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Apply the general formalism of the recurrence relations given in the book to find the following two relations for Laguerre polynomials: (a) \(n L_{n}^{v}-(n+v) L_{n-1}^{v}-x \frac{d L_{n}^{v}}{d x}=0 .\) (b) \((n+1) L_{n+1}^{v}-(2 n+v+1-x) L_{n}^{v}+(n+v) L_{n-1}^{v}=0 .\)

Short Answer

Expert verified
The solution to these problems involves applying the general formalism of recurrence relations to the given Laguerre polynomials. This will involve taking the derivative with respect to x, then simplifying using basic algebraic manipulation. Finally, the form will be checked against the given relations.

Step by step solution

01

Analyzing the recurrence relations

First, look at the given equations. These are the recurrence relations of the Laguerre polynomials which need to be derived using the given formalism.
02

Apply the general formalism

The general formalism of recurrence relations for the Laguerre polynomials is given by the formula: \(L_{n}^{v}= \frac{e^{x} x^{-v}}{n!} \frac{d^n (e^{-x} x^{n+v})}{dx^n}\). Apply this formula to each recurrence relation.
03

Differentiating the Laguerre polynomials

Use the given formalism to differentiate the Laguerre polynomials for the two relations. In each case, the derivative \( \frac{d L_{n}^{v}}{d x} \) will need to be computed before the equation can be solved.
04

Solving the equations

After differentiating as needed, the equations should be solvable by algebraic manipulation. Use the laws of indices to simplify each equation and isolate the Laguerre polynomial on one side, if necessary.
05

Final check

Check the final forms against the given relations. This will involve making sure the indices of the recurrences match as provided in the problem statement and that the general form for each is preserved.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Recurrence Relations
Recurrence relations are mathematical expressions that define sequences iteratively by relating future values to present and past ones. They are fundamental tools in numerical analysis, helping to simplify complex problems. In the context of Laguerre polynomials, recurrence relations allow us to connect different polynomials in the series by expressing a given polynomial in terms of its predecessors.

Understanding recurrence relations provides an analytical framework for solving higher-order problems by breaking them down into related, simpler ones. For example, when dealing with the Laguerre polynomials, recurrence relations serve as a shortcut to generate higher-degree polynomials from known lower-degree ones without recourse to the full-blown generative formula each time.
Differential Equations
Differential equations are equations involving derivatives that indicate how a function changes over time or space. In mathematical physics and many other sciences, they are used extensively to model real-world phenomena.

For the Laguerre polynomials, differential equations showcase the rate of change of these polynomials with respect to a variable, often 'x'. The process of differentiating in step 3 of our exercise is actually the act of solving a differential equation to find the polynomial's form at a specific instant. This approach is central to understanding the behavior and properties of the functions that describe physical systems, like wave functions in quantum mechanics, where orthogonal polynomials like those of Laguerre often arise.
Mathematical Physics
Mathematical physics refers to the application of mathematical methods to solve problems in physics and developing new mathematical techniques suitable for such applications and for the formulation of physical theories. It is a rich field where concepts like differentiation, series expansion, and, importantly, orthogonal polynomials, like Laguerre polynomials, have critical roles.

These polynomials often emerge in the solutions to the Schrödinger equation in quantum mechanics or in describing the statistical distribution of energy states in physical systems. The recurrence relations from our exercise are not just abstract mathematical constructs; they have concrete applications in finding solutions to problems in electromagnetic theory, quantum mechanics, and other physics domains.
Orthogonal Polynomials
Orthogonal polynomials are a class of polynomials that adhere to a specific orthogonality relation under some weighting function over a certain interval. This property is harnessed in various fields, such as in approximation theory and numerical analysis, because of their desirable attributes in representing functions.

The Laguerre polynomials make up one such family of orthogonal polynomials. They are particularly useful because of their property of weighting exp(-x), which makes them applicable for functions involving exponential decay, a common scenario in both physical and engineering problems. The two recurrence relations we encounter in the exercise affirm the interconnected nature of these polynomials and highlight the systematic approach to generate the entire family from a fixed set of rules or formulas.

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Most popular questions from this chapter

Expand \(|x|\) in the interval \((-1,+1)\) in terms of Legendre polynomials.

Use the expansion of the generating function for Hermite polynomials to obtain $$\sum_{m, n=0}^{\infty} e^{-x^{2}} H_{m}(x) H_{n}(x) \frac{s^{m} t^{n}}{m ! n !}=e^{-x^{2}+2 x(s+t)-\left(s^{2}+t^{2}\right)}$$ Then integrate both sides over \(x\) and use the orthogonality of the Hermite polynomials to get $$\sum_{n=0}^{\infty} \frac{(s t)^{n}}{(n !)^{2}} \int_{-\infty}^{\infty} e^{-x^{2}} H_{n}^{2}(x) d x=\sqrt{\pi} e^{2 s t}$$ Deduce from this the normalization constant \(h_{n}\) of \(H_{n}(x)\).

Show that for Legendre polynomials, \(k_{n}^{(n)}=2^{n} \Gamma\left(n+\frac{1}{2}\right) /\left[n ! \Gamma\left(\frac{1}{2}\right)\right]\). Hint: Multiply and divide the expression given in the book by \(n !\); take a factor of 2 out of all terms in the numerator; the even terms yield a factor of \(n !\), and the odd terms give a gamma function.

Use a recurrence relations for Hermite polynomials to show that $$H_{n}(0)=\left\\{\begin{array}{ll} 0 & \text { if } n \text { is odd } \\\\(-1)^{m} \frac{(2 m) !}{m !} & \text { if } n=2 m . \end{array}\right.$$

Let \(L_{n} \equiv L_{n}^{0}\). Now differentiate both sides of $$g(x, t)=\frac{e^{-x t /(1-t)}}{1-t}=\sum_{0}^{\infty} t^{n} L_{n}(x)$$ with respect to \(x\) and compare powers of \(t\) to obtain \(L_{n}^{\prime}(0)=-n\) and \(L_{n}^{\prime \prime}(0)=\frac{1}{2} n(n-1)\). Hint: Differentiate \(1 /(1-t)=\sum_{n=0}^{\infty} t^{n}\) to get an ex- pression for \((1-t)^{-2}\).

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