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Computational finance

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Computational finance is a branch of applied computer science that deals with problems of practical interest in finance . Some slightly different definitions are the study of data and algorithms currently used in finance and the mathematics of computer programs that realize financial models or systems .

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81-441: Computational finance emphasizes practical numerical methods rather than mathematical proofs and focuses on techniques that apply directly to economic analyses . It is an interdisciplinary field between mathematical finance and numerical methods . Two major areas are efficient and accurate computation of fair values of financial securities and the modeling of stochastic time series . The birth of computational finance as

162-471: A , b ∈ R {\displaystyle a,b\in \mathbb {R} } ) and x {\displaystyle x} denotes the Cartesian product , square brackets denote closed intervals , then there is an interval I = [ x 0 − h , x 0 + h ] ⊂ [ x 0 − a , x 0 +

243-445: A ] {\displaystyle I=[x_{0}-h,x_{0}+h]\subset [x_{0}-a,x_{0}+a]} for some h ∈ R {\displaystyle h\in \mathbb {R} } where the solution to the above equation and initial value problem can be found. That is, there is a solution and it is unique. Since there is no restriction on F {\displaystyle F} to be linear, this applies to non-linear equations that take

324-400: A discretization error because the solution of the discrete problem does not coincide with the solution of the continuous problem. In the example above to compute the solution of 3 x 3 + 4 = 28 {\displaystyle 3x^{3}+4=28} , after ten iterations, the calculated root is roughly 1.99. Therefore, the truncation error is roughly 0.01. Once an error

405-621: A finite difference method, or (particularly in engineering) a finite volume method . The theoretical justification of these methods often involves theorems from functional analysis . This reduces the problem to the solution of an algebraic equation. Since the late twentieth century, most algorithms are implemented in a variety of programming languages. The Netlib repository contains various collections of software routines for numerical problems, mostly in Fortran and C . Commercial products implementing many different numerical algorithms include

486-445: A ) = −24, f ( b ) = 57. From this table it can be concluded that the solution is between 1.875 and 2.0625. The algorithm might return any number in that range with an error less than 0.2. Ill-conditioned problem: Take the function f ( x ) = 1/( x  − 1) . Note that f (1.1) = 10 and f (1.001) = 1000: a change in x of less than 0.1 turns into a change in f ( x ) of nearly 1000. Evaluating f ( x ) near x = 1

567-489: A closed rectangle R = [ x 0 − a , x 0 + a ] × [ y 0 − b , y 0 + b ] {\displaystyle R=[x_{0}-a,x_{0}+a]\times [y_{0}-b,y_{0}+b]} in the x − y {\displaystyle x-y} plane, where a {\displaystyle a} and b {\displaystyle b} are real (symbolically:

648-710: A differential equation is a result that describes dynamically changing phenomena, evolution, and variation. Often, quantities are defined as the rate of change of other quantities (for example, derivatives of displacement with respect to time), or gradients of quantities, which is how they enter differential equations. Specific mathematical fields include geometry and analytical mechanics . Scientific fields include much of physics and astronomy (celestial mechanics), meteorology (weather modeling), chemistry (reaction rates), biology (infectious diseases, genetic variation), ecology and population modeling (population competition), economics (stock trends, interest rates and

729-508: A discipline can be traced to Harry Markowitz in the early 1950s. Markowitz conceived of the portfolio selection problem as an exercise in mean-variance optimization. This required more computer power than was available at the time, so he worked on useful algorithms for approximate solutions. Mathematical finance began with the same insight, but diverged by making simplifying assumptions to express relations in simple closed forms that did not require sophisticated computer science to evaluate. In

810-404: A finite sum of regions can be found, and hence the approximation of the exact solution. Similarly, to differentiate a function, the differential element approaches zero, but numerically only a nonzero value of the differential element can be chosen. An algorithm is called numerically stable if an error, whatever its cause, does not grow to be much larger during the calculation. This happens if

891-425: A novel approach, subsequently elaborated by Thomé and Frobenius . Collet was a prominent contributor beginning in 1869. His method for integrating a non-linear system was communicated to Bertrand in 1868. Clebsch (1873) attacked the theory along lines parallel to those in his theory of Abelian integrals . As the latter can be classified according to the properties of the fundamental curve that remains unchanged under

