o  o 
3 x o x x o o o o x o o  o  o  o 
4 x x x x o o o o x o o  o  o  o 
5 x x o x x o o x x o o  o  o  o 
6 x x o x x x o o o o o  o  o  o 
7 x x x x x x x x o o o  o  o  o 
# candidate ARMA(1,0) - LB test sufficient: we can reject the null hypothesis at 5% - i.e. there is serial dependencies in the residual
m1 = arima(lret_wmt, c(1,0,0))
Box.test(m1$residuals, lag = 10 , type = "Ljung")

    Box-Ljung test

data:  m1$residuals
X-squared = 27.644, df = 10, p-value = 0.002058
# candidate ARMA(3,1) - LB test sufficient: we can reject the null hypothesis at 5% - i.e. there is serial dependencies in the residual 
m2 = arima(lret_wmt, c(3,0,1))
Box.test(m2$residuals, lag = 10 , type = "Ljung")

    Box-Ljung test

data:  m2$residuals
X-squared = 24.656, df = 10, p-value = 0.006038
# candidate ARMA(5,2)
m3 = arima(lret_wmt, c(5,0,2))
Box.test(m3$residuals, lag = 10 , type = "Ljung")

    Box-Ljung test

data:  m3$residuals
X-squared = 13.308, df = 10, p-value = 0.2069
#fit ARMA - GARCH model 
model_C1 = garchFit(~arma(5,2)+garch(1,1),lret_wmt,trace = F)
Warning in arima(.series$x, order = c(u, 0, v), include.mean = include.mean) :
  possible convergence problem: optim gave code = 1
summary(model_C1)

Title:
 GARCH Modelling 

Call:
 garchFit(formula = ~arma(5, 2) + garch(1, 1), data = lret_wmt, 
    trace = F) 

Mean and Variance Equation:
 data ~ arma(5, 2) + garch(1, 1)
<environment: 0x000001bff6582df0>
 [data = lret_wmt]

Conditional Distribution:
 norm 

Coefficient(s):
        mu         ar1         ar2         ar3         ar4         ar5         ma1         ma2       omega      alpha1       beta1  
 0.1290380  -0.3900016  -0.7518651  -0.0465791  -0.0684031   0.0069665   0.3222041   0.6914670   0.2000378   0.1174106   0.7797547  

Std. Errors:
 based on Hessian 

Error Analysis:
        Estimate  Std. Error  t value Pr(>|t|)    
mu      0.129038    0.061355    2.103   0.0355 *  
ar1    -0.390002    0.180382   -2.162   0.0306 *  
ar2    -0.751865    0.181482   -4.143 3.43e-05 ***
ar3    -0.046579    0.039658   -1.175   0.2402    
ar4    -0.068403    0.030796   -2.221   0.0263 *  
ar5     0.006966    0.031635    0.220   0.8257    
ma1     0.322204    0.177503    1.815   0.0695 .  
ma2     0.691467    0.175721    3.935 8.32e-05 ***
omega   0.200038    0.043933    4.553 5.28e-06 ***
alpha1  0.117411    0.023050    5.094 3.51e-07 ***
beta1   0.779755    0.037184   20.970  < 2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Log Likelihood:
 -2848.271    normalized:  -1.656935 

Description:
 Fri Dec  6 16:49:17 2024 by user: Toby Lam 


Standardised Residuals Tests:
                                   Statistic   p-Value
 Jarque-Bera Test   R    Chi^2  1.801635e+04 0.0000000
 Shapiro-Wilk Test  R    W      8.817975e-01 0.0000000
 Ljung-Box Test     R    Q(10)  4.577784e+00 0.9175425
 Ljung-Box Test     R    Q(15)  5.656693e+00 0.9849556
 Ljung-Box Test     R    Q(20)  9.070822e+00 0.9820724
 Ljung-Box Test     R^2  Q(10)  1.597135e+00 0.9985996
 Ljung-Box Test     R^2  Q(15)  2.281165e+00 0.9999296
 Ljung-Box Test     R^2  Q(20)  2.745289e+00 0.9999981
 LM Arch Test       R    TR^2   1.699656e+00 0.9997460

Information Criterion Statistics:
     AIC      BIC      SIC     HQIC 
3.326667 3.361539 3.326586 3.339570 
plot(model_C1,which = 13)

fitted model

\[ X_t = 0.1290 - 0.3900 X_{t-1} -0.7519 X_{t-2} -0.04658 X_{t-3} -0.06840 X_{t-4} +0.006966 X_{t-5} + 0.3222\varepsilon_{t-1} + 0.6915 \varepsilon_{t-2}\\ h_t = 0.2000 + 0.1174 \varepsilon_{t-1}^2 +0.7798 h_{t-1} \]

