Laguerre polynomials

Laguerre polynomials  are a sequence of polynomials that are solutions to the Laguerre differential equation:

where is a constant.

When , eq420 simplifies to . The solution to this first-order differential equation is , which can be expressed as the Taylor series . This implies that eq420 has a power series solution around . To determine the exact form of the power series solution to eq420, let .

Substituting , and  in eq420 yields

Setting in the first sum,

Eq422 is only true if all coefficients of in is 0 (see this article for explanation). So, , or equivalently,

Eq423 is a recurrence relation. If we know the value of , we can use the relation to find .

Recurrence relation

Comparing the recurrence relations, we have

where by convention (so that ).

Letting in eq424 and substituting it in yields the Laguerre polynomials:

where we have replaced with .

The first few Laguerre polynomials are:

 

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Rodrigues’ formula for the Laguerre polynomials

The Rodrigues’ formula for the Laguerre polynomials is a mathematical expression that provides a method to calculate any Laguerre polynomial using differentiation.

It is given by

To prove eq428, we apply Leibniz’ theorem as follows:

Substituting and in the above equation and rearranging yields

Letting , we have , which is the expression for the Laguerre polynomials

 

Question

How do we change the variable in the summation by letting ?

Answer

When , , and when , . So, . Reversing the summation order, .

 

 

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Generating function for the Laguerre polynomials

The generating function for the Laguerre polynomials is a mathematical tool that, when expanded as a power series, produces Laguerre polynomials as its coefficients in terms of a variable.

Eq430 means that the cofficient of in the expansion of is . To prove this, we expand the exponential term as a Taylor series:

Expanding as a binomial series gives

Since ,

Letting

We now have a sum over and then over . Since and both and range from to , the sum over  ranges from to . The new range of in the outer sum is determined by the conditions that and , where and range from to . Consequently, has a lower limit of 0 and an upper limit of . Eq431, after swapping the order of summation, then becomes

where are the Laguerre polynomials.

 

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Recurrence relations of the Laguerre Polynomials

The recurrence relations of the Laguerre polynomials describe how each polynomial in the sequence can be obtained from its predecessors.

Some useful recurrence relations of the Laguerre polynomials include

To derive eq434, differentiate eq430 with respect to to give

Substituting eq430 gives

Equating the coefficients of yields

which rearranges to eq434.

To derive eq435, differentiate eq430 with respect to to give

Substituting eq430 gives

Equating the coefficients of yields eq435. To derive eq436, differentiate eq434 with respect to to yield

Substituting eq435 gives

Letting in eq435, substituting the result in the above equation and rearranging yields eq436.

 

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Associated Laguerre polynomials

The associated Laguerre polynomials are a sequence of polynomials that are solutions to the associated Laguerre differential equation:

where are the associated Laguerre polynomials.

To show that are solutions to eq442, we refer to eq420, where . Letting , we have . Differentiating this equation times with respect to gives

Applying Leibniz’ theorem,

This implies that . Since is also a solution to the associated Laguerre differential equation, can also be expressed as

When , eq442 becomes the Laguerre differential equation. Therefore, . Substituting eq425 in eq443 yields

For , the terms in the summation equal zero. For , we note that , and so,

Letting ,

Eq444 is the general expression for the un-normalised associated Laguerre polynomials. Using eq444, the first few associated Laguerre polynomials in terms of are

 

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Orthogonality of the Laguerre polynomials

The orthogonality of the Laguerre polynomials states that the integral of the product of two distinct Laguerre polynomials over a specified interval is zero.

It is defined mathematically as:

where is known as a weight function.

 

Question

Why is the weight function included? Can the orthogonality of the Laguerre polynomials be defined as , where ? Why are the limits of integration from 0 to ?

Answer

The weight function is an integral part of the orthogonality definition of Laguerre polynomials due to its role in ensuring convergence and its practical applications. It is often tied to specific problems, such as those in quantum mechanics. Omitting the weight function would sever this connection and could potentially alter the orthogonality properties of the polynomials. Therefore, defining orthogonality without the weight function would generally be invalid and would not reflect the intended use and properties of the Laguerre polynomials.

