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Course Calendar
Class DATE Contents
1 Sep. 26 Course information & Course overview
2 Oct. 4 Bayes Estimation
3 〃 11 Classical Bayes Estimation - Kalman Filter -
4 〃 18 Simulation-based Bayesian Methods
5 〃 25 Modern Bayesian Estimation :Particle Filter
6 Nov. 1 HMM(Hidden Markov Model)
Nov. 8 No Class
7 〃 15 Supervised Learning
8 〃 29 Bayesian Decision
9 Dec. 6 PCA(Principal Component Analysis)
10 〃 13 ICA(Independent Component Analysis)
11 〃 20 Applications of PCA and ICA
12 〃 27 Clustering, k-means et al.
13 Jan. 17 Other Topics 1 Kernel machine.
14 〃 22(Tue) Other Topics 2
Lecture Plan
Simulation-based Bayesian Estimation
- Prelude to the particle filter -
1. Why simulation-based ?
2. Monte Carlo Sampling Methods
Historical example
Monte Carlo Approximation
3. Sampling Theory
Sample Generation Method
Importance Sampling
1. Why simulation-based ?
Go Nonlinear and Non-Gaussian
Kalman Filter
Linear
Gaussian density
Analytic form
Particle Filter
Nonlinear
Non-Gaussian
density
Simulation-based
(Monte Carlo
approaches)
Extended
Kalman Filter
Linearization
of nonlinear
system
(Unscented
Kalman filter)
2. Monte Carlo Methods
3.1 Historical example
- Buffon’s Needle - A needle of length l is dropped at random on
a flat surface ruled with parallel lines a distance d>l apart, what is
the probability that the needle will cross one of the lines.
d
l
 
 
2
Probability =
2
Dropped times, is the number of times
the needle crosses a line.
E Ml
d n
n l
E M d
n M




The experiment by Captain Fox (1864) estimates =3.1416
The Monte Carlo (MC) methods is a collection of techniques
performing estimation through random sampling.
 
     
Let perform a numerical integration:
: N-dimensional vector
Factorize where ( ) is interpreted as a proability density
satisfyin
I g x dx x
g x f x p x p x



   
      
 
   
 
   ( )
1
g 0 and 1.
For the new expression
,
(1) Draw N samples : 1, , independently from the density .
(2) Approximate by an empirical density distribution
1
ˆ
(3)
i
N
i
i
p x p x dx
I E f x f x p x dx
x i N p x
p x
p x x x
N


 
 

 



        
 ( )
1 1
1 1ˆ ˆ
N N
ii
i i
I E f x f x x x dx f x
N N

 
    
2.2 Monte Carlo Approximation (Integration)
This approximation is referred to as Monte Carlo integration
Remarks:
1) Numerical integration techniques are not efficient due to;
/ the number of points to be evaluated increases with the
dimensionality of parameter space,
/very small proportion of the samples will make a significant
contribution to the integral
2) Key idea of MC is to represent the target distribution as a set of
random samples.
MC method provides appropriate results in some statistical sense
(Convergence, non-biased etc. ) as far as we generate proper samples.
From the low of large numbers approves the convergence of MC
integration.
3. Sampling Theory
 
 
    
1
1
:Given an input random vector ,the PDF transformed by
z which is monotonic, one-to-one, invertible ( ) is given by
where :Jacobian of the transformation .
(whe
Z
Z X
x p z
T x T
x
p z p x T z
z
x
T
z




 



Corollary
n and are scalars, opearation means the absolute value)x z 
Monte Carlo simulation starts by generating random samples from a
known distribution.
3.1 Sample generation method:
From a given probability density function (PDF) to a target density
 : X
x
PDF p x  
z
: ZPDF p z
T(x)
In practice, it is difficult to generate the samples directly from the
density . Instead, the samples can be generated by , referred
to as importance distribution or proposal distribution, whose PDF is
similar as .
 i
x
 p x  q x
 
   
 
     
 
 
 
Similarity of means:
0 0
In terms of , we have
where : is referred to as the .
q x
p x q x for all x
q x
I f x x q x dx
p x
x importance weght
q x


  



3.2 Importance sampling
 p x
         
The importance sampling approximation of can be written by
N
( i ) ( i )
i
I
ˆ ˆI I f x x q x dx x f x
N
 

    1
1
 
 
 
 
 
     
 
 
 
   ( ) ( )
1
can be evaluated up to a normalization constant, i.e.
( is unknown), q ( is unknown)
Then,
=
1
,
p q
p q
q
p
N
q i i
p i
p x
p x q x
p x Z x Z
Z Z
Z p x
I f x p x dx f x q x dx
Z q x
Z
w x f x
Z N 
 


 

Case :
 
 
 
( )
( )
( )
i
i
i
p x
w x
q x

 
   
 
( )
( )
1
( )
1
Consider the case ( ), the ratio can be evaluated by using the sample
set as follows.
1
1
1
Thus,
1
i
N
q i
p i
q
N
p i
i
f x
x
Z
p x dx w x
Z N
Z
Z
w x
N


 



 
     
 
 