2d) IGARCH Model

fitting the IGARCH(1,1) model to the time series \(z_t\)


zret = lret_wmt - mean(lret_wmt)

spec1=ugarchspec(variance.model=list(model="iGARCH",garchOrder=c(1,1)),mean.model=list(armaOrder=c(0,0)))
mm=ugarchfit(zret,spec=spec1)
mm

*---------------------------------*
*          GARCH Model Fit        *
*---------------------------------*

Conditional Variance Dynamics   
-----------------------------------
GARCH Model : iGARCH(1,1)
Mean Model  : ARFIMA(0,0,0)
Distribution    : norm 

Optimal Parameters
------------------------------------
        Estimate  Std. Error  t value Pr(>|t|)
mu      0.000000    0.029637   0.0000  1.0e+00
omega   0.007722    0.001926   4.0087  6.1e-05
alpha1  0.044440    0.006565   6.7697  0.0e+00
beta1   0.955560          NA       NA       NA

Robust Standard Errors:
        Estimate  Std. Error  t value Pr(>|t|)
mu      0.000000    0.040574   0.0000 1.000000
omega   0.007722    0.005223   1.4785 0.139270
alpha1  0.044440    0.025872   1.7177 0.085847
beta1   0.955560          NA       NA       NA

LogLikelihood : -2901.029 

Information Criteria
------------------------------------
                   
Akaike       3.3787
Bayes        3.3883
Shibata      3.3787
Hannan-Quinn 3.3823

Weighted Ljung-Box Test on Standardized Residuals
------------------------------------
                        statistic p-value
Lag[1]                      2.537  0.1112
Lag[2*(p+q)+(p+q)-1][2]     2.643  0.1754
Lag[4*(p+q)+(p+q)-1][5]     3.876  0.2699
d.o.f=0
H0 : No serial correlation

Weighted Ljung-Box Test on Standardized Squared Residuals
------------------------------------
                        statistic p-value
Lag[1]                     0.7211  0.3958
Lag[2*(p+q)+(p+q)-1][5]    0.8096  0.9011
Lag[4*(p+q)+(p+q)-1][9]    1.1217  0.9806
d.o.f=2

Weighted ARCH LM Tests
------------------------------------
            Statistic Shape Scale P-Value
ARCH Lag[3]  0.003869 0.500 2.000  0.9504
ARCH Lag[5]  0.123037 1.440 1.667  0.9824
ARCH Lag[7]  0.314495 2.315 1.543  0.9920

Nyblom stability test
------------------------------------
Joint Statistic:  1.2822
Individual Statistics:              
mu     0.03649
omega  0.26378
alpha1 0.18205

Asymptotic Critical Values (10% 5% 1%)
Joint Statistic:         0.846 1.01 1.35
Individual Statistic:    0.35 0.47 0.75

Sign Bias Test
------------------------------------


Adjusted Pearson Goodness-of-Fit Test:
------------------------------------
  group statistic p-value(g-1)
1    20     133.5    3.218e-19
2    30     145.2    2.071e-17
3    40     154.1    1.303e-15
4    50     172.4    1.204e-15


Elapsed time : 0.0635159 

the fitted model \[ h_t = 0.007722 + 0.04444 \varepsilon_t^2 + 0.9556 h_{t-1} \]

2e) serial correlation in the fitted model

under the Ljung Box test, we cannot reject the Null Hypothesis at the 5% level - that is there is no serial correlation in the standardized residuals

zstd = as.numeric(sigma(mm))

sres_z = zret/zstd

Box.test(sres_z,lag = 10, type = "Ljung")

    Box-Ljung test

data:  sres_z
X-squared = 11.714, df = 10, p-value = 0.3046

Question 3

getSymbols('^GSPC', from = '2018-01-02', to = '2024-11-01')
[1] "GSPC"
lret_wmt = log(WMT$WMT.Close/lag(WMT$WMT.Close))*100

lret_spx =log(GSPC$GSPC.Close/lag(GSPC$GSPC.Close))*100


lret_comb = merge(lret_spx,lret_wmt)
lret_comb = na.omit(lret_comb)

lret_wmt = as.numeric(lret_comb$WMT.Close)
lret_spx = as.numeric(lret_comb$GSPC.Close)