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972-473: A point which is outside the given points must be found. Regression is also similar, but it takes into account that the data are imprecise. Given some points, and a measurement of the value of some function at these points (with an error), the unknown function can be found. The least squares -method is one way to achieve this. Another fundamental problem is computing the solution of some given equation. Two cases are commonly distinguished, depending on whether

1053-426: A rational transformation, Clebsch proposed to classify the transcendent functions defined by differential equations according to the invariant properties of the corresponding surfaces f = 0 {\displaystyle f=0} under rational one-to-one transformations. From 1870, Sophus Lie 's work put the theory of differential equations on a better foundation. He showed that the integration theories of

1134-513: A unique maximum (possibly infinite) open interval such that any solution that satisfies this initial condition is a restriction of the solution that satisfies this initial condition with domain I max {\displaystyle I_{\max }} . In the case that x ± ≠ ± ∞ {\displaystyle x_{\pm }\neq \pm \infty } , there are exactly two possibilities where Ω {\displaystyle \Omega }

1215-452: A well-conditioned problem may be either numerically stable or numerically unstable. An art of numerical analysis is to find a stable algorithm for solving a well-posed mathematical problem. The field of numerical analysis includes many sub-disciplines. Some of the major ones are: Interpolation: Observing that the temperature varies from 20 degrees Celsius at 1:00 to 14 degrees at 3:00, a linear interpolation of this data would conclude that it

1296-541: Is a vector-valued function of y {\displaystyle \mathbf {y} } and its derivatives, then is an explicit system of ordinary differential equations of order n > {\displaystyle n>} and dimension m {\displaystyle m} . In column vector form: These are not necessarily linear. The implicit analogue is: where 0 = ( 0 , 0 , … , 0 ) {\displaystyle {\boldsymbol {0}}=(0,0,\ldots ,0)}

1377-399: Is a solution containing n {\displaystyle n} arbitrary independent constants of integration . A particular solution is derived from the general solution by setting the constants to particular values, often chosen to fulfill set ' initial conditions or boundary conditions '. A singular solution is a solution that cannot be obtained by assigning definite values to

1458-427: Is a term that includes both rocket scientists and financial engineers, as well as quantitative portfolio managers). This led to a second major extension of the range of computational methods used in finance, also a move away from personal computers to mainframes and supercomputers . Around this time computational finance became recognized as a distinct academic subfield. The first degree program in computational finance

1539-462: Is a theory of a special type of second-order linear ordinary differential equation. Their solutions are based on eigenvalues and corresponding eigenfunctions of linear operators defined via second-order homogeneous linear equations . The problems are identified as Sturm–Liouville problems (SLP) and are named after J. C. F. Sturm and J. Liouville , who studied them in the mid-1800s. SLPs have an infinite number of eigenvalues, and

1620-468: Is an equation of the form where a 0 ( x ) , … , a n ( x ) {\displaystyle a_{0}(x),\ldots ,a_{n}(x)} and b ( x ) {\displaystyle b(x)} are arbitrary differentiable functions that do not need to be linear, and y ′ , … , y ( n ) {\displaystyle y',\ldots ,y^{(n)}} are

1701-401: Is an ill-conditioned problem. Well-conditioned problem: By contrast, evaluating the same function f ( x ) = 1/( x  − 1) near x = 10 is a well-conditioned problem. For instance, f (10) = 1/9 ≈ 0.111 and f (11) = 0.1: a modest change in x leads to a modest change in f ( x ). Furthermore, continuous problems must sometimes be replaced by a discrete problem whose solution

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1782-623: Is an interval, is called a solution or integral curve for F {\displaystyle F} , if u {\displaystyle u} is n {\displaystyle n} -times differentiable on I {\displaystyle I} , and Given two solutions u : J ⊂ R → R {\displaystyle u:J\subset \mathbb {R} \to \mathbb {R} } and v : I ⊂ R → R {\displaystyle v:I\subset \mathbb {R} \to \mathbb {R} } , u {\displaystyle u}

1863-424: Is called principal component analysis . Optimization problems ask for the point at which a given function is maximized (or minimized). Often, the point also has to satisfy some constraints . The field of optimization is further split in several subfields, depending on the form of the objective function and the constraint. For instance, linear programming deals with the case that both the objective function and

1944-433: Is called an extension of v {\displaystyle v} if I ⊂ J {\displaystyle I\subset J} and A solution that has no extension is called a maximal solution . A solution defined on all of R {\displaystyle \mathbb {R} } is called a global solution . A general solution of an n {\displaystyle n} th-order equation

