Hideki Tanemura
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Hideki Tanemura has a total of 14 co-authors. Here are the top co-authors by number of shared publications:
- Makoto Katori
Department of Physics Faculty of Science and Engineering Chuo University Kasuga Bunkyo-ku 112-8551 Tokyo Japan
26 shared publications - Rahul Roy
Indian Statistical Institute, New Delhi, India
10 shared publications - Hirofumi Osada
Chubu University, Kasugai, Japan
6 shared publications - Masato Takei
Yokohama National University
6 shared publications - Taro Nagao
Department of Physics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan
4 shared publications - Norio Konno
Ritsumeikan University
3 shared publications
Latest Publications
- 24 November 2025
- Published by Springer Nature in Indian Journal of Pure and Applied Mathematics
- Vol. 57 (1) , 215-233
Elephant random walk with varying memory
- 24 November 2025
- Published by Springer Nature in Indian Journal of Pure and Applied Mathematics
- Vol. 57 (1) , 215-233
Elephant random walk with varying memory
- 16 January 2025
- Published by Cambridge University Press (CUP) in Journal of Applied Probability
- Vol. 62 (3) , 997-1009
The elephant random walk in the triangular array setting
Gut and Stadmüller (2021, 2022) initiated the study of the elephant random walk with limited memory. Aguech and El Machkouri (2024) published a paper in which they discuss an extension of the results by Gut and Stadtmüller (2022) for an ‘increasing memory’ version of the elephant random walk without stops. Here we present a formal definition of the process that was hinted at by Gut and Stadtmüller. This definition is based on the triangular array setting. We give a positive answer to the open problem in Gut and Stadtmüller (2022) for the elephant random walk, possibly with stops. We also obtain the central limit theorem for the supercritical case of this model.
- 16 January 2025
- Published by Cambridge University Press (CUP) in Journal of Applied Probability
- Vol. 62 (3) , 997-1009
The elephant random walk in the triangular array setting
Gut and Stadmüller (2021, 2022) initiated the study of the elephant random walk with limited memory. Aguech and El Machkouri (2024) published a paper in which they discuss an extension of the results by Gut and Stadtmüller (2022) for an ‘increasing memory’ version of the elephant random walk without stops. Here we present a formal definition of the process that was hinted at by Gut and Stadtmüller. This definition is based on the triangular array setting. We give a positive answer to the open problem in Gut and Stadtmüller (2022) for the elephant random walk, possibly with stops. We also obtain the central limit theorem for the supercritical case of this model.
- Open Access
- 13 December 2024
- Published by Springer Nature in Stochastics and Partial Differential Equations: Analysis and Computations
- Vol. 13 (2) , 770-886
Infinite-dimensional stochastic differential equations arising from Airy random point fields
- 13 December 2024
- Published by Springer Nature in Stochastics and Partial Differential Equations: Analysis and Computations
- Vol. 13 (2) , 770-886
Open AccessInfinite-dimensional stochastic differential equations arising from Airy random point fields
- 6 December 2024
- Published by Springer Nature in Journal of Mathematical Biology
- Vol. 90 (1) , 1-27
On a model of evolution of subspecies
Ben-Ari and Schinazi (J Stat Phys 162:415–425, 2016) introduced a stochastic model to study ‘virus-like evolving population with high mutation rate’. This model is a birth and death model with an individual at birth being either a mutant with a random fitness parameter in [0, 1] or having one of the existing fitness parameters with uniform probability; whereas a death event removes the entire population of the least fitness. We change this to incorporate the notion of ‘survival of the fittest’, by requiring that a non-mutant individual, at birth, has a fitness according to a preferential attachment mechanism, i.e., it has a fitness f with a probability proportional to the size of the population of fitness f. Also death just removes one individual with the least fitness. This preferential attachment rule leads to a power law behaviour in the asymptotics, unlike the exponential behaviour obtained by Ben-Ari and Schinazi (J Stat Phys 162:415–425, 2016).