3a) test CAPM model

m_capm = lm(lret_wmt~lret_spx)
summary(m_capm)

Call:
lm(formula = lret_wmt ~ lret_spx)

Residuals:
     Min       1Q   Median       3Q      Max 
-13.0862  -0.5708  -0.0232   0.5513   8.5045 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  0.03180    0.02983   1.066    0.287    
lret_spx     0.48974    0.02376  20.613   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.236 on 1717 degrees of freedom
Multiple R-squared:  0.1984,    Adjusted R-squared:  0.1979 
F-statistic: 424.9 on 1 and 1717 DF,  p-value: < 2.2e-16

fitted model \[ X_t = 0.03180 + 0.4897R_{m,t}+\varepsilon_t \]

3b) confirm significance of CAPM, create dummy variables

we let the null hypothesis be that the sensitivity to market returns \(\beta\) (how much percentage point movement of the market returns affect percentage point movement of the stock return), is 0. whilst the alternative hypothesis is that it is not 0

as the p value for the \(\beta\) from the t-test is 2e-16. it means that we can reject the Null Hypothesis at the 5% level- that is to say there is statistical evidence, that the return of the stock is sensitive to the market returns

# create dummy variable c1
c1 = rep(0,length(lret_spx))
idx=c(1:length(lret_spx))[lret_spx>0]
c1[idx] = 1

# create dummy variable nsp 
lret_nsp = c1*lret_spx

3c) design Threshold model - abnormal returns

we let the null hypothesis be that the alternative abnormal return in a positive market regime \(\tilde\alpha\) is 0. whilst the alternative hypothesis for is that it is not 0

as the p value for the \(\tilde{\alpha}\) from the t-test is 0.0987. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative abnormal return in stock returns in a positive market regime


m_tcapm1 = lm(lret_wmt~c1+lret_spx)
summary(m_tcapm1)

Call:
lm(formula = lret_wmt ~ c1 + lret_spx)

Residuals:
     Min       1Q   Median       3Q      Max 
-13.0930  -0.5732  -0.0111   0.5641   8.5389 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  0.10143    0.05163   1.964   0.0496 *  
c1          -0.13105    0.07933  -1.652   0.0987 .  
lret_spx     0.52390    0.03149  16.638   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.236 on 1716 degrees of freedom
Multiple R-squared:  0.1997,    Adjusted R-squared:  0.1987 
F-statistic:   214 on 2 and 1716 DF,  p-value: < 2.2e-16

fitted model at 5% level of significance, \(I\{\cdot\}\) is the indicator variable

\[ X_t = 0.1014 -0.1311 I\{R_{m,t} > 0\} + 0.5239 R_{m,t} + \varepsilon_t \]

3d) design Threshold model - marginal effects

we let the null hypothesis be that the alternative - sensitivity to market returns in a positive market regime \(\tilde{\beta}\) (how much percentage point movement of the market returns affect percentage point movement of the stock return, given market return is positive), whilst the alternative hypothesis is that it is not 0

as the p value for the \(\tilde{\beta}\) from the t-test is 0.612. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative sensitivity of stock returns to market returns during a positive market regime


m_tcapm1 = lm(lret_wmt~lret_nsp+lret_spx)
summary(m_tcapm1)

Call:
lm(formula = lret_wmt ~ lret_nsp + lret_spx)

Residuals:
     Min       1Q   Median       3Q      Max 
-13.1081  -0.5760  -0.0210   0.5527   8.5039 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  0.01844    0.03979   0.463    0.643    
lret_nsp     0.03221    0.06351   0.507    0.612    
lret_spx     0.47517    0.03728  12.747   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.236 on 1716 degrees of freedom
Multiple R-squared:  0.1985,    Adjusted R-squared:  0.1976 
F-statistic: 212.5 on 2 and 1716 DF,  p-value: < 2.2e-16

fitted model \[ X_t = 0.4752 R_{m,t} + 0.03221 R_{m,t} I \{R_{m,t} > 0\}+ \varepsilon_t \]

3e) combined thresholding model

we let the null hypothesis be that the alternative abnormal return in a positive market regime \(\tilde\alpha\) is 0. whilst the alternative hypothesis for is that it is not 0.