2025-524: Is called the Euler method for solving an ordinary differential equation. One of the simplest problems is the evaluation of a function at a given point. The most straightforward approach, of just plugging in the number in the formula is sometimes not very efficient. For polynomials, a better approach is using the Horner scheme , since it reduces the necessary number of multiplications and additions. Generally, it

2106-419: Is frequently used when discussing the method of undetermined coefficients and variation of parameters . For non-linear autonomous ODEs it is possible under some conditions to develop solutions of finite duration, meaning here that from its own dynamics, the system will reach the value zero at an ending time and stays there in zero forever after. These finite-duration solutions can't be analytical functions on

2187-440: Is generated, it propagates through the calculation. For example, the operation + on a computer is inexact. A calculation of the type ⁠ a + b + c + d + e {\displaystyle a+b+c+d+e} ⁠ is even more inexact. A truncation error is created when a mathematical procedure is approximated. To integrate a function exactly, an infinite sum of regions must be found, but numerically only

2268-406: Is important to estimate and control round-off errors arising from the use of floating-point arithmetic . Interpolation solves the following problem: given the value of some unknown function at a number of points, what value does that function have at some other point between the given points? Extrapolation is very similar to interpolation, except that now the value of the unknown function at

2349-472: Is known to approximate that of the continuous problem; this process is called ' discretization '. For example, the solution of a differential equation is a function . This function must be represented by a finite amount of data, for instance by its value at a finite number of points at its domain, even though this domain is a continuum . The study of errors forms an important part of numerical analysis. There are several ways in which error can be introduced in

2430-525: Is more useful for differentiation and integration , whereas Lagrange's notation y ′ , y ″ , … , y ( n ) {\displaystyle y',y'',\ldots ,y^{(n)}} is more useful for representing higher-order derivatives compactly, and Newton's notation ( y ˙ , y ¨ , y . . . ) {\displaystyle ({\dot {y}},{\ddot {y}},{\overset {...}{y}})}

2511-654: Is obvious from the names of important algorithms like Newton's method , Lagrange interpolation polynomial , Gaussian elimination , or Euler's method . The origins of modern numerical analysis are often linked to a 1947 paper by John von Neumann and Herman Goldstine , but others consider modern numerical analysis to go back to work by E. T. Whittaker in 1912. To facilitate computations by hand, large books were produced with formulas and tables of data such as interpolation points and function coefficients. Using these tables, often calculated out to 16 decimal places or more for some functions, one could look up values to plug into

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2592-587: Is often used in physics for representing derivatives of low order with respect to time. Given F {\displaystyle F} , a function of x {\displaystyle x} , y {\displaystyle y} , and derivatives of y {\displaystyle y} . Then an equation of the form is called an explicit ordinary differential equation of order n {\displaystyle n} . More generally, an implicit ordinary differential equation of order n {\displaystyle n} takes

2673-473: Is sold at a lemonade stand , at $ 1.00 per glass, that 197 glasses of lemonade can be sold per day, and that for each increase of $ 0.01, one less glass of lemonade will be sold per day. If $ 1.485 could be charged, profit would be maximized, but due to the constraint of having to charge a whole-cent amount, charging $ 1.48 or $ 1.49 per glass will both yield the maximum income of $ 220.52 per day. Differential equation: If 100 fans are set up to blow air from one end of

2754-790: Is the zero vector . In matrix form For a system of the form F ( x , y , y ′ ) = 0 {\displaystyle \mathbf {F} \left(x,\mathbf {y} ,\mathbf {y} '\right)={\boldsymbol {0}}} , some sources also require that the Jacobian matrix ∂ F ( x , u , v ) ∂ v {\displaystyle {\frac {\partial \mathbf {F} (x,\mathbf {u} ,\mathbf {v} )}{\partial \mathbf {v} }}} be non-singular in order to call this an implicit ODE [system]; an implicit ODE system satisfying this Jacobian non-singularity condition can be transformed into an explicit ODE system. In

2835-517: Is the open set in which F {\displaystyle F} is defined, and ∂ Ω ¯ {\displaystyle \partial {\bar {\Omega }}} is its boundary. Note that the maximum domain of the solution This means that F ( x , y ) = y 2 {\displaystyle F(x,y)=y^{2}} , which is C 1 {\displaystyle C^{1}} and therefore locally Lipschitz continuous, satisfying

