g05xdc computes scaled increments of sample paths of a free or non-free Wiener process, where the sample paths are constructed by a Brownian bridge algorithm. The initialization function g05xcc must be called prior to the first call to g05xdc.
The function may be called by the names: g05xdc or nag_rand_bb_inc.
3Description
For details on the Brownian bridge algorithm and the bridge construction order see Section 2.6 in the G05 Chapter Introduction and Section 3 in g05xcc. Recall that the terms Wiener process (or free Wiener process) and Brownian motion are often used interchangeably, while a non-free Wiener process (also known as a Brownian bridge process) refers to a process which is forced to terminate at a given point.
Fix two times , let be any set of time points satisfying , and let , , denote a -dimensional Wiener sample path at these time points.
The Brownian bridge increments generator uses the Brownian bridge algorithm to construct sample paths for the (free or non-free) Wiener process , and then uses this to compute the scaled Wiener increments
4References
Glasserman P (2004) Monte Carlo Methods in Financial Engineering Springer
5Arguments
Note: the following variable is used in the parameter descriptions:
, the length of the array times passed to the initialization function g05xcc.
1: – Nag_OrderTypeInput
On entry: the order argument specifies the two-dimensional storage scheme being used, i.e., row-major ordering or column-major ordering. C language defined storage is specified by . See Section 3.1.3 in the Introduction to the NAG Library CL Interface for a more detailed explanation of the use of this argument.
Constraint:
or .
2: – IntegerInput
On entry: the number of Wiener sample paths.
Constraint:
.
3: – IntegerInput
On entry: the dimension of each Wiener sample path.
Constraint:
.
4: – IntegerInput
On entry: if , a free Wiener process is created and diff is ignored.
If , a non-free Wiener process is created where diff is the difference between the terminal value and the starting value of the process.
Constraint:
or .
5: – const doubleInput
On entry: the difference between the terminal value and starting value of the Wiener process. If , diff is ignored.
6: – doubleInput/Output
Note: the dimension, dim, of the array z
must be at least
when
;
when
.
The th element of the matrix is stored in
when ;
when .
On entry: the Normal random numbers used to construct the sample paths.
If quasi-random numbers are used, the -dimensional quasi-random points should be stored in successive rows of .
On exit: the Normal random numbers premultiplied by c.
7: – IntegerInput
On entry: the stride separating row or column elements (depending on the value of order) in the array z.
Constraints:
if , ;
if , .
8: – const doubleInput
Note: the dimension, dim, of the array c
must be at least
.
The th element of the matrix is stored in .
On entry: the lower triangular Cholesky factorization such that gives the covariance matrix of the Wiener process. Elements of above the diagonal are not referenced.
9: – IntegerInput
On entry: the stride separating matrix row elements in the array c.
Constraint:
.
10: – doubleOutput
Note: the dimension, dim, of the array b
must be at least
when
;
when
.
The th element of the matrix is stored in
when ;
when .
On exit: the scaled Wiener increments.
Let denote the th dimension of the th point of the th sample path where , and . The increment is stored at .
11: – IntegerInput
On entry: the stride separating row or column elements (depending on the value of order) in the array b.
Constraints:
if , ;
if , .
12: – const doubleCommunication Array
Note: the dimension, , of this array is dictated by the requirements of associated functions that must have been previously called. This array MUST be the same array passed as argument rcomm in the previous call to g05xccorg05xdc.
On entry: communication array as returned by the last call to g05xccorg05xdc. This array MUST NOT be directly modified.
13: – NagError *Input/Output
The NAG error argument (see Section 7 in the Introduction to the NAG Library CL Interface).
6Error Indicators and Warnings
NE_ALLOC_FAIL
Dynamic memory allocation failed.
See Section 3.1.2 in the Introduction to the NAG Library CL Interface for further information.
NE_ARRAY_SIZE
On entry, and . Constraint: .
On entry, and . Constraint: .
On entry, . Constraint: .
On entry, and . Constraint: .
On entry, and . Constraint: .
NE_BAD_PARAM
On entry, argument had an illegal value.
NE_ILLEGAL_COMM
On entry, rcomm was not initialized or has been corrupted.
NE_INT
On entry, . Constraint: .
On entry, . Constraint: .
On entry, . Constraint: .
NE_INTERNAL_ERROR
An internal error has occurred in this function. Check the function call and any array sizes. If the call is correct then please contact NAG for assistance.
See Section 7.5 in the Introduction to the NAG Library CL Interface for further information.
NE_NO_LICENCE
Your licence key may have expired or may not have been installed correctly.
See Section 8 in the Introduction to the NAG Library CL Interface for further information.
7Accuracy
Not applicable.
8Parallelism and Performance
g05xdc is threaded by NAG for parallel execution in multithreaded implementations of the NAG Library.
g05xdc makes calls to BLAS and/or LAPACK routines, which may be threaded within the vendor library used by this implementation. Consult the documentation for the vendor library for further information.
Please consult the X06 Chapter Introduction for information on how to control and interrogate the OpenMP environment used within this function. Please also consult the Users' Note for your implementation for any additional implementation-specific information.
9Further Comments
None.
10Example
The scaled Wiener increments produced by this function can be used to compute numerical solutions to stochastic differential equations (SDEs) driven by (free or non-free) Wiener processes. Consider an SDE of the form
on the interval where is a (free or non-free) Wiener process and and are suitable functions. A numerical solution to this SDE can be obtained by the Euler–Maruyama method. For any discretization of , set
for so that is an approximation to . The scaled Wiener increments produced by g05xdc can be used in the
Euler–Maruyama scheme outlined above by writing
The following example program uses this method to solve the SDE for geometric Brownian motion
where is a Wiener process, and compares the results against the analytic solution
Quasi-random variates are used to construct the Wiener increments.