Connect via MCP →

Enter Calculation

Formula

Advertisement

Results

L31(x) at x = 0
4
degree n = 3, parameter α = 1
Rows generated 51
x range 0 to 5
Last value 3.166667
x L31(x)
0 4
0.1 3.419833
0.2 2.878667
0.3 2.3755
0.4 1.909333
0.5 1.479167
0.6 1.084
0.7 0.722833
0.8 0.394667
0.9 0.0985
1 -0.166667
1.1 -0.401833
1.2 -0.608
1.3 -0.786167
1.4 -0.937333
1.5 -1.0625
1.6 -1.162667
1.7 -1.238833
1.8 -1.292
1.9 -1.323167
2 -1.333333
2.1 -1.3235
2.2 -1.294667
2.3 -1.247833
2.4 -1.184
2.5 -1.104167
2.6 -1.009333
2.7 -0.9005
2.8 -0.778667
2.9 -0.644833
3 -0.5
3.1 -0.345167
3.2 -0.181333
3.3 -0.0095
3.4 0.169333
3.5 0.354167
3.6 0.544
3.7 0.737833
3.8 0.934667
3.9 1.1335
4 1.333333
4.1 1.533167
4.2 1.732
4.3 1.928833
4.4 2.122667
4.5 2.3125
4.6 2.497333
4.7 2.676167
4.8 2.848
4.9 3.011833
5 3.166667

What this calculator does

This tool tabulates the associated (generalized) Laguerre polynomial \(L_{n}^{(\alpha)}(x)\) over a sequence of x values. You provide the degree n, the parameter α, a starting x, a step size, and how many rows to generate. The calculator returns the value of the polynomial at each x. It is pure mathematics and applies universally — no region- or country-specific assumptions.

How to use it

Enter n (a non-negative integer), α (any real number; the standard orthogonality case uses \(\alpha > -1\)), the initial value of x, the increment, and the number of rows. The x values are generated as $$x_i = \text{startX} + i \times \text{stepX}$$ for \(i = 0, 1, \dots, \text{count}-1\), and each value \(L_{n}^{(\alpha)}(x_i)\) is computed and listed.

The formula explained

The closed form is a finite sum, $$L_{n}^{(\alpha)}(x) = \sum_{k=0}^{n} (-1)^k \binom{n+\alpha}{n-k} \frac{x^k}{k!},$$ where \(\binom{n+\alpha}{n-k}\) is the generalized binomial coefficient. For numerical stability the calculator instead uses the three-term recurrence: $$L_0 = 1,\quad L_1 = 1 + \alpha - x,\quad (k+1)L_{k+1} = (2k+1+\alpha-x)L_{k} - (k+\alpha)L_{k-1}.$$ This avoids large factorials and cancellation for moderate-to-large n.

Graph of several associated Laguerre polynomial curves crossing the x-axis
Associated Laguerre polynomials oscillate and cross zero more often as the degree n increases.

Worked example

With the defaults \(n = 3\), \(\alpha = 1\) the explicit polynomial is $$L_{3}^{(1)}(x) = 4 - 6x + 2x^2 - \tfrac{1}{6}x^3.$$ At \(x = 0\) the value is \(4\). At \(x = 0.1\) it is $$4 - 0.6 + 0.02 - 0.0001667 \approx 3.419833.$$ At \(x = 1\) it equals $$4 - 6 + 2 - 0.166667 = -0.166667.$$

First Associated Laguerre Polynomials

The associated (generalized) Laguerre polynomials \(L_n^{(\alpha)}(x)\) are polynomials of degree \(n\) in \(x\) whose coefficients depend on the parameter \(\alpha\). The closed form is

$$L_n^{(\alpha)}(x)=\sum_{k=0}^{n}(-1)^k\binom{n+\alpha}{n-k}\frac{x^k}{k!}.$$

The first five, written in general \(\alpha\) form, are:

\(n\) \(L_n^{(\alpha)}(x)\)
0 \(1\)
1 \(-x+(\alpha+1)\)
2 \(\dfrac{x^2}{2}-(\alpha+2)x+\dfrac{(\alpha+1)(\alpha+2)}{2}\)
3 \(-\dfrac{x^3}{6}+\dfrac{(\alpha+3)x^2}{2}-\dfrac{(\alpha+2)(\alpha+3)x}{2}+\dfrac{(\alpha+1)(\alpha+2)(\alpha+3)}{6}\)
4 \(\dfrac{x^4}{24}-\dfrac{(\alpha+4)x^3}{6}+\dfrac{(\alpha+3)(\alpha+4)x^2}{4}-\dfrac{(\alpha+2)(\alpha+3)(\alpha+4)x}{6}+\dfrac{(\alpha+1)(\alpha+2)(\alpha+3)(\alpha+4)}{24}\)