2916-415: Is used and the result is an approximation of the true solution (assuming stability ). In contrast to direct methods, iterative methods are not expected to terminate in a finite number of steps, even if infinite precision were possible. Starting from an initial guess, iterative methods form successive approximations that converge to the exact solution only in the limit. A convergence test, often involving

2997-405: Is used in contrast with partial differential equations (PDEs) which may be with respect to more than one independent variable, and, less commonly, in contrast with stochastic differential equations (SDEs) where the progression is random. A linear differential equation is a differential equation that is defined by a linear polynomial in the unknown function and its derivatives, that

3078-1284: The IMSL and NAG libraries; a free-software alternative is the GNU Scientific Library . Over the years the Royal Statistical Society published numerous algorithms in its Applied Statistics (code for these "AS" functions is here ); ACM similarly, in its Transactions on Mathematical Software ("TOMS" code is here ). The Naval Surface Warfare Center several times published its Library of Mathematics Subroutines (code here ). There are several popular numerical computing applications such as MATLAB , TK Solver , S-PLUS , and IDL as well as free and open-source alternatives such as FreeMat , Scilab , GNU Octave (similar to Matlab), and IT++ (a C++ library). There are also programming languages such as R (similar to S-PLUS), Julia , and Python with libraries such as NumPy , SciPy and SymPy . Performance varies widely: while vector and matrix operations are usually fast, scalar loops may vary in speed by more than an order of magnitude. Many computer algebra systems such as Mathematica also benefit from

3159-473: The Jacobi method , Gauss–Seidel method , successive over-relaxation and conjugate gradient method are usually preferred for large systems. General iterative methods can be developed using a matrix splitting . Root-finding algorithms are used to solve nonlinear equations (they are so named since a root of a function is an argument for which the function yields zero). If the function is differentiable and

3240-415: The conjugate gradient method . For these methods the number of steps needed to obtain the exact solution is so large that an approximation is accepted in the same manner as for an iterative method. As an example, consider the problem of solving for the unknown quantity x . For the iterative method, apply the bisection method to f ( x ) = 3 x − 24. The initial values are a = 0, b = 3, f (

3321-404: The 1960s, hedge fund managers such as Ed Thorp and Michael Goodkin (working with Harry Markowitz, Paul Samuelson and Robert C. Merton ) pioneered the use of computers in arbitrage trading. In academics, sophisticated computer processing was needed by researchers such as Eugene Fama in order to analyze large amounts of financial data in support of the efficient-market hypothesis . During

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3402-412: The 1970s, the main focus of computational finance shifted to options pricing and analyzing mortgage securitizations . In the late 1970s and early 1980s, a group of young quantitative practitioners who became known as "rocket scientists" arrived on Wall Street and brought along personal computers . This led to an explosion of both the amount and variety of computational finance applications. Many of

3483-474: The Jacobian singularity criterion sufficient for this taxonomy to be comprehensive at all orders. The behavior of a system of ODEs can be visualized through the use of a phase portrait . Given a differential equation a function u : I ⊂ R → R {\displaystyle u:I\subset \mathbb {R} \to \mathbb {R} } , where I {\displaystyle I}

3564-498: The arbitrary constants in the general solution. In the context of linear ODE, the terminology particular solution can also refer to any solution of the ODE (not necessarily satisfying the initial conditions), which is then added to the homogeneous solution (a general solution of the homogeneous ODE), which then forms a general solution of the original ODE. This is the terminology used in the guessing method section in this article, and

3645-644: The arts. Current growth in computing power has enabled the use of more complex numerical analysis, providing detailed and realistic mathematical models in science and engineering. Examples of numerical analysis include: ordinary differential equations as found in celestial mechanics (predicting the motions of planets, stars and galaxies), numerical linear algebra in data analysis, and stochastic differential equations and Markov chains for simulating living cells in medicine and biology. Before modern computers, numerical methods often relied on hand interpolation formulas, using data from large printed tables. Since

3726-461: The author and upon which notation is most useful for the task at hand. In this context, the Leibniz's notation d y d x , d 2 y d x 2 , … , d n y d x n {\displaystyle {\frac {dy}{dx}},{\frac {d^{2}y}{dx^{2}}},\ldots ,{\frac {d^{n}y}{dx^{n}}}}

