In various fields such as signal processing, imaging processing, analytical chemistry, and spectroscopic analysis, smoothing and differentiation is important and necessary. With a matrix approach, the Savitzky–Golay smoothing and differentiation filter was extended recently to even length. In this article, a more general approach is proposed for convenient computation.

In the classic article written by Savitzky and Golay (1), which has been cited more than 3800 times according to ISI Web of Science, a kind of digital filter for smoothing and differentiation was developed. In their approach, each successive subset of 2*m *+ 1 points is fitted by a polynomial of degree *n* (*n *≤2*m*) in the least-squares sense. The *s*-th (0 ≤ s ≤ *n*) differentiation (zeroth differentiation = smoothing) of the original data at the midpoint is obtained by performing the differentiation on the fitted polynomial rather than on the original data. Finally, the running least-squares polynomial fitting can be performed simply and automatically by convolving the entire input data with a digital filter of length 2*m *+ 1.

The history and development of the Savitzky–Golay (SG) smoothing and differentiation filter have been reviewed in brief (2). The original tabular coefficients of the SG filter have been corrected by Steinier et al. (3) and Madden (4) subsequently. The typo of a formula by Madden (4) has been spotted recently (5). As pointed out by Mark and Workman (5), one limitation is that the existing SG filter is subject to using an odd number of data subset. With a matrix approach, the SG filter was extended recently for even number (2*m*) data (i.e., the SG filter could have an even length [6]). The feasibility of the even-length SG filter has been validated with computer simulations (6). In the least-square strain estimator (LSQSE) of ultrasound elastography, it was concluded that a data subset of number 8 could obtain the best performance (7). This method is equivalent to the SG differentiation filter with a linear fitting (8), and the data subset of even number corresponds to an even length of the filter. As discussed in (6), for an even order differentiation, the SG filter of even length has a better characteristic of attenuation at the high frequency of ω= π than that of odd length. However, the matrix approach (6) is not very convenient to calculate the filter coefficients. In this article, a more general approach based upon Gram polynomials is developed to calculate the convolution coefficients of the even-length SG filter for all polynomial degrees, all differentiation orders, and all data points.

Consider an even number (2*m*, 2*m *– 1 ≥*n*) of data subset and assume the index of the data samples ranges from –*m *+ 1 to *m*. The data samples can be regarded equivalently as being symmetrical about the origin, by shifting the origin one half. Therefore, the input signal are represented by (6)

The matrix G_{(2m) x (n+1)} contains the convolution coefficients of the SG filter for different order differentiation at the origin (that is, the imaginary midpoint or the center of symmetry), given by (6)

where *n* is the fitting polynomial degree, S is the 2*m* x *n *+ 1 basic matrix, as (6)

where s_{i} is the *i*-th column vector of S.

The convolution coefficients for the s-th differentiation evaluated at the imaginary midpoint are given by (6)

where g_{s} is the *s*-th column vector of G, the subscript 0 represents the evaluated midpoint. With the matrix approach mentioned earlier, some closed-form solutions as well as the numerical table can be obtained (6). However, only the filter coefficients for the imaginary midpoint are convenient to obtain.

It is expected that it is difficult to obtain the matrix inversion (S^{T} S)^{-1} in Equation 2 with an explicit formula if *s* is large. Therefore, one would prefer numerical computation to symbolic computation. If *n* or *s* increase, however, the matrix S^{T} S tends to be ill conditioned (9). Hence, a more successful and general approach with the orthogonal polynomials (Gram polynomials or Legendre polynomials) has been proposed (9–11). In this article, such an approach also is extended for an even-length SG filter. All the equations are similar to those in (10), but the effects of the even number data and the aforementioned translation of the origin have been taken into account.

The smoothing and the differentiation are expressed as

and

respectively, where *f _{n} * (

The convolution coefficients in Equations 6 and 7 are calculated as

and

respectively, where (*a*)^{(b)} is a generalized factorial function given by

*P _{k,m}* (

*P ^{(s)k,m } * is the

According to the ordinary definition of the Gram polynomials and their derivatives given by Equations 11 and 12, respectively, the explicit expressions for some low-order Gram polynomials are calculated and listed as follows

However, Equations 11 and 12 are not very practical for calculation purposes, especially for calculating the derivatives. An alternative method using the recursive properties of the Gram polynomials and their derivatives can be expressed as

and

respectively.

The appendix contains the routines of the previously mentioned approach with Gram polynomials. With these routines, one easily can obtain results that are identical to those given by (6). Table I lists some results of the even-length SG filter for the midpoint of the data subset. Furthermore, the results in (6) or Equation 5 are only for the midpoint. Using Equations 8 and 9, the even-length SG filter evaluated at any position can be obtained easily. Note that *t* = 0 for the imaginary midpoint of the data subset, while *t* = –*m *+ 1/2, –*m* + 3/2 and *m* – 1/2 for the first, second, and last points, repetitively. Some convolution coefficients of the even-length SG filters evaluated at the sampled data points as well as those at the imaginary midpoint are given in Table II.

Table I. Convolution coefficients of the even-length SG filter (t = 0)

As can be seen in Table II, the SG filters for the midpoint are symmetrical (or antisymmetical), and therefore, have the advantage of linear phase. In addition, the asymmetric odd-length SG filters (for points except the midpoint) can distort data and have poorer noise attenuation (12), especially for the points far away from the the midpoint. They are useful in some cases, but should be applied with caution (12). It is expected that the asymmetric even-length SG filters will have some similar performances.

