It is the first of the polygamma functions.
Relation to harmonic numbers 
where Hn is the nth harmonic number, and γ is the Euler-Mascheroni constant. For half-integer values, it may be expressed as
Integral representations 
If the real part of is positive then the digamma function has the following integral representation
This may be written as
which follows from Euler's integral formula for the harmonic numbers.
Series formula 
Digamma can be computed in the complex plane outside negative integers (Abramowitz and Stegun 6.3.16), using
This can be utilized to evaluate infinite sums of rational functions, i.e., , where p(n) and q(n) are polynomials of n.
Performing partial fraction on un in the complex field, in the case when all roots of q(n) are simple roots,
For the series to converge,
or otherwise the series will be greater than harmonic series and thus diverges.
With the series expansion of higher rank polygamma function a generalized formula can be given as
provided the series on the left converges.
Taylor series 
Newton series 
The Newton series for the digamma follows from Euler's integral formula:
where is the binomial coefficient.
Reflection formula 
Recurrence formula and characterization 
The digamma function satisfies the recurrence relation
- (see proof)
Thus, it can be said to "telescope" 1/x, for one has
where is the Euler-Mascheroni constant.
More generally, one has
Actually, is the only solution of the functional equation that is monotone on and satisfies . This fact follows immediately from the uniqueness of the function given its recurrence equation and convexity-restriction. This implies the useful difference equation :
Gaussian sum 
The digamma has a Gaussian sum of the form
and a neat generalization of this is
where q must be a natural number, but 1-qa not.
Gauss's digamma theorem 
For positive integers m and k (with m < k), the digamma function may be expressed in finite many terms of elementary functions as
and because of its recurrence equation for all rational arguments.
Computation and approximation 
which is the beginning of the asymptotical expansion of . The full asymptotic series of this expansions is
where is the kth Bernoulli number and is the Riemann zeta function. Although the infinite sum converges for no x, this expansion becomes more accurate for larger values of x and any finite partial sum cut off from the full series. To compute for small x, the recurrence relation
can be used to shift the value of x to a higher value. Beal suggests using the above recurrence to shift x to a value greater than 6 and then applying the above expansion with terms above cut off, which yields "more than enough precision" (at least 12 digits except near the zeroes).
- (see proof)
From the above asymptotic series for you can derive asymptotic series for that contain only rational functions and constants. The first series matches the overall behaviour of well, that is, it behaves asymptotically identically for large arguments and has a zero of unbounded multiplicity at the origin, too. It can be considered a Taylor expansion of at .
The other expansion is more precise for large arguments and saves computing terms of even order.
(See derivation of all coefficients.)
Special values 
The digamma function has values in closed form for rational numbers, as a result of Gauss's digamma theorem. Some are listed below:
The roots of the digamma function are the saddle points of the complex-valued gamma function. Thus they lie all on the real axis. The only one on the positive real axis is the unique minimum of the real-valued gamma function on at . All others occur single between the pols on the negative axis: . Already 1881 Hermite observed that holds asymptotically . A better approximation of the location of the roots is given by
and using a further term it becomes still better
which both spring off the reflection formula via and substituting by its not convergent asymptotic expansion. The correct 2nd term of this expansion is of course , where the given one works good to approximate roots with small index n.
the Digamma function appears in the regularization of divergent integrals , this integral can be approximated by a divergent general Harmonic series , but the following value can be attached to the series
See also 
- Polygamma function
- Trigamma function
- Chebyshev expansions of the Digamma function in Wimp, Jet (1961). "Polynomial approximations to integral transforms". Math. Comp. 15: 174–178. doi:10.1090/S0025-5718-61-99221-3.
- Abramowitz, M.; Stegun, I. A., eds. (1972). "6.3 psi (Digamma) Function.". Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. New York: Dover. pp. 258–259. Unknown parameter
- Weisstein, Eric W., "Digamma function", MathWorld.
- Bernardo, José M. (1976). "Algorithm AS 103 psi(digamma function) computation". Applied Statistics 25: 315–317.
- Beal, Matthew J. (2003). Variational Algorithms for Approximate Bayesian Inference (PhD thesis). The Gatsby Computational Neuroscience Unit, University College London. pp. 265–266.