3807-429: The availability of arbitrary-precision arithmetic which can provide more accurate results. Ordinary differential equation In mathematics , an ordinary differential equation ( ODE ) is a differential equation (DE) dependent on only a single independent variable . As with other DE, its unknown(s) consists of one (or more) function(s) and involves the derivatives of those functions. The term "ordinary"

3888-472: The constraints are linear. A famous method in linear programming is the simplex method . The method of Lagrange multipliers can be used to reduce optimization problems with constraints to unconstrained optimization problems. Numerical integration, in some instances also known as numerical quadrature , asks for the value of a definite integral . Popular methods use one of the Newton–Cotes formulas (like

3969-519: The corresponding eigenfunctions form a complete, orthogonal set, which makes orthogonal expansions possible. This is a key idea in applied mathematics, physics, and engineering. SLPs are also useful in the analysis of certain partial differential equations. There are several theorems that establish existence and uniqueness of solutions to initial value problems involving ODEs both locally and globally. The two main theorems are In their basic form both of these theorems only guarantee local results, though

4050-399: The derivative is known, then Newton's method is a popular choice. Linearization is another technique for solving nonlinear equations. Several important problems can be phrased in terms of eigenvalue decompositions or singular value decompositions . For instance, the spectral image compression algorithm is based on the singular value decomposition. The corresponding tool in statistics

4131-480: The differential equation, and is indicated in the notation F ( x ( t ) ) {\displaystyle F(x(t))} . In what follows, y {\displaystyle y} is a dependent variable representing an unknown function y = f ( x ) {\displaystyle y=f(x)} of the independent variable x {\displaystyle x} . The notation for differentiation varies depending upon

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4212-724: The equation into an equivalent linear ODE (see, for example Riccati equation ). Some ODEs can be solved explicitly in terms of known functions and integrals . When that is not possible, the equation for computing the Taylor series of the solutions may be useful. For applied problems, numerical methods for ordinary differential equations can supply an approximation of the solution. Ordinary differential equations (ODEs) arise in many contexts of mathematics and social and natural sciences . Mathematical descriptions of change use differentials and derivatives. Various differentials, derivatives, and functions become related via equations, such that

4293-638: The equation is linear or not. For instance, the equation 2 x + 5 = 3 {\displaystyle 2x+5=3} is linear while 2 x 2 + 5 = 3 {\displaystyle 2x^{2}+5=3} is not. Much effort has been put in the development of methods for solving systems of linear equations . Standard direct methods, i.e., methods that use some matrix decomposition are Gaussian elimination , LU decomposition , Cholesky decomposition for symmetric (or hermitian ) and positive-definite matrix , and QR decomposition for non-square matrices. Iterative methods such as

4374-449: The field of numerical analysis is the design and analysis of techniques to give approximate but accurate solutions to a wide variety of hard problems, many of which are infeasible to solve symbolically: The field of numerical analysis predates the invention of modern computers by many centuries. Linear interpolation was already in use more than 2000 years ago. Many great mathematicians of the past were preoccupied by numerical analysis, as

4455-545: The first order as accepted circa 1900. The primitive attempt in dealing with differential equations had in view a reduction to quadratures . As it had been the hope of eighteenth-century algebraists to find a method for solving the general equation of the n {\displaystyle n} th degree, so it was the hope of analysts to find a general method for integrating any differential equation. Gauss (1799) showed, however, that complex differential equations require complex numbers . Hence, analysts began to substitute

4536-537: The force F {\displaystyle F} , is given by the differential equation which constrains the motion of a particle of constant mass m {\displaystyle m} . In general, F {\displaystyle F} is a function of the position x ( t ) {\displaystyle x(t)} of the particle at time t {\displaystyle t} . The unknown function x ( t ) {\displaystyle x(t)} appears on both sides of

4617-498: The form F ( x , y ) {\displaystyle F(x,y)} , and it can also be applied to systems of equations. When the hypotheses of the Picard–Lindelöf theorem are satisfied, then local existence and uniqueness can be extended to a global result. More precisely: For each initial condition ( x 0 , y 0 ) {\displaystyle (x_{0},y_{0})} there exists

4698-542: The form: There are further classifications: A number of coupled differential equations form a system of equations. If y {\displaystyle \mathbf {y} } is a vector whose elements are functions; y ( x ) = [ y 1 ( x ) , y 2 ( x ) , … , y m ( x ) ] {\displaystyle \mathbf {y} (x)=[y_{1}(x),y_{2}(x),\ldots ,y_{m}(x)]} , and F {\displaystyle \mathbf {F} }