Table II. Convolution coefficients of the even-length SG filter (m = 3)

The even-length SG filter for the midpoint is similar to the interpolation in the sense of least square polynomial fitting (2*m* – 1 > *p*) or polynomial approximation (2*m* – 1 = *p*). Therefore, the results of smoothing and differentiation correspond to an imaginary point between the original sampled data points, rather than the same wavelength as one of the original data. To avoid the asymmetry, the even-length SG filter evaluated at the midpoint also can be used for the neighboring sampled points. However, that will result in a time delay of half a sampling interval and a worse performance accordingly (6). For example, the two-point backward derivative formula, which can be regarded as an even-length SG differentiation filter (6), is more precise to calculate the derivative at a point halfway between the data points, rather than at either one of the two points. Fortunately, it does not matter when the sampling interval is small enough.

The widely used SG filter was extended recently for even number data subset. In this article, a more general approach with Gram polynomials is proposed to calculate the convolution coefficients of the even-length SG filter for all polynomial degrees, all differentiation orders, and all evaluated points.

The routines of the even-length SG filter written in MATLAB (The MathWorks, Inc., Natick, MA) can be found in (13). The routines of the Gram polynomial approach presented in this paper are given as below. They also are written in MATLAB and can obtain both of the numerical results and the symbolic results (by using the Symbolic Math Toolbox). However, the symbolic calculation is much slower.

function hnstm = gsdf_even_gram_poly (n,s,t,m)

% hnstm = sgsdf_gram_poly(n,s,t,m)

% n: polynomial degree

% s: derivative(differentiation) order (0 = smoothing)

% t: evaluation point (commonly, t = 0, i.e., smoothing or differentiation

% at the imaginary central point of the 2*m points)

% 2*m: data point number, i.e., filter length

% hnstm: convolution coefficients

hnstm = [];

for i = -m + 1/2:m - 1/2

hnstm = [hnstm hinstm(i,n,s,t,m)];

end

function value=hinstm(i,n,s,t,m)

% Equs. (8) and (9)

value=0;

for k=0:n

value=value+(2*k+1)*gff(2*m1,k)/gff(2*m+k,k+1)*...

Pkmi(k,m,i)*Pkmsi(k,m,s,t);

end

function value = gff(a,b)

% generalized factorial function (Equation 10)

if b == 0

value = 1;

else

value = prod(a-(0:b - 1));

end

function value = Pkmsi(k,m,s,i)

% s-th derivative of Gram polynomials (Equation 15)

if s == 0

value = Pkmi(k,m,i);

else if k == -1 || k == 0

value = 0;

else

value = 2*(2*k-1)/k/(2*m-k)*(i*Pkmsi(k-1,m,s,i)+s*Pkmsi(k-1,m,s-1,i))-...

(k-1)*(2*m+k-1)/k/(2*m-k)*Pkmsi(k-2,m,s,i);

end

function value = Pkmi(k,m,i)

% Gram polynomials (Equation 14)

if k == -1

value = 0;

else if k == 0

value=1;

else

value = 2*(2*k-1)/k/(2*m-k)*i*Pkmi(k-1,m,i)-(k-1)*(2*m+k-1)/k/(2*m-k)*Pkmi(k-2,m,i);

end

The closed-form solutions listed in (2) can be obtained with the following routine.

function sgsdf_even_closed_form(n,s)

% n: polynomial degree

% s: derivative(differentiation) order (0 = smoothing)

subs(factor(hinstm(sym('k'),n,s, sym(0), sym('m'))),'k', 'k-1/2')

Some examples of the usage of these routines are given in Table III.

Table III. Some examples of the usage of the MATLAB routines

This work is supported in part by the National Natural Science Foundation of China (60171039, 30470466).

1. A. Savitzky and M.J.E. Golay, *Anal. Chem. ***36**(8), 1627–1639 (1964).

2. J.W. Luo, K. Ying, P. He, and J. Bai, *Digit. Signal Prog*. **15**(2), 122–136 (2005).

3. J. Steinier, Y. Termonia, and J. Deltour, *Anal. Chem*. **44**(11), 1906–1909 (1972).

4. H.H. Madden, *Anal. Chem. ***50**(9), 1383–1386 (1978).

5. H. Mark and J. Workman, *Spectroscopy ***18**(12), 106–111 (2003).

6. J.W. Luo, K. Ying, and J. Bai, *Signal Process*., **85**(7) 1429–1434 (2005).

7. F. Kallel and J. Ophir, *Ultrason. Imaging ***19**(3), 195–208 (1997).

8. J.W. Luo, J. Bai, P. He, and K. Ying, *IEEE Trans. Ultrason. Ferroelectr. Freq. Control ***51**(9), 1119–1127 (2004).

9. J.S. Lim, and A.V. Oppenheim, Eds., *Advanced Topics in Signal Processing* (Prentice-Hall, Englewood Cliffs, NJ, 1988).

10. P.A. Gorry, *Anal. Chem*. **62**(6), 570–573 (1990).

11. J.S. Waugh, Ed., *Advances in Magnetic Resonance* (Academic Press, New York, NY, 1966), vol. 2.

12. P.D. Wentzell, T.P. Doherty, and S.R. Crouch, *Anal. Chem.*s **59**(2), 367–371 (1987).

13. The MATLAB Central File Exchange, at: http://www.mathworks.com/matlabcentral/fileexchange/loadCategory.do?objectId=66&objectType=Category.

**Jianwen Luo **and **Jing Bai** are with the Department of Biomedical Engineering at Tsinghua University (Beijing, China). E-mail: jianwen.luo@gmail.com

Articles in this issue

Savitzky–Golay Smoothing and Differentiation Filter of Even Length: A Gram Polynomial Approach

Focus on Quality — Validation of Spectrometry Software: Importance of Accurate Date and Time Stamps

Tutorial — Mass Analyzers: An Overview of Several Designs and Their Applications, Part I

Continuous Wave Optical Parametric Oscillators Break New Spectral Ground