Abstract

The expected number of real zeros of an algebraic polynomial 𝑎𝑜+𝑎1𝑥+𝑎2𝑥2++𝑎𝑛𝑥𝑛 with random coefficient 𝑎𝑗,𝑗=0,1,2,,𝑛 is known. The distribution of the coefficients is often assumed to be identical albeit allowed to have different classes of distributions. For the nonidentical case, there has been much interest where the variance of the 𝑗th coefficient is var(𝑎𝑗)=𝑛𝑗. It is shown that this class of polynomials has significantly more zeros than the classical algebraic polynomials with identical coefficients. However, in the case of nonidentically distributed coefficients it is analytically necessary to assume that the means of coefficients are zero. In this work we study a case when the moments of the coefficients have both binomial and geometric progression elements. That is we assume 𝐸(𝑎𝑗)=𝑛𝑗𝜇𝑗+1 and var(𝑎𝑗)=𝑛𝑗𝜎2𝑗. We show how the above expected number of real zeros is dependent on values of 𝜎2 and 𝜇 in various cases.

1. Origin of Polynomials

Let (Ω,Pr,𝒜) be a fixed probability space, and for 𝜔Ω let {𝑎𝑗(𝜔)}𝑛𝑗=0 be a sequence of independent identically distributed random variables defined on Ω. There has been considerable work on obtaining the expected number of real zeros of algebraic𝑃𝑛(𝑥,𝜔)𝑃𝑛(𝑥)=𝑛𝑗=0𝑎𝑗(𝜔)𝑥𝑗,(1.1)and trigonometric 𝑛𝑗=0𝑎𝑗(𝜔)cos𝑗𝜃 polynomials with random coefficients 𝑎𝑗(𝜔)s. The study of the random algebraic polynomials was initiated by Kac [1], and the recent works include [2, 3]. It is shown that under general assumptions for the distribution of coefficients the expected number of real zeros is asymptotic to (2/𝜋)log𝑛 as 𝑛. For the case of random trigonometric polynomials, Dunnage [4] obtained the first result which was later generalized by Wilkins Jr. [5, 6] and recently studied in [7, 8]. It is shown that, again for a wide class of distributions for the coefficients, there are significantly more real zeros in the case of trigonometric polynomial compared with the algebraic case. The asymptotic value for the expected number of zeros for the latter case is 2𝑛/3. Besides the comprehensive book of Bharucha-Reid and Sambandham [9], the earlier results of general topics on random polynomials are reviewed in [10].

Motivated by the interesting work of Edelman and Kostlan [11], who, among others, considered polynomials of the form 𝑛𝑗=0𝑎𝑗(𝜔)(𝑛𝑗)1/2𝑥𝑗, [2, 12] obtained many characteristics, like the number of real zeros or the number of maxima of these types of polynomials. This is interesting as they showed that for this case of nonidentically distributed coefficients the expected number of real zeros is 𝑂(𝑛), which is significantly more than the classical algebraic case but less than that of trigonometric polynomials. Also in this direction of nonidentical coefficients, a case in which the mean of coefficients 𝑎𝑗(𝜔) increases with 𝑗 is studied in [3, 13]. Now it would be interesting to study a random polynomial formed by combining the above two distribution laws. It is natural to ask, for instance, what would be the behavior of 𝑃𝑛(𝑥) in (1.1) if for constants 𝜇 and 𝜎 the mean and variance of coefficients are 𝐸(𝑎𝑗(𝜔))=(𝑛𝑗)𝜇𝑗+1 and var(𝑎𝑗(𝜔))=(𝑛𝑗)𝜎2𝑗.

With the latter assumption of the distribution of the coefficients, we first show that if 𝜇=0, the expected number of real zeros of 𝑃𝑛(𝑥) denoted by 𝐸𝑁𝑛,𝑃(0,)𝐸𝑁𝑛(0,) is independent of 𝜎. The case of nonzero 𝜇 is studied in Theorem 1.2. The analysis for the general case is complicated, and we only give the result for a case that 𝜇=𝜎2. We prove the following theorem.

Theorem 1.1. For 𝜇=0 and 𝜎2>0, the expected number of real zeros of 𝑃𝑛(𝑥) is independent of 𝜎2. That is 𝐸𝑁𝑛(,0)=𝐸𝑁𝑛(0,)=𝑛2.(1.2)

The analysis for the case of 𝜇0 would be complicated. Without loss of much generality and certainly interest, we restrict ourselves to the case of 𝜇=𝜎2. We prove the following theorem.