similarly we let the null hypothesis be that the alternative - sensitivity to market returns in a positive market regime \(\tilde{\beta}\) (how much percentage point movement of the market returns affect percentage point movement of the stock return, given market return is positive), whilst the alternative hypothesis is that it is not 0

as the p value for the \(\tilde{\alpha}\) from the t-test is 0.0906. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative abnormal return in stock returns in a positive market regime

as the p value for the \(\tilde{\beta}\) from the t-test is 0.5289. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative sensitivity of stock returns to market returns during a positive market regime


m_tcapm1 = lm(lret_wmt~c1+lret_nsp+lret_spx)
summary(m_tcapm1)

Call:
lm(formula = lret_wmt ~ c1 + lret_nsp + lret_spx)

Residuals:
     Min       1Q   Median       3Q      Max 
-13.1205  -0.5729  -0.0119   0.5641   8.5392 

Coefficients:
            Estimate Std. Error t value Pr(>|t|)    
(Intercept)  0.08676    0.05665   1.531   0.1259    
c1          -0.13471    0.07955  -1.693   0.0906 .  
lret_nsp     0.04009    0.06365   0.630   0.5289    
lret_spx     0.50673    0.04166  12.164   <2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 1.236 on 1715 degrees of freedom
Multiple R-squared:  0.1998,    Adjusted R-squared:  0.1984 
F-statistic: 142.8 on 3 and 1715 DF,  p-value: < 2.2e-16

fitted model \[ X_t = 0.08676 -0.1347 I\{R_{m,t}>0\} + 0.5067 R_{m,t} + 0.04009 R_{m,t} I\{R_{m,t}>0\}+ \varepsilon_t \]

Question 4

4a) describe the markov chain regime switching model

the markov chain regime switching model (MCSM), supposes that there is a set of unobservable states in the system, in which the behaviors of the time series is different under. these states jump to other states in the markov chain, as describe by the markov transition probability

4b) appealing features of MCSM

there is no need to assume or specific prior states like we have to in threshold models, the states can also be unobservant unlike threshold models

4c) fit a two state regime switching model



#Model with only intercept
mod<-lm(lret_wmt~lret_nsp + lret_spx)

#fit an constant model
msm_model = msmFit(mod, k=2, sw=c(T,T,T,T))
summary(msm_model)
Markov Switching Model

Call: msmFit(object = mod, k = 2, sw = c(T, T, T, T))

Coefficients:

Regime 1 
---------
               Estimate Std. Error t value Pr(>|t|)   
(Intercept)(S)  -0.0404     0.2919 -0.1384 0.889924   
lret_nsp(S)      0.2564     0.2415  1.0617 0.288372   
lret_spx(S)      0.4423     0.1523  2.9041 0.003683 **
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 3.381196
Multiple R-squared: 0.1869

Standardized Residuals:
          Min            Q1           Med            Q3           Max 
-13.431221722  -0.052082713  -0.002405205   0.043898711   8.411864474 

Regime 2 
---------
               Estimate Std. Error t value  Pr(>|t|)    
(Intercept)(S)   0.0915     0.0334  2.7395  0.006153 ** 
lret_nsp(S)     -0.1876     0.0688 -2.7267  0.006397 ** 
lret_spx(S)      0.5346     0.0412 12.9757 < 2.2e-16 ***
---
Signif. codes:  0 ‘***’ 0.001 ‘**’ 0.01 ‘*’ 0.05 ‘.’ 0.1 ‘ ’ 1

Residual standard error: 0.8499172
Multiple R-squared: 0.2297

Standardized Residuals:
          Min            Q1           Med            Q3           Max 
-2.225361e+00 -5.124874e-01 -8.764533e-05  4.986231e-01  2.312729e+00 

Transition probabilities:
          Regime 1   Regime 2
Regime 1 0.6915957 0.02446478
Regime 2 0.3084043 0.97553522

fitted model at 5%

\[ S_1 : X_t = -0.0404 +0.4423 R_{m,t} +0.2564 R_{m,t} I\{R_{m,t}> 0\} + \varepsilon_{t,1}\\ S_2 : X_t = 0.0915 + 0.5346 R_{m,t} -0.1867 R_{m,t} I\{R_{m,t}> 0\} + \varepsilon_{t,2}\\ \]

4d) interpret coefficients

\(\alpha_1 \ \& \ \alpha_2\) represent the abnormal returns in the different states, \(\beta_1 \ \& \ \beta_2\) represents stock return’s normal sensitivity to the market returns. If \(\gamma_i \neq 0\) then \(\beta_i\) can be interpreted as the sensitivity during a negative market regime. \(\sigma_1^2 \ \& \ \sigma_2^2\) represents the level of innovation or return shocks in the two different periods. Sometimes it is also possible to interpret the states for example in state 1 the constant term \(\mu\) is negative which suggests a market downturn state.

