Abstract
Elephant random walk is a kind of one-dimensional discrete-time random walk with infinite memory: For each step, with probability \(\alpha \) the walker adopts one of his/her previous steps uniformly chosen at random, and otherwise he/she performs like a simple random walk (possibly with bias). It admits a phase transition from diffusive to superdiffusive behavior at the critical value \(\alpha _c=1/2\). For \(\alpha \in (\alpha _c, 1)\), there is a scaling factor \(a_n\) of order \(n^{\alpha }\) such that the position \(S_n\) of the walker at time n scaled by \(a_n\) converges to a nondegenerate random variable \({\widehat{W}}\), whose distribution is not Gaussian. Our main result shows that the fluctuation of \(S_n\) around \({\widehat{W}} \cdot a_n\) is still Gaussian. We also give a description of a phase transition induced by bias decaying polynomially in time.
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Communicated by Irene Giardina.
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Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
N.K. is partially supported by JSPS Grant-in-Aid for Young Scientists (B) No. 16K17620. M.T. is partially supported by JSPS Grant-in-Aid for Young Scientists (B) No. 16K21039, and JSPS Grant-in-Aid for Scientific Research (C) No. 19K03514.
Appendix
Appendix
1.1 Lemmas from Calculus
Lemma A1
(Schütz and Trimper [20], (12) and (13)) The general solution \(\{x_n\}\) to the recursion
is given by
Lemma A2
(see e.g. Knopp [18], p.34) If a real sequence \(\{a_n\}\) and a positive sequence \(\{b_n\}\) satisfy
then
Lemma A3
Consider a positive real sequence \(\{a_n\}\) which monotonically diverges to \(+\infty \), and another real sequence \(\{b_n\}\).
- (i)
(Kronecker’s lemma) If \(\displaystyle \sum _{k=1}^{\infty } \dfrac{b_k}{a_k}\) converges, then \(\displaystyle \lim _{n \rightarrow \infty } \dfrac{1}{a_n}\sum _{k=1}^n b_k =0\).
- (ii)
(Heyde [14], Lemma 1 (ii)) If \(\displaystyle \sum _{k=1}^{\infty } a_k b_k\) converges, then\(\displaystyle \lim _{n \rightarrow \infty } a_n\sum _{k=n}^{\infty } b_k =0\).
1.2 Martingale Limit Theorems
Theorem A1
(Hall and Heyde [15], Theorem 2.15) Suppose that \(\{M_n\}\) is a square-integrable martingale with mean 0. Let \(d_k=M_k-M_{k-1}\) for \(k=1,2,\cdots \), where \(M_0=0\). On the event
\(\{M_n\}\) converges a.s..
The following theorem is a special case of Heyde [14], Theorem 1 (b).
Theorem A2
Suppose that \(\{M_n\}\) is a square-integrable martingale with mean 0. Let \(d_k=M_k-M_{k-1}\) for \(k=1,2,\cdots \), where \(M_0=0\). If
holds in addition, then we have the following: Let \(\displaystyle s_n^2 := \sum _{k=n}^{\infty } E[ (d_k)^2]\).
- (i)
The limit \(M_{\infty }:=\sum _{k=1}^{\infty } d_k\) exists a.s., and \(M_n {\mathop {\rightarrow }\limits ^{L^2}} M_{\infty }\).
- (ii)
Assume that
- a)
\(\displaystyle \dfrac{1}{s_n^2} \sum _{k=n}^{\infty } (d_k)^2 \rightarrow 1\) as \(n \rightarrow \infty \) in probability, and
- b)
\(\displaystyle \lim _{n \rightarrow \infty } \dfrac{1}{s_n^2}E\left[ \sup _{k \ge n} (d_k)^2\right] =0\).
Then we have
$$\begin{aligned} \dfrac{M_{\infty } - M_n}{s_{n+1}} = \dfrac{ \sum _{k=n+1}^{\infty } d_k}{s_{n+1}}{\mathop {\rightarrow }\limits ^{\text {d}}} N(0,1). \end{aligned}$$ - a)
- (iii)
Assume that the following three conditions hold:
- a’)
\(\displaystyle \dfrac{1}{s_n^2} \sum _{k=n}^{\infty } (d_k)^2 \rightarrow 1\) as \(n \rightarrow \infty \) a.s.,
- c)
\(\displaystyle \sum _{k=1}^{\infty } \dfrac{1}{s_k} E[ |d_k| : |d_k| > \varepsilon s_k] < +\infty \) for any \(\varepsilon > 0\), and
- d)
\(\displaystyle \sum _{k=1}^{\infty } \dfrac{1}{s_k^4} E[ (d_k)^4 : |d_k| \le \delta s_k] < +\infty \) for some \(\delta > 0\).
Then \(\displaystyle \limsup _{n \rightarrow \infty } \pm \dfrac{M_{\infty } - M_n}{{\widehat{\phi }}(s_{n+1}^2)} =1\) a.s., where \({\widehat{\phi }}(t):=\sqrt{2t\log |\log t|}\).
- a’)
Remark A1
A sufficient condition for b) in Theorem A2 is that
for any \(\varepsilon > 0\). (See the proof of Corollary 1 in Heyde [14]).
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Kubota, N., Takei, M. Gaussian Fluctuation for Superdiffusive Elephant Random Walks. J Stat Phys 177, 1157–1171 (2019). https://doi.org/10.1007/s10955-019-02414-0
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DOI: https://doi.org/10.1007/s10955-019-02414-0