Theorem 1.2. The expected number of real zeros of 𝑃𝑛(𝑥) for different values of 𝜇 satisfies 𝐸𝑁𝑛(0,)=𝑂(1),if𝜇=𝜎>1,𝑛221arctan𝜇1𝜇,if0<𝜇=𝜎<1.(1.3)For 𝑥 negative and for every 𝜇=𝜎2, 𝐸𝑁𝑛(,0)𝑛2.(1.4)

2. Moments

In order to obtain the expected number of real zeros we use a generalization of the well-known Kac-Rice formula initiated in [1, 14, 15]. To this end, we need the following moments of 𝑃𝑛(𝑥) and its dervative 𝑃𝑛(𝑥). First, we assume the general assumptions on the means and the variances of coefficients as stated above. That is, 𝐸(𝑎𝑗)=(𝑛𝑗)𝜇𝑗+1 and var(𝑎𝑗)=(𝑛𝑗)𝜎2𝑗. Since these coefficients are independent, it is easy to show𝛼=𝐸(𝑃𝑛(𝑥))=𝜇𝑛𝑗=0𝑛𝑗(𝑥𝜇)𝑗=𝜇(1+𝜇𝑥)𝑛,(2.1)𝛽=𝐸(𝑃𝑛(𝑥))=𝜇2𝑛𝑗=0𝑗𝑛𝑗(𝜇𝑥)𝑗1=𝑛𝜇2(1+𝜇𝑥)𝑛1,𝐴(2.2)2=var(𝑃𝑛(𝑥))=𝑛𝑗=0𝑛𝑗(𝜎𝑥)2𝑗=(1+𝜎2𝑥2)𝑛,𝐵(2.3)2=var(𝑃𝑛(𝑥))=𝜎2𝑛𝑗=0𝑗2𝑛𝑗(𝜎𝑥)2=𝑛𝜎2(1+𝜎2𝑥2)𝑛2(1+𝑛𝜎2𝑥2),(2.4) and finally𝐶=cov(𝑃𝑛(𝑥),𝑃𝑛(𝑥))=𝜎2𝑥𝑛𝑗=0𝑗𝑛𝑗(𝜎𝑥)2𝑗2=𝑛𝜎2𝑥(1+𝜎2𝑥2)𝑛1.(2.5) Then from (2.3)–(2.5) we can obtainΔ2=𝐴2𝐵2𝐶2=𝑛𝜎2(1+𝜎2𝑥2)2𝑛2.(2.6)With the above notations, we can now write the Kac-Rice for the expected number of real zeros of 𝑃𝑛(𝑥) in the interval (𝑎,𝑏) as, see also [10, page 43],𝐸𝑁𝑛(𝑎,𝑏)=𝐼1(𝑎,𝑏)+𝐼2(𝑎,𝑏),(2.7)where𝐼1(𝑎,𝑏)=𝑏𝑎Δ𝜋𝐴2𝛼exp2𝐵2+𝛽2𝐴22𝛼𝛽𝐶2Δ2𝐼𝑑𝑥,(2.8)2(𝑎,𝑏)=𝑏𝑎2|𝛽𝐴2𝐶𝛼|𝜋𝐴3𝛼exp22𝐴2erf|𝛽𝐴2𝐶𝛼|2𝐴Δ𝑑𝑥,(2.9) where as usual erf(𝑥)=𝑥0exp(𝑡2)𝑑𝑡. Now we can progress and evaluate further the following terms required in the Kac-Rice formulae (2.7)–(2.9). From (2.1)–(2.5) we can derive

𝛼2𝐵2+𝛽2𝐴22𝛼𝛽𝐶=𝑛𝜇2(1+𝜇𝑥)2𝑛2(1+𝜎2𝑥2)𝑛2(𝑛𝜎4𝑥2+𝜎2+2𝜇𝑥𝜎2+𝜇2𝑥2𝜎2+𝑛𝜇22𝑛𝜇𝜎2𝑥).(2.10)This together with (2.6) yields𝛼2𝐵2+𝛽2𝐴22𝛼𝛽𝐶2Δ2=𝜇2(1+𝜇𝑥)2𝑛2{𝑛(𝜎2𝑥𝜇)2+𝜎2(1+𝜇𝑥)2}2𝜎2(1+𝜎2𝑥2)𝑛.(2.11)