- 6 December 2024
- Published by Springer Nature in Journal of Mathematical Biology
- Vol. 90 (1) , 1-27
On a model of evolution of subspecies
Ben-Ari and Schinazi (J Stat Phys 162:415–425, 2016) introduced a stochastic model to study ‘virus-like evolving population with high mutation rate’. This model is a birth and death model with an individual at birth being either a mutant with a random fitness parameter in [0, 1] or having one of the existing fitness parameters with uniform probability; whereas a death event removes the entire population of the least fitness. We change this to incorporate the notion of ‘survival of the fittest’, by requiring that a non-mutant individual, at birth, has a fitness according to a preferential attachment mechanism, i.e., it has a fitness f with a probability proportional to the size of the population of fitness f. Also death just removes one individual with the least fitness. This preferential attachment rule leads to a power law behaviour in the asymptotics, unlike the exponential behaviour obtained by Ben-Ari and Schinazi (J Stat Phys 162:415–425, 2016).
- Open AccessHow often can two independent elephant random walks on $\mathbb{Z}$ meet?We show that two independent elephant random walks on the integer lattice $\mathbb{Z}$ meet each other finitely often or infinitely often depends on whether the memory parameter $p$ is strictly larger than $3/4$ or not. Asymptotic results for the distance between them are also obtained.Open AccessHow often can two independent elephant random walks on $\mathbb{Z}$ meet?We show that two independent elephant random walks on the integer lattice $\mathbb{Z}$ meet each other finitely often or infinitely often depends on whether the memory parameter $p$ is strictly larger than $3/4$ or not. Asymptotic results for the distance between them are also obtained.
- Open Access
The elephant random walk in the triangular array setting
Gut and Stadmüller (2021, 2022) initiated the study of the elephant random walk with limited memory. Aguech and El Machkouri (2024) published a paper in which they discuss an extension of results by Gut and Stadtmüller (2022) for an "increasing memory" version of the elephant random walk without stops. Here we present a formal definition of the process which has been hinted at Eq. (2.2) in Gut and Stadtmüller (2022). This definition is based on the triangular array setting. We give a positive answer to the open problem in Gut and Stadtmüller (2022) for the elephant random walk, possibly with stops. We also obtain the CLT for the supercritical case of this model.
Open AccessThe elephant random walk in the triangular array setting
Gut and Stadmüller (2021, 2022) initiated the study of the elephant random walk with limited memory. Aguech and El Machkouri (2024) published a paper in which they discuss an extension of results by Gut and Stadtmüller (2022) for an "increasing memory" version of the elephant random walk without stops. Here we present a formal definition of the process which has been hinted at Eq. (2.2) in Gut and Stadtmüller (2022). This definition is based on the triangular array setting. We give a positive answer to the open problem in Gut and Stadtmüller (2022) for the elephant random walk, possibly with stops. We also obtain the CLT for the supercritical case of this model.
- Open Access
Phase transitions for a unidirectional elephant random walk with a power law memory
For the standard elephant random walk, Laulin (2022) studied the case when the increment of the random walk is not uniformly distributed over the past history instead has a power law distribution. We study such a problem for the unidirectional elephant random walk introduced by Harbola, Kumar and Lindenberg (2014). Depending on the memory parameter $p$ and the power law exponent $β$, we obtain three distinct phases in one such phase the elephant travels only a finite distance almost surely, and the other two phases are distinguished by the speed at which the elephant travels.Open AccessPhase transitions for a unidirectional elephant random walk with a power law memory
For the standard elephant random walk, Laulin (2022) studied the case when the increment of the random walk is not uniformly distributed over the past history instead has a power law distribution. We study such a problem for the unidirectional elephant random walk introduced by Harbola, Kumar and Lindenberg (2014). Depending on the memory parameter $p$ and the power law exponent $β$, we obtain three distinct phases in one such phase the elephant travels only a finite distance almost surely, and the other two phases are distinguished by the speed at which the elephant travels. - Open Access
- 1 January 2024
- Published by Institute of Mathematical Statistics in Electronic Communications in Probability
- Vol. 29 (none) , 1-12
Phase transitions for a unidirectional elephant random walk with a power law memory
For the standard elephant random walk, Laulin (2022) studied the case when the increment of the random walk is not uniformly distributed over the past history instead has a power law distribution. We study such a problem for the unidirectional elephant random walk introduced by Harbola, Kumar and Lindenberg (2014). Depending on the memory parameter p and the power law exponent β, we obtain three distinct phases in one such phase the elephant travels only a finite distance almost surely, in the other phase there is a positive probability that the elephant travels an infinite distance and in the third phase the elephant travels an infinite distance with probability 1. For the critical case of the transition from the first phase to the second phase, the proof of our result requires coupling with a multi-type branching process.