Special case \(\alpha=0\). Setting \(\alpha=0\) recovers the ordinary Laguerre polynomials \(L_n(x)=L_n^{(0)}(x)\):

\(n\) \(L_n(x)\)
0 \(1\)
1 \(1-x\)
2 \(1-2x+\tfrac12 x^2\)
3 \(1-3x+\tfrac32 x^2-\tfrac16 x^3\)
4 \(1-4x+3x^2-\tfrac23 x^3+\tfrac{1}{24}x^4\)

The leading coefficient is always \(\dfrac{(-1)^n}{n!}\), independent of \(\alpha\).

Key Terms & Variables

Degree \(n\)
A non-negative integer giving the polynomial degree; \(L_n^{(\alpha)}(x)\) has exactly \(n\) roots. In the calculator this is the field degree.
Parameter \(\alpha\)
A real number (commonly \(\alpha>-1\)) that shifts the binomial coefficients and the orthogonality weight. The field alpha. With \(\alpha=0\) the polynomials reduce to the ordinary Laguerre polynomials.
Argument \(x\)
The point at which the polynomial is evaluated. The table sweeps \(x_i=\text{startX}+i\cdot\text{stepX}\). The natural domain for orthogonality is \((0,\infty)\).
Generalized binomial coefficient
For real upper index, \(\binom{n+\alpha}{n-k}=\dfrac{\Gamma(n+\alpha+1)}{\Gamma(k+\alpha+1)\,(n-k)!}\), which extends \(\binom{m}{j}=m!/(j!(m-j)!)\) to non-integer \(\alpha\) via the Gamma function.
Three-term recurrence
The stable way to generate the polynomials: \((k+1)L_{k+1}^{(\alpha)}=(2k+1+\alpha-x)L_k^{(\alpha)}-(k+\alpha)L_{k-1}^{(\alpha)}\), starting from \(L_0^{(\alpha)}=1\) and \(L_1^{(\alpha)}=1+\alpha-x\).
Orthogonality on \((0,\infty)\)
The polynomials are mutually orthogonal: \(\displaystyle\int_0^\infty L_n^{(\alpha)}(x)L_m^{(\alpha)}(x)\,w(x)\,dx=\frac{\Gamma(n+\alpha+1)}{n!}\delta_{nm}\).
Weight function \(w(x)=x^{\alpha}e^{-x}\)
The factor against which orthogonality holds; for \(\alpha=0\) it is the simple exponential weight \(e^{-x}\). Convergence of the integral requires \(\alpha>-1\).

Interpreting the Table

Reading a computed table of \(L_n^{(\alpha)}(x)\) becomes easier with these facts:

  • Number of real roots. For \(\alpha>-1\), \(L_n^{(\alpha)}(x)\) has exactly \(n\) simple real zeros, all lying in the open interval \((0,\infty)\). If your table column crosses zero \(n\) times, you have located all of them.
  • Sign changes. Because all zeros are simple, the polynomial changes sign at each one. Between two consecutive zeros the values keep a constant sign, so a sign flip between adjacent rows brackets a root — useful as a starting interval for a bisection or Newton root finder.
  • Value at the origin. Every associated Laguerre polynomial satisfies \(L_n^{(\alpha)}(0)=\binom{n+\alpha}{n}=\dfrac{\Gamma(n+\alpha+1)}{n!\,\Gamma(\alpha+1)}\). For example, with \(n=4,\ \alpha=0\) the first row at \(x=0\) is 1, and with \(n=4,\ \alpha=2\) it is \(\binom{6}{4}=\) 15.
  • Quantum mechanics. The radial part of the hydrogen-atom wavefunction is built from \(L_{n-\ell-1}^{(2\ell+1)}\!\left(2r/(na_0)\right)\); the polynomial's nodes correspond to the radial nodes of the orbital.
  • Gauss–Laguerre quadrature. The zeros listed in the table are exactly the abscissae used to approximate \(\int_0^\infty f(x)\,x^{\alpha}e^{-x}\,dx\), with weights derived from the same polynomials.

This is general mathematical reference information; verify any value you rely on in a critical application.

FAQ

What if n = 0? \(L_{0}^{(\alpha)}(x) = 1\) for every x and every α.

Can α be negative or non-integer? Yes — both the sum and the recurrence work for any real α. The classical orthogonality on \((0, \infty)\) requires \(\alpha > -1\).

Can the step be zero or negative? Yes. A negative step walks x downward; a zero step repeats the same x and produces a degenerate (constant-x) table.

Last updated: