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Taichi Inoue

Publications and source records attributed to Taichi Inoue.

4 recordsLinked to original sources

Hasse-Arf property and abelian extensions for local fields with imperfect residue fields

For a finite totally ramified extension $L$ of a complete discrete valuation field $K$ with the perfect residue field of characteristic $p>0$, it is known that $L/K$ is an abelian extension if the upper ramification breaks are integers and if the wild inertia group is abelian. We prove a similar result without the assumption that the residue field is perfect. As an application, we prove a converse to the Hasse-Arf theorem for a complete discrete valuation field with the imperfect residue field. More precisely, for a complete discrete valuation field $K$ with the residue field $\overline{K}$ of residue characteristic $p>2$ and a finite non-abelian Galois extension $L/K$ such that the Galois group of $L/K$ is equal to the inertia group $I$ of $L/K$, we construct a complete discrete valuation field $K'$ with the residue field $\overline{K}$ and a finite Galois extension $L'/K'$ which has at least one non-integral upper ramification break and whose Galois group and inertia group are isomorphic to $I$.

math.NT

Computational Power of a Single Oblivious Mobile Agent in Two-Edge-Connected Graphs

We investigated the computational power of a single mobile agent in an $n$-node graph with storage (i.e., node memory). Generally, a system with one-bit agent memory and $O(1)$-bit storage is as powerful as that with $O(n)$-bit agent memory and $O(1)$-bit storage. Thus, we focus on the difference between one-bit memory and oblivious (i.e., zero-bit memory) agents. Although their computational powers are not equivalent, all the known results exhibiting such a difference rely on the fact that oblivious agents cannot transfer any information from one side to the other across the bridge edge. Hence, our main question is as follows: Are the computational powers of one-bit memory and oblivious agents equivalent in 2-edge-connected graphs or not? The main contribution of this study is to answer this question under the relaxed assumption that each node has $O(\log\Delta)$-bit storage (where $\Delta$ is the maximum degree of the graph). We present an algorithm for simulating any algorithm for a single one-bit memory agent using an oblivious agent with $O(n^2)$-time overhead per round. Our results imply that the topological structure of graphs differentiating the computational powers of oblivious and non-oblivious agents is completely characterized by the existence of bridge edges.

cs.DS

Tuning of temperature dependence of resonance frequency shift of atomically thin mechanical resonators with van der Waals heterojunction

Atomically thin 2-dimensional (2D) mechanical resonators are expected to be highly sensitive force sensor and high performance nano-electro-mechanical systems because of their excellent electrical and mechanical properties. For practical application, the stability of their resonance frequencies against the temperature is very crucial. Here, we demonstrate the manipulation of thermal expansion coefficients (TECs) by making van der Waals heterojunction, graphene and MoS2, which have opposite signs of TECs. The apparent TEC of the 2D heterojunction is greatly suppressed to 1/3 of monolayer graphene without the limitation of tunability of the resonance frequency by application of electrostatic attraction.

physics.app-ph

Resonance control of graphene drum resonator in nonlinear regime by standing wave of light

We demonstrate the control of resonance characteristics of a drum type graphene mechanical resonator in nonlinear oscillation regime by the photothermal effect, which is induced by a standing wave of light between a graphene and a substrate. Unlike the conventional Duffing type nonlinearity, the resonance characteristics in nonlinear oscillation regime is modulated by the standing wave of light despite a small variation amplitude. From numerical calculations with a combination of equations of heat and motion with Duffing type nonlinearity, this can be explained that the photothermal effect causes delayed modulation of stress or tension of the graphene.

physics.app-ph