arXiv subjects

Mitsuru Yamagiwa

Publications and source records attributed to Mitsuru Yamagiwa.

6 recordsLinked to original sources

arXiv2019

Partial Pressures in Liquid Mixtures and Osmotic Pressures

We have shown in this investigation that the partial pressure can be defined uniquely as each wall pressure exerted by a component in liquid mixtures, and is an important observable physical quantity. As a consequence of this definition, the law of partial pressures is applicable to liquid mixtures with strong interactions. Furthermore, it has been shown here that the gas-liquid phase equilibrium in mixtures is established by the balance of each partial-pressure for every component between the two phases. Hence, for a dilute solution Henry's law, Raoult's law and van't Hoff's law can be derived on the basis of the concept of partial pressure.

cond-mat.stat-mech↗

arXiv2009

Control of energy distribution of the proton beam with an oblique incidence of the laser pulse

We investigate proton acceleration by a laser pulse obliquely incident on a double layer target via 3D PIC simulations. It is found that the proton beam energy spread changes by the laser irradiation position and it reaches a minimum at certain position. This provides a way to control the proton energy spectrum. We show that by appropriately adjusting the size and position of the second proton layer that high energy protons with much smaller energy spread can be obtained.

physics.plasm-ph↗

arXiv2008

Radiotherapy using a laser proton accelerator

Laser acceleration promises innovation in particle beam therapy of cancer where an ultra-compact accelerator system for cancer beam therapy can become affordable to a broad range of patients. This is not feasible without the introduction of a technology that is radically different from the conventional accelerator-based approach. The laser acceleration method provides many enhanced capabilities for the radiation oncologist. It reduces the overall system size and weight by more than one order of magnitude. The characteristics of the particle beams (protons) make them suitable for a class of therapy that might not be possible with the conventional accelerator, such as the ease for changing pulse intensity, the focus spread, the pinpointedness, and the dose delivery in general. A compact, uncluttered system allows a PET device to be located in the vicinity of the patient in concert with the compact gantry. The radiation oncologist may be able to irradiate a localized tumor by scanning with a pencil-like particle beam while ascertaining the actual dosage in the patient with an improved in-beam PET verification of auto-radioactivation induced by the beam therapy. This should yield an unprecedented flexibility in the feedback radiotherapy by the radiation oncologist. Laser accelerated radiotherapy has a unique niche in a current world of high energy accelerator using synchrotron or cyclotron.

physics.med-ph↗

arXiv2007

Electron and nuclear pressures in electron-nucleus mixtures

It is shown for an electron-nucleus mixture that the electron and nuclear pressures are defined clearly and simply by the virial theorem; the total pressure of this system is a sum of these two pressures. The electron pressure is different from the conventional electron pressure being expressed as the sum of two times of kinetic energy and the potential energy in that the nuclear virial term is subtracted; this fact is exemplified by several kinds of definitions for the electron pressure enumerated in this work. The conventional definition of the electron pressure in terms of the nuclear virial term is shown inappropriate. Similar remarks are made about the definition of the stress tensor in this mixture. It is also demonstrated that both of the electron and nuclear pressures become zero at the same time for a metal in the vacuum, in contrast to the conventional viewpoint that the zero pressure is realized by a result of the cancellation between the electron and nuclear pressures, each of which is not zero. On the basis of these facts, a simple equation of states for liquid metals is derived, and examined numerically for liquid alkaline metals by use of the quantum hypernetted chain equation and the Ashcroft model potential.

cond-mat.stat-mech↗

arXiv2003

Thermodynamics in Density-Functional Theory and Force Theorems

The density-functional (DF) theory provides a simple method for calculating the properties of an interacting system under an external potential by associating it with a corresponding non-interacting system. Here, we find some relations in this non-interacting system, which can enable us to set up the thermodynamical relations for a neutral electron-nucleus mixture in terms of quantities of the non-interacting system and the exchange-correlation effect. In this way, Andersen's force theorems are clearly described and easily proved in conjunction with other types of force theorems, Janak's theorem extended to a finite-temperature system, pressure formulas and some thermodynamical relations. For this purpose, the thermodynamics in the DF theory is presented in a systematic and explicit way.

physics.chem-ph↗

arXiv2001

Pressure formulas for liquid metals and plasmas based on the density-functional theory

At first, pressure formulas for the electrons under the external potential produced by fixed nuclei are derived both in the surface integral and volume integral forms concerning an arbitrary volume chosen in the system; the surface integral form is described by a pressure tensor consisting of a sum of the kinetic and exchange-correlation parts in the density-functional theory, and the volume integral form represents the virial theorem with subtraction of the nuclear virial. Secondly on the basis of these formulas, the thermodynamical pressure of liquid metals and plasmas is represented in the forms of the surface integral and the volume integral including the nuclear contribution. From these results, we obtain a virial pressure formula for liquid metals, which is more accurate and simpler than the standard representation. From the view point of our formulation, some comments are made on pressure formulas derived previously and on a definition of pressure widely used.

cond-mat.mtrl-sci↗