4779-504: The formulas given and achieve very good numerical estimates of some functions. The canonical work in the field is the NIST publication edited by Abramowitz and Stegun , a 1000-plus page book of a very large number of commonly used formulas and functions and their values at many points. The function values are no longer very useful when a computer is available, but the large listing of formulas can still be very handy. The mechanical calculator

4860-814: The latter can be extended to give a global result, for example, if the conditions of Grönwall's inequality are met. Also, uniqueness theorems like the Lipschitz one above do not apply to DAE systems, which may have multiple solutions stemming from their (non-linear) algebraic part alone. The theorem can be stated simply as follows. For the equation and initial value problem: y ′ = F ( x , y ) , y 0 = y ( x 0 ) {\displaystyle y'=F(x,y)\,,\quad y_{0}=y(x_{0})} if F {\displaystyle F} and ∂ F / ∂ y {\displaystyle \partial F/\partial y} are continuous in

4941-514: The market equilibrium price changes). Many mathematicians have studied differential equations and contributed to the field, including Newton , Leibniz , the Bernoulli family , Riccati , Clairaut , d'Alembert , and Euler . A simple example is Newton's second law of motion—the relationship between the displacement x {\displaystyle x} and the time t {\displaystyle t} of an object under

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5022-403: The method of sparse grids . Numerical analysis is also concerned with computing (in an approximate way) the solution of differential equations , both ordinary differential equations and partial differential equations . Partial differential equations are solved by first discretizing the equation, bringing it into a finite-dimensional subspace. This can be done by a finite element method ,

5103-738: The mid 20th century, computers calculate the required functions instead, but many of the same formulas continue to be used in software algorithms. The numerical point of view goes back to the earliest mathematical writings. A tablet from the Yale Babylonian Collection ( YBC 7289 ), gives a sexagesimal numerical approximation of the square root of 2 , the length of the diagonal in a unit square . Numerical analysis continues this long tradition: rather than giving exact symbolic answers translated into digits and applicable only to real-world measurements, approximate solutions within specified error bounds are used. The overall goal of

5184-419: The middle of the nineteenth century has it received special attention. A valuable but little-known work on the subject is that of Houtain (1854). Darboux (from 1873) was a leader in the theory, and in the geometric interpretation of these solutions he opened a field worked by various writers, notably Casorati and Cayley . To the latter is due (1872) the theory of singular solutions of differential equations of

5265-445: The midpoint rule or Simpson's rule ) or Gaussian quadrature . These methods rely on a "divide and conquer" strategy, whereby an integral on a relatively large set is broken down into integrals on smaller sets. In higher dimensions, where these methods become prohibitively expensive in terms of computational effort, one may use Monte Carlo or quasi-Monte Carlo methods (see Monte Carlo integration ), or, in modestly large dimensions,

5346-549: The new techniques came from signal processing and speech recognition rather than traditional fields of computational economics like optimization and time series analysis. By the end of the 1980s, the winding down of the Cold War brought a large group of displaced physicists and applied mathematicians , many from behind the Iron Curtain , into finance. These people become known as " financial engineers " ("quant"

5427-623: The older mathematicians can, using Lie groups , be referred to a common source, and that ordinary differential equations that admit the same infinitesimal transformations present comparable integration difficulties. He also emphasized the subject of transformations of contact . Lie's group theory of differential equations has been certified, namely: (1) that it unifies the many ad hoc methods known for solving differential equations, and (2) that it provides powerful new ways to find solutions. The theory has applications to both ordinary and partial differential equations. A general solution approach uses

5508-438: The problem is well-conditioned , meaning that the solution changes by only a small amount if the problem data are changed by a small amount. To the contrary, if a problem is 'ill-conditioned', then any small error in the data will grow to be a large error. Both the original problem and the algorithm used to solve that problem can be well-conditioned or ill-conditioned, and any combination is possible. So an algorithm that solves

5589-402: The problems of mathematical analysis (as distinguished from discrete mathematics ). It is the study of numerical methods that attempt to find approximate solutions of problems rather than the exact ones. Numerical analysis finds application in all fields of engineering and the physical sciences, and in the 21st century also the life and social sciences like economics, medicine, business and even