The weight function naturally defines the integration range because as , making the integral convergent over this range. This range is also connected to specific problems, such as the radial part of the wave functions in quantum mechanics. In the context of the hydrogen atom, represents a distance, which is always non-negative.

 

To prove eq438, we multiply eq430 for and to give

Multiplying through by and integrating with respect to yields

which simplifies to

Expressing the LHS as a binomial series gives

Equating the coefficients of when gives eq438. If we further equate the coefficients of when , we have .

Therefore,

 

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Rodrigues’ formula for the associated Laguerre polynomials

The Rodrigues’ formula for the associated Laguerre polynomials is a mathematical expression that provides a method to calculate any associated Laguerre polynomial using differentiation.

It is given by

To prove eq446, we apply Leibniz’ theorem as follows:

Substituting and in the above equation and rearranging yields

Letting , we have , which is the expression for the associated Laguerre polynomials.

 

Question

How do we change the variable in the summation by letting ?

Answer

When , , and when , . So, . Reversing the summation order, .

 

 

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Generating functions for the associated Laguerre polynomials

The generating function for the associated Laguerre polynomials is a mathematical tool that, when expanded as a power series, produces associated Laguerre polynomials as its coefficients in terms of a variable.

It is defined as

To prove eq448, we differentiate the generating function for the Laguerre polynomials (see eq430) times with respect to to give

When , the terms in the summation equal zero. So,

From eq443, , which when substituted in the above equation yields,

Letting gives

which rearranges to eq448.

 

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Recurrence relations of the associated Laguerre Polynomials

The recurrence relations of the associated Laguerre polynomials describe how each polynomial in the sequence can be obtained from its predecessors.

Some useful recurrence relations of the associated Laguerre polynomials include

Eq450 can be proven by differentiating the generating function for the associated Laguerre polynomials (see eq448) with respect to to give

Substituting eq448 yields

Equating the coefficients of  and rearranging them results in eq450. Eq451 can be proven by replacing with in the recurrence relations of the Laguerre polynomials (see eq436) to give

Differentiating this equation times with respect to using Leibniz’ theorem and multiplying through by yields

Only the last two terms in the summation ( and ) survives. Therefore,

Substituting eq443 and rearranging the result gives eq451.

 

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Orthogonality of the associated Laguerre polynomials

The orthogonality of the associated Laguerre polynomials states that the integral of the product of two distinct associated Laguerre polynomials over a specified interval is zero.

It is defined mathematically as:

where is known as a weight function.

 

Question

Why is the weight function included? Can the orthogonality of the associated Laguerre polynomials be defined as , where ? Why are the limits of integration from 0 to ? Why are the polynomials and not ?

Answer

The weight function is an integral part of the orthogonality definition of associated Laguerre polynomials due to its role in ensuring convergence and its practical applications. It is often tied to specific problems, such as those in quantum mechanics. Omitting the weight function would sever this connection and could potentially alter the orthogonality properties of the polynomials. Therefore, defining orthogonality without the weight function would generally be invalid and would not reflect the intended use and properties of the associated Laguerre polynomials.

The weight function naturally defines the integration range because as , making the integral convergent over this range. This range is also connected to specific problems, such as the radial part of the wave functions in quantum mechanics. In the context of the hydrogen atom, represents a distance, which is always non-negative.

The eigenvalue of is a function of and not . Since the eigenfunctions of a Hermitian operator are orthogonal, two associated Laguerre polynomials with distinct values of  must be orthogonal. If we allow the values of to be different, we wouldn’t know if the result of the integral is solely due to the values of .

 

To prove eq453, we multiply the generating function for the associated Laguerre polynomials (see eq448) for and to give

Multiplying through by and integrating with respect to yields

 

Question

Show that , where is a non-negative integer.,

Answer

Let , and , and then and . Integrating by parts,

Let and , and then and . Integrating by parts

If we carry out integrations by parts, we have

 

Therefore, eq454 becomes

Expressing the LHS as a binomial series,

So,

Equating the coefficients of when  gives eq453.

 

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