- 1 January 2024
- Published by Institute of Mathematical Statistics in Electronic Communications in Probability
- Vol. 29 (none) , 1-12
Open AccessPhase transitions for a unidirectional elephant random walk with a power law memory
For the standard elephant random walk, Laulin (2022) studied the case when the increment of the random walk is not uniformly distributed over the past history instead has a power law distribution. We study such a problem for the unidirectional elephant random walk introduced by Harbola, Kumar and Lindenberg (2014). Depending on the memory parameter p and the power law exponent β, we obtain three distinct phases in one such phase the elephant travels only a finite distance almost surely, in the other phase there is a positive probability that the elephant travels an infinite distance and in the third phase the elephant travels an infinite distance with probability 1. For the critical case of the transition from the first phase to the second phase, the proof of our result requires coupling with a multi-type branching process.
- 3 September 2022
- Published by Springer Nature
- p. 511-533
Infinite Particle Systems with Hard-Core and Long-Range Interaction
- 3 September 2022
- Published by Springer Nature
- p. 511-533
Infinite Particle Systems with Hard-Core and Long-Range Interaction
- Open Access
Infinite-dimensional stochastic differential equations and tail $ σ$-fields II: the IFC condition
In a previous report, the second and third authors gave general theorems for unique strong solutions of infinite-dimensional stochastic differential equations (ISDEs) describing the dynamics of infinitely many interacting Brownian particles. One of the critical assumptions is the \lq\lq IFC" condition. The IFC condition requires that, for a given weak solution, the scheme consisting of the finite-dimensional stochastic differential equations (SDEs) related to the ISDEs exists. Furthermore, the IFC condition implies that each finite-dimensional SDE has unique strong solutions. Unlike other assumptions, the IFC condition is challenging to verify, and so the previous report only verified solution for solutions given by quasi-regular Dirichlet forms. In the present paper, we provide a sufficient condition for the IFC requirement in more general situations. In particular, we prove the IFC condition without assuming the quasi-regularity or symmetry of the associated Dirichlet forms. As an application of the theoretical formulation, the results derived in this paper are used to prove the uniqueness of Dirichlet forms and the dynamical universality of random matrices.
Open AccessInfinite-dimensional stochastic differential equations and tail $ σ$-fields II: the IFC condition
In a previous report, the second and third authors gave general theorems for unique strong solutions of infinite-dimensional stochastic differential equations (ISDEs) describing the dynamics of infinitely many interacting Brownian particles. One of the critical assumptions is the \lq\lq IFC" condition. The IFC condition requires that, for a given weak solution, the scheme consisting of the finite-dimensional stochastic differential equations (SDEs) related to the ISDEs exists. Furthermore, the IFC condition implies that each finite-dimensional SDE has unique strong solutions. Unlike other assumptions, the IFC condition is challenging to verify, and so the previous report only verified solution for solutions given by quasi-regular Dirichlet forms. In the present paper, we provide a sufficient condition for the IFC requirement in more general situations. In particular, we prove the IFC condition without assuming the quasi-regularity or symmetry of the associated Dirichlet forms. As an application of the theoretical formulation, the results derived in this paper are used to prove the uniqueness of Dirichlet forms and the dynamical universality of random matrices.