4e) observe any significant asymmetric pattern in marginal effects

Yes, this is observed in state 2, where there is a different \(\beta\) for positive and negative market returns

4f) write down & interpret the probability transition matrix

the columns of the matrix indicate the current state, whilst the rows indicate the next state. hence position [1,1] indicate the probability of the to remain in the current state, given we are currently in state one.

similarly [1,2] is the probability to be in state 1 in the next time step given that we are currently in state 1. by definition column sum of the matrix = 1

tmat = msm_model@transMat
tmat
          [,1]       [,2]
[1,] 0.6915957 0.02446478
[2,] 0.3084043 0.97553522

4g) expected duration in each regime

Expected duration of state 1 is 40.88 periods (trading days), expected duration of state 2 is 3.242 periods (trading days)

duration = 1/(1-diag(tmat))
duration
[1]  3.242497 40.875078
---
title: "R Notebook"
output: html_notebook
---

# Problem Set 3

**LAM Chun Ming (58555905)**

please find the full version here <https://rpubs.com/TCML/1254698>

```{r}
library('TSA')
library('fGarch')
library('parallel')
library('rugarch')
library('quantmod')
library('tseries')
library('forecast')
library('MSwM')
```

### Question 1

#### 1a) download VIX data

```{r}
getSymbols("VIX", from = '2006-01-01', to = '2024-10-22')
vix = as.numeric(VIX[,6])
vix = na.omit(vix)

dvix = diff(vix)
```

#### 1b.1) Write down an equivalent AR representation

ARCH(p) model is given as follows $$
h_t=\alpha_0 + \sum_{i=1}^{p}\alpha_i\varepsilon_{t-i}^2 \\
\varepsilon_t =z_t \sqrt{h_t} , \space \space z_t \sim i.i.d(0,1)
$$ we can use the fact that we can always decompose $\varepsilon_t^2 = h_t + v_t$ where $v_t$ is some arbitrary error, and show that this is the same as AR(p) on the squared error (or the de-meaned process) $\varepsilon_t^2$

$$
\varepsilon_t^2 = \alpha_0 + \sum_{i=1}^p\alpha_i\varepsilon_{t-i}^2 +v_t
$$

#### 1b.2) Explain and show the best order q can be determined

because, this the equivalent to the AR(p) process on the squared error term, we can run PACF on the squared error, as we would determined a AR process, following which we use an MLE method to fit the actual parameters

here we first find the de-meaned process by first fitting an ARIMA model

```{r}
# uses EACF on the differenced VIX (to remove stationary)
eacf(dvix)
m_arima = arima(vix, order = c(3,1,2))

# checking model goodness of fit - cannot reject the Null Hypothesis at 5% level - i.e. there is no serial dependency in the lag 
Box.test(m_arima$residuals,lag = 10)

# taking residuals 
res= m_arima$residuals

```

after fitting the ARIMA process, we fit an ARCH model, by considering it's AR equivalence

```{r}
pacf(res^2)
# PACF suggests AR of 3 <=> ARCH(3), 

# fitting model
model_ARCH3 = garchFit(~garch(3,0), data = res , trace = F)

# here all values are significant
summary(model_ARCH3)
```

#### 1b.3) write down the fitted ARCH & AR model

fitted at the

$$
ARCH: h_t = 91270 + 0.06927 \varepsilon_{t-1}^2 + 0.1504\varepsilon_{t-2}^2 + 0.2492\varepsilon_{t-3}^2\\
AR: \varepsilon_t^2 = 91270 + 0.06927 \varepsilon_{t-1}^2 + 0.1504\varepsilon_{t-2}^2 + 0.2492\varepsilon_{t-3}^2 + v_t \\
$$