5670-599: The residual , is specified in order to decide when a sufficiently accurate solution has (hopefully) been found. Even using infinite precision arithmetic these methods would not reach the solution within a finite number of steps (in general). Examples include Newton's method, the bisection method , and Jacobi iteration . In computational matrix algebra, iterative methods are generally needed for large problems. Iterative methods are more common than direct methods in numerical analysis. Some methods are direct in principle but are usually used as though they were not, e.g. GMRES and

5751-403: The room to the other and then a feather is dropped into the wind, what happens? The feather will follow the air currents, which may be very complex. One approximation is to measure the speed at which the air is blowing near the feather every second, and advance the simulated feather as if it were moving in a straight line at that same speed for one second, before measuring the wind speed again. This

5832-614: The same sources, implicit ODE systems with a singular Jacobian are termed differential algebraic equations (DAEs). This distinction is not merely one of terminology; DAEs have fundamentally different characteristics and are generally more involved to solve than (nonsingular) ODE systems. Presumably for additional derivatives, the Hessian matrix and so forth are also assumed non-singular according to this scheme, although note that any ODE of order greater than one can be (and usually is) rewritten as system of ODEs of first order , which makes

5913-422: The solution of the problem. Round-off errors arise because it is impossible to represent all real numbers exactly on a machine with finite memory (which is what all practical digital computers are). Truncation errors are committed when an iterative method is terminated or a mathematical procedure is approximated and the approximate solution differs from the exact solution. Similarly, discretization induces

5994-464: The study of functions, thus opening a new and fertile field. Cauchy was the first to appreciate the importance of this view. Thereafter, the real question was no longer whether a solution is possible by means of known functions or their integrals, but whether a given differential equation suffices for the definition of a function of the independent variable or variables, and, if so, what are the characteristic properties. Two memoirs by Fuchs inspired

6075-694: The successive derivatives of the unknown function y {\displaystyle y} of the variable x {\displaystyle x} . Among ordinary differential equations, linear differential equations play a prominent role for several reasons. Most elementary and special functions that are encountered in physics and applied mathematics are solutions of linear differential equations (see Holonomic function ). When physical phenomena are modeled with non-linear equations, they are generally approximated by linear differential equations for an easier solution. The few non-linear ODEs that can be solved explicitly are generally solved by transforming

6156-620: The symmetry property of differential equations, the continuous infinitesimal transformations of solutions to solutions ( Lie theory ). Continuous group theory , Lie algebras , and differential geometry are used to understand the structure of linear and non-linear (partial) differential equations for generating integrable equations, to find its Lax pairs , recursion operators, Bäcklund transform , and finally finding exact analytic solutions to DE. Symmetry methods have been applied to differential equations that arise in mathematics, physics, engineering, and other disciplines. Sturm–Liouville theory

6237-409: The whole real line, and because they will be non-Lipschitz functions at their ending time, they are not included in the uniqueness theorem of solutions of Lipschitz differential equations. As example, the equation: Admits the finite duration solution: The theory of singular solutions of ordinary and partial differential equations was a subject of research from the time of Leibniz, but only since

6318-410: Was 17 degrees at 2:00 and 18.5 degrees at 1:30pm. Extrapolation: If the gross domestic product of a country has been growing an average of 5% per year and was 100 billion last year, it might be extrapolated that it will be 105 billion this year. Regression: In linear regression, given n points, a line is computed that passes as close as possible to those n points. Optimization: Suppose lemonade

6399-402: Was also developed as a tool for hand computation. These calculators evolved into electronic computers in the 1940s, and it was then found that these computers were also useful for administrative purposes. But the invention of the computer also influenced the field of numerical analysis, since now longer and more complicated calculations could be done. The Leslie Fox Prize for Numerical Analysis

6480-558: Was initiated in 1985 by the Institute of Mathematics and its Applications . Direct methods compute the solution to a problem in a finite number of steps. These methods would give the precise answer if they were performed in infinite precision arithmetic . Examples include Gaussian elimination , the QR factorization method for solving systems of linear equations , and the simplex method of linear programming . In practice, finite precision

6561-491: Was offered by Carnegie Mellon University in 1994. Over the last 20 years, the field of computational finance has expanded into virtually every area of finance, and the demand for practitioners has grown dramatically. Moreover, many specialized companies have grown up to supply computational finance software and services. Numerical analysis Numerical analysis is the study of algorithms that use numerical approximation (as opposed to symbolic manipulations ) for

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