3. Proof of Theorems

First in the case of 𝜇=0 from (2.7) and (2.3)–(2.6) by letting 𝑦=𝜎𝑥 we can show𝐸𝑁𝑛(0,)=𝑛𝜋0𝜎1+𝜎2𝑥2=𝑑𝑥𝑛𝜋0𝑑𝑦1+𝑦2=𝑛2.(3.1)This proves Theorem 1.1. Now we proceed with the more general case of 𝜇0. As explained above, in order to simplify the analysis we let 𝜇=𝜎2. This yields (2.11) to𝛼2𝐵2+𝛽2𝐴22𝛼𝛽𝐶2Δ2=𝑓𝑛(𝑥,𝜇)𝑔𝑛(𝑥,𝜇),(3.2)where𝑔𝑛(𝑥,𝜇)=𝑛𝜇2(𝑥1)2+𝜇(1+𝜇𝑥)2,(3.3)and for all sufficiently large 𝑛,𝑓𝑛(𝑥,𝜇)=(1+𝜇𝑥)2𝑛2(1+𝜇𝑥2)𝑛(1+𝜇𝑥)2𝑛(1+𝜇𝑥2)𝑛=1+𝜇2𝑥2+2𝜇𝑥1+𝜇𝑥2𝑛.(3.4)Now we assume 𝑥>0. Then if we let 𝜇>1, since1+𝜇2𝑥2+2𝜇𝑥1+𝜇𝑥2>1,(3.5)we can see that 𝑓𝑛(𝑥,𝜇) as 𝑛. Therefore the exponential term that appears in (2.8) tends to zero exponentially fast. Hence the only contribution to 𝐸𝑁𝑛(0,) is from 𝐼2(0,). In the following, we show that the latter is 𝑂(1). To this end, we note that since from the definition for all 𝑥, erf(𝑥)𝜋/2, then𝐼21(0,)<2𝜋0𝛽𝐴2𝐶𝛼𝐴3𝛼exp22𝐴2𝑑𝑥.(3.6)Now we let 𝑢=𝛼/𝐴, and since (𝑑/𝑑𝑥)(𝛼/𝐴)=(𝛽𝐴2𝛼𝐶)/𝐴3 from (3.6) we obtain𝐼21(0,)<2𝜋0𝑢exp221𝑑𝑢2.(3.7)This completes the first part of Theorem 1.2. On the other hand, if 𝜇<1, the behavior of 𝑓𝑛(𝑥,𝜇) will depend on 𝑥. That is for 0<𝑥<2/(1𝜇), 𝑓𝑛(𝑥,𝜇) as 𝑛 and for 𝑥>2/(1𝜇), 𝑓𝑛(𝑥,𝜇)0 as 𝑛. Therefore the only contribution to 𝐸𝑁𝑛(0,) from 𝐼1 is in the interval (2/(1𝜇),) as 𝐼1(0,2/(1𝜇)) will tend to zero exponentially fast. Also for 𝜈=𝜇𝑥,𝐼121𝜇,𝑛𝜋2/(1𝜇)𝜇1+𝜇𝑥2𝑑𝑥=𝑛𝜋2/(1𝜇)𝑑𝜈1+𝜈2𝑛221arctan𝜇.1𝜇(3.8)The above argument for 𝐼2(0,) in (3.7) remains valid, and therefore we have proof of the first part of Theorem 1.2.

For 𝑥<0 without loss of generality, we only consider the case of 𝜇>0 (since 𝜇=𝜎2). For this case 𝑔𝑛(𝑥,𝜇) remains positive. However, for 𝑥2>𝜖/𝜇, where for 𝑎=1loglog𝑛10/log𝑛 we let 𝜖=𝑛𝑎, we have, (see also [10, page 31]),(1+𝜇𝑥2)𝑛>(1+𝜖)𝑛{(1+𝑛𝑎)𝑛𝑎}𝑛1𝑎=exp(𝑛1𝑎)𝑛10.(3.9)Hence𝑓𝑛(𝑥,𝜇)<(1+𝜇𝑥2)𝑛<𝑛10,(3.10)which tends to zero very fast as 𝑛. Therefore the exponential term in 𝐼1 tends to be one, and hence𝐼1𝜖𝜇,𝑛𝜋𝜖/𝜇𝑑𝑥1+𝑥2𝑛2.(3.11)Also in the interval (0,𝜖/𝜇),𝐼10,𝜖𝜇<0𝜖/𝜇Δ𝜋𝐴2𝑑𝑥<𝑛𝜇𝜋0𝜖/𝜇𝑑𝑥1+𝜇𝑥2𝑛2𝜋arctan𝜖,(3.12)which is small. This completes the proof of Theorem 1.2.