#### 1c.1) Write down an ARMA equivalent for GARCH(m,s) GARCH model is given as follows

$$
\varepsilon_t = z_t \sqrt{h_t} \ \ s.t.: z_t \sim i.i.d(0,1)\\
h_t = \alpha_0 + \sum_{i=1}^m \alpha_i\varepsilon_{t-i}^2 + \sum_{j=1}^s \beta_j h_{t-j}
$$

again decomposing $\varepsilon_t^2 = h_t + v_t$,

$$
\varepsilon_t^2  = \alpha_0 + \sum_{i=1}^m \alpha_i \varepsilon_{t-i}^2 + \sum_{j=1}^s  \beta_j (\varepsilon_{t-j}^2-v_{t-j}) + v_t
$$

by regrouping into $\varepsilon_{t-j}^2 \ \& \ v_{t-j}$ , note that $I\{\cdot\}$ is the indicator function

$$
\varepsilon_t^2  = \alpha_0 + \sum_{i=1}^m \tilde\alpha_i \varepsilon_{t-i}^2 + \sum_{j=1}^s  \tilde\beta_j v_{t-j} + v_t\\
s.t. : \  \tilde\alpha_i = \alpha_iI\{i\leq m\} + \beta_i I\{i\leq s\}\\
\tilde \beta_j = -\beta_j 
$$

#### 1c.2) fit and write down the model

```{r}
model =  garchFit(~garch(1,1), data = res, trace = F)

summary(model)

```

fitted model

$$
h_t = 12860 + 0.06878 \varepsilon_{t-1}^2 + 0.8291 h_{t-1}
$$

#### 1d) fit model assuming a student - t distribution

```{r}
model =  garchFit(~garch(1,1), data = res, cond.dist = 'std', trace = F)

summary(model)
```

the fitted model $$
h_t = 28.30 + 0.6327\varepsilon_{t-1}^2 +  0.7263 h_{t-1}
$$

#### 1e.1) explain how to choose ARMA orders

following work done in part **1a)**

```{r}
# test for stationarity in vix data ; we cannot reject the Null Hypothesis data is non stationary
adf.test(vix)

# differencing to remove stationarity, test again; we can reject the Null Hypothesis - i.e. the data is stationary
adf.test(dvix)

# use EACF to select for model - this produces candidate model ARMA(0,1) & ARMA(2,1) 
eacf(dvix)

# try to fit for ARMA(0,1)
m1 = arima(vix, order = c(0,1,1))

# test for validity - can reject the null hypothesis at 5% - there is serial dependencies in the residual
Box.test(m1$residuals,lag = 10)

# try second candidate 
m2 = arima(vix, order = c(2,1,1))

# test for validity - can reject the null hypothesis at 5% - there is serial dependencies in the residual  
Box.test(m2$residuals,lag = 10)

# try third candidate 

m3 = arima(vix, order = c(3,1,2))

# test for validity - cannot reject the null hypothesis at 5% - there is no serial dependencies in the residual
Box.test(m3$residuals,lag = 10)


# accept the ARMA(3,2) on the differenced data 
```

#### 1e.2) write down the fitted model

first fit the model using an MLE method

```{r}

model =  garchFit(~arma(3,2)+garch(1,1), data = dvix,  trace = F)

summary(model)
```

fitted model

$$
X_t = 0.9605 X_{t-1} -0.4149 X_{t-2} + 0.07945 X_{t-3} - \varepsilon_{t-1} + 0.3465 \varepsilon_{t-2}+\varepsilon_t\\
h_t = 15570 + 0.09434 \varepsilon_{t-1}^2 + 0.7862 h_{t-1} 
$$

### Question 2

#### 2a) expected value of returns the Null hypothesis states that the mean of the daily log percentage returns is 0, whilst the alternative is that it is not 0.

here the p value is 0.1105, the sample statistic has a 11.05% probability to be observed given an assumed Null Hypothesis. therefore we cannot reject the Null Hypothesis at the 5% level. That is to say, given our sample, we do not see sufficient statistical evidence that the population daily log percentage return is different from 0.

```{r}
getSymbols("WMT",from = "2018-01-02", to = "2024-11-01")

# find the log percentage returns 
wmt = WMT$WMT.Close
lret_wmt = log(wmt/lag(wmt))*100

# format data
lret_wmt = na.omit(lret_wmt)
lret_wmt = as.numeric(lret_wmt)

# find the mean
mean(lret_wmt)

# conduct t test
t.test(lret_wmt)
```

#### 2b) are there serial correlation in the return and squared return

Taking the Ljung Box test shows that, we can reject the Null Hypothesis for both the log returns and the log squared returns. that is, there is serial dependencies in both time series

```{r}

Box.test(lret_wmt, lag = 10, type = "Ljung")
Box.test(lret_wmt^2, lag = 10, type = "Ljung")