 
( )
( ) ( ) ( )
1 1
( )
( )
( )
1
Therefore,
where :
iN N
i i i
pi i
q
i
i
N
j
j
w x
I f x w x f x
Z
Z
w x
w x
w x
 

 
 
  
 

 


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2012 mdsp pr04 monte carlo

  • 1. Course Calendar Class DATE Contents 1 Sep. 26 Course information & Course overview 2 Oct. 4 Bayes Estimation 3 〃 11 Classical Bayes Estimation - Kalman Filter - 4 〃 18 Simulation-based Bayesian Methods 5 〃 25 Modern Bayesian Estimation :Particle Filter 6 Nov. 1 HMM(Hidden Markov Model) Nov. 8 No Class 7 〃 15 Supervised Learning 8 〃 29 Bayesian Decision 9 Dec. 6 PCA(Principal Component Analysis) 10 〃 13 ICA(Independent Component Analysis) 11 〃 20 Applications of PCA and ICA 12 〃 27 Clustering, k-means et al. 13 Jan. 17 Other Topics 1 Kernel machine. 14 〃 22(Tue) Other Topics 2
  • 2. Lecture Plan Simulation-based Bayesian Estimation - Prelude to the particle filter - 1. Why simulation-based ? 2. Monte Carlo Sampling Methods Historical example Monte Carlo Approximation 3. Sampling Theory Sample Generation Method Importance Sampling
  • 3. 1. Why simulation-based ? Go Nonlinear and Non-Gaussian Kalman Filter Linear Gaussian density Analytic form Particle Filter Nonlinear Non-Gaussian density Simulation-based (Monte Carlo approaches) Extended Kalman Filter Linearization of nonlinear system (Unscented Kalman filter)
  • 4. 2. Monte Carlo Methods 3.1 Historical example - Buffon’s Needle - A needle of length l is dropped at random on a flat surface ruled with parallel lines a distance d>l apart, what is the probability that the needle will cross one of the lines. d l     2 Probability = 2 Dropped times, is the number of times the needle crosses a line. E Ml d n n l E M d n M     The experiment by Captain Fox (1864) estimates =3.1416 The Monte Carlo (MC) methods is a collection of techniques performing estimation through random sampling.
  • 5.         Let perform a numerical integration: : N-dimensional vector Factorize where ( ) is interpreted as a proability density satisfyin I g x dx x g x f x p x p x                          ( ) 1 g 0 and 1. For the new expression , (1) Draw N samples : 1, , independently from the density . (2) Approximate by an empirical density distribution 1 ˆ (3) i N i i p x p x dx I E f x f x p x dx x i N p x p x p x x x N                       ( ) 1 1 1 1ˆ ˆ N N ii i i I E f x f x x x dx f x N N         2.2 Monte Carlo Approximation (Integration) This approximation is referred to as Monte Carlo integration
  • 6. Remarks: 1) Numerical integration techniques are not efficient due to; / the number of points to be evaluated increases with the dimensionality of parameter space, /very small proportion of the samples will make a significant contribution to the integral 2) Key idea of MC is to represent the target distribution as a set of random samples. MC method provides appropriate results in some statistical sense (Convergence, non-biased etc. ) as far as we generate proper samples. From the low of large numbers approves the convergence of MC integration.
  • 7. 3. Sampling Theory          1 1 :Given an input random vector ,the PDF transformed by z which is monotonic, one-to-one, invertible ( ) is given by where :Jacobian of the transformation . (whe Z Z X x p z T x T x p z p x T z z x T z          Corollary n and are scalars, opearation means the absolute value)x z  Monte Carlo simulation starts by generating random samples from a known distribution. 3.1 Sample generation method: From a given probability density function (PDF) to a target density  : X x PDF p x   z : ZPDF p z T(x)
  • 8. In practice, it is difficult to generate the samples directly from the density . Instead, the samples can be generated by , referred to as importance distribution or proposal distribution, whose PDF is similar as .  i x  p x  q x                     Similarity of means: 0 0 In terms of , we have where : is referred to as the . q x p x q x for all x q x I f x x q x dx p x x importance weght q x         3.2 Importance sampling  p x
  • 9.           The importance sampling approximation of can be written by N ( i ) ( i ) i I ˆ ˆI I f x x q x dx x f x N        1 1                          ( ) ( ) 1 can be evaluated up to a normalization constant, i.e. ( is unknown), q ( is unknown) Then, = 1 , p q p q q p N q i i p i p x p x q x p x Z x Z Z Z Z p x I f x p x dx f x q x dx Z q x Z w x f x Z N         Case :       ( ) ( ) ( ) i i i p x w x q x 
  • 10.         ( ) ( ) 1 ( ) 1 Consider the case ( ), the ratio can be evaluated by using the sample set as follows. 1 1 1 Thus, 1 i N q i p i q N p i i f x x Z p x dx w x Z N Z Z w x N                      ( ) ( ) ( ) ( ) 1 1 ( ) ( ) ( ) 1 Therefore, where : iN N i i i pi i q i i N j j w x I f x w x f x Z Z w x w x w x                