```

#### 2c) fit an ARCH - GARCH model to the rt series

the model seems adequate - the QQ plot shows reasonable good fit for most of the central quantile data points, Ljung Box test on the residuals also shows no serial dependencies in the residual

```{r}

# use EACF
eacf(lret_wmt)

# candidate ARMA(1,0) - LB test sufficient: we can reject the null hypothesis at 5% - i.e. there is serial dependencies in the residual
m1 = arima(lret_wmt, c(1,0,0))
Box.test(m1$residuals, lag = 10 , type = "Ljung")

# candidate ARMA(3,1) - LB test sufficient: we can reject the null hypothesis at 5% - i.e. there is serial dependencies in the residual 
m2 = arima(lret_wmt, c(3,0,1))
Box.test(m2$residuals, lag = 10 , type = "Ljung")

# candidate ARMA(5,2)
m3 = arima(lret_wmt, c(5,0,2))
Box.test(m3$residuals, lag = 10 , type = "Ljung")


#fit ARMA - GARCH model 
model_C1 = garchFit(~arma(5,2)+garch(1,1),lret_wmt,trace = F)
summary(model_C1)

plot(model_C1,which = 13)

```

fitted model

$$
X_t = 0.1290 - 0.3900 X_{t-1} -0.7519 X_{t-2} -0.04658 X_{t-3} -0.06840 X_{t-4} +0.006966 X_{t-5} + 0.3222\varepsilon_{t-1} + 0.6915 \varepsilon_{t-2}\\
h_t = 0.2000 + 0.1174 \varepsilon_{t-1}^2 +0.7798 h_{t-1}
$$

#### 2d) IGARCH Model

fitting the IGARCH(1,1) model to the time series $z_t$

```{r}

zret = lret_wmt - mean(lret_wmt)

spec1=ugarchspec(variance.model=list(model="iGARCH",garchOrder=c(1,1)),mean.model=list(armaOrder=c(0,0)))
mm=ugarchfit(zret,spec=spec1)
mm

```

the fitted model $$
h_t = 0.007722 + 0.04444 \varepsilon_t^2 + 0.9556 h_{t-1}
$$

#### 2e) serial correlation in the fitted model

under the Ljung Box test, we cannot reject the Null Hypothesis at the 5% level - that is there is no serial correlation in the standardized residuals

```{r}
zstd = as.numeric(sigma(mm))

sres_z = zret/zstd

Box.test(sres_z,lag = 10, type = "Ljung")
```

### Question 3

```{r}
getSymbols('^GSPC', from = '2018-01-02', to = '2024-11-01')

lret_wmt = log(WMT$WMT.Close/lag(WMT$WMT.Close))*100

lret_spx =log(GSPC$GSPC.Close/lag(GSPC$GSPC.Close))*100


lret_comb = merge(lret_spx,lret_wmt)
lret_comb = na.omit(lret_comb)

lret_wmt = as.numeric(lret_comb$WMT.Close)
lret_spx = as.numeric(lret_comb$GSPC.Close)
```

#### 3a) test CAPM model

```{r}
m_capm = lm(lret_wmt~lret_spx)
summary(m_capm)
```

fitted model $$
X_t = 0.03180 + 0.4897R_{m,t}+\varepsilon_t
$$

#### 3b) confirm significance of CAPM, create dummy variables

we let the null hypothesis be that the sensitivity to market returns $\beta$ (how much percentage point movement of the market returns affect percentage point movement of the stock return), is 0. whilst the alternative hypothesis is that it is not 0

as the p value for the $\beta$ from the t-test is 2e-16. it means that we can reject the Null Hypothesis at the 5% level- that is to say there is statistical evidence, that the return of the stock is sensitive to the market returns

```{r}
# create dummy variable c1
c1 = rep(0,length(lret_spx))
idx=c(1:length(lret_spx))[lret_spx>0]
c1[idx] = 1

# create dummy variable nsp 
lret_nsp = c1*lret_spx
```

#### 3c) design Threshold model - abnormal returns

we let the null hypothesis be that the alternative abnormal return in a positive market regime $\tilde\alpha$ is 0. whilst the alternative hypothesis for is that it is not 0

as the p value for the $\tilde{\alpha}$ from the t-test is 0.0987. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative abnormal return in stock returns in a positive market regime

```{r}

m_tcapm1 = lm(lret_wmt~c1+lret_spx)
summary(m_tcapm1)
```

fitted model at 5% level of significance, $I\{\cdot\}$ is the indicator variable

$$
X_t = 0.1014 -0.1311 I\{R_{m,t} > 0\} + 0.5239 R_{m,t} + \varepsilon_t
$$

#### 3d) design Threshold model - marginal effects

we let the null hypothesis be that the alternative - sensitivity to market returns in a positive market regime $\tilde{\beta}$ (how much percentage point movement of the market returns affect percentage point movement of the stock return, given market return is positive), whilst the alternative hypothesis is that it is not 0

as the p value for the $\tilde{\beta}$ from the t-test is 0.612. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative sensitivity of stock returns to market returns during a positive market regime

```{r}

m_tcapm1 = lm(lret_wmt~lret_nsp+lret_spx)
summary(m_tcapm1)
```

fitted model $$
X_t = 0.4752 R_{m,t} + 0.03221 R_{m,t} I \{R_{m,t} > 0\}+ \varepsilon_t 
$$

#### 3e) combined thresholding model

we let the null hypothesis be that the alternative abnormal return in a positive market regime $\tilde\alpha$ is 0. whilst the alternative hypothesis for is that it is not 0.

similarly we let the null hypothesis be that the alternative - sensitivity to market returns in a positive market regime $\tilde{\beta}$ (how much percentage point movement of the market returns affect percentage point movement of the stock return, given market return is positive), whilst the alternative hypothesis is that it is not 0

as the p value for the $\tilde{\alpha}$ from the t-test is 0.0906. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative abnormal return in stock returns in a positive market regime

as the p value for the $\tilde{\beta}$ from the t-test is 0.5289. it means that we cannot reject the Null Hypothesis at the 5% level- that is to say there is not sufficient statistical evidence, that there exists an alternative sensitivity of stock returns to market returns during a positive market regime

```{r}

m_tcapm1 = lm(lret_wmt~c1+lret_nsp+lret_spx)
summary(m_tcapm1)
```

fitted model $$
X_t = 0.08676 -0.1347 I\{R_{m,t}>0\} + 0.5067 R_{m,t} + 0.04009 R_{m,t} I\{R_{m,t}>0\}+ \varepsilon_t 
$$

### Question 4

#### 4a) describe the markov chain regime switching model

the markov chain regime switching model (MCSM), supposes that there is a set of unobservable states in the system, in which the behaviors of the time series is different under. these states jump to other states in the markov chain, as describe by the markov transition probability

#### 4b) appealing features of MCSM

there is no need to assume or specific prior states like we have to in threshold models, the states can also be unobservant unlike threshold models

#### 4c) fit a two state regime switching model

```{r}


#Model with only intercept
mod<-lm(lret_wmt~lret_nsp + lret_spx)

#fit an constant model
msm_model = msmFit(mod, k=2, sw=c(T,T,T,T))
summary(msm_model)

```

fitted model at 5%

$$
S_1 : X_t = -0.0404 +0.4423 R_{m,t} +0.2564 R_{m,t} I\{R_{m,t}> 0\} + \varepsilon_{t,1}\\
S_2 : X_t = 0.0915 + 0.5346 R_{m,t} -0.1867 R_{m,t} I\{R_{m,t}> 0\} + \varepsilon_{t,2}\\
$$

#### 4d) interpret coefficients

$\alpha_1 \ \& \ \alpha_2$ represent the abnormal returns in the different states, $\beta_1 \ \& \ \beta_2$ represents stock return's normal sensitivity to the market returns. If $\gamma_i \neq 0$ then $\beta_i$ can be interpreted as the sensitivity during a negative market regime. $\sigma_1^2 \ \& \ \sigma_2^2$ represents the level of innovation or return shocks in the two different periods. Sometimes it is also possible to interpret the states for example in state 1 the constant term $\mu$ is negative which suggests a market downturn state.

#### 4e) observe any significant asymmetric pattern in marginal effects

Yes, this is observed in state 2, where there is a different $\beta$ for positive and negative market returns

#### 4f) write down & interpret the probability transition matrix

the columns of the matrix indicate the current state, whilst the rows indicate the next state. hence position [1,1] indicate the probability of the to remain in the current state, given we are currently in state one.

similarly [1,2] is the probability to be in state 1 in the next time step given that we are currently in state 1. by definition column sum of the matrix = 1

```{r}
tmat = msm_model@transMat
tmat

```

#### 4g) expected duration in each regime

Expected duration of state 1 is 40.88 periods (trading days), expected duration of state 2 is 3.242 periods (trading days)

```{r}
duration = 1/(1-diag(tmat))
duration
```
