関連する実験動画
Updated: Jul 9, 2026

07:17
Non-equilibrium Microwave Plasma for Efficient High Temperature Chemistry
Published on: August 1, 2017
ハンベリー・ブラウン・トウィス効果は,超冷たい量子ガスのためのものです
M Schellekens1, R Hoppeler, A Perrin
1Laboratoire Charles Fabry de l'Institut d'Optique, UMR 8501 du CNRS, Centre Scientifique d'Orsay, Bâtiment 503, 91403 Orsay CEDEX, France.
まとめ
我々は,ハンベリー・ブラウン・ツィス効果に似た,原子のボース・アインシュタイン凝縮体における量子相関を観察した. 熱雲は粒子の束を表示し,一貫したサンプルは平らな相関を示します.
科学分野:
- 原子物理学 原子物理学とは
- 量子光学とは,量子光学である.
- 凝縮物質物理学 凝縮物質物理学
背景:
- ボーゼ・アインシュタイン凝縮 (Bose-Einstein condensation,BEC) とは,物質の量子状態である.
- 二体相関は,粒子の量子統計的性質を明らかにする.
- ハンベリー・ブラウン・トゥイス (HBT) 効果は,量子光学における光子相関を証明している.
研究 の 目的:
- BEC値に近い原子雲の2体相関を調査する.
- ハンベリー・ブラウン・トゥイス効果の原子類似性を探求する.
- 量子相関が雲の大きさと相関性に依存しているかを分析する.
主な方法:
- 膨張する原子雲をBEC値の上下に研究した.
- 三次元で測定された二体相関関数.
- 熱的および一貫した原子サンプルのための相関関数の比較.
主要な成果:
- 熱原子雲の相関関数における観察された束の挙動.
- 一貫した原子サンプルに対して平らな相関関数が見つかりました.
- ハンベリー・ブラウン・トゥイス効果の原子類似性を実証した.
結論:
- 量子相関は,熱的サンプルと一貫した原子サンプルの間に著しく異なる.
- 観測された原子相関は,HBT効果と一致しています.
- 雲の大きさは,これらの量子相関の現れに影響する.
関連する概念動画
Real Gases: Effects of Intermolecular Forces and Molecular Volume Deriving Van der Waals Equation
Thus far, the ideal gas law, PV = nRT, has been applied to a variety of different types of problems, ranging from reaction stoichiometry and empirical and molecular formula problems to determining the density and molar mass of a gas. However, the behavior of a gas is often non-ideal, meaning that the observed relationships between its pressure, volume, and temperature are not accurately described by the gas laws.
Kinetic Theory of an Ideal Gas
A mole is defined as the amount of any substance that contains as many molecules as there are atoms in exactly 12 grams of carbon-12. An Italian scientist Amedeo Avogadro (1776–1856) formed the hypothesis that equal volumes of gas at equal pressure and temperature contain equal numbers of molecules, independent of the type of gas. Later, the hypothesis was developed to form the SI unit for measuring the amount of any substance.
The number of molecules in one mole is called Avogadro's number...
The number of molecules in one mole is called Avogadro's number...
Heat Capacities of an Ideal Gas III
The number of independent ways a gas molecule can move along straight line, rotate, and vibrate is called its degrees of freedom. Supposing d represents the number of degrees of freedom of an ideal gas, the molar heat capacity at constant volume of an ideal gas in terms of d is
Joule-Thomson Effect
The Joule-Thomson effect, also known as the Joule-Kelvin effect, describes the temperature change of a fluid when it is forced through a valve or porous plug while keeping it in a thermally insulated environment. This experiment is called a throttling process. This is an important effect widely used in refrigeration and the liquefaction of gases.
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
This experiment forces high-pressure gas through a throttle valve or a porous plug to a lower-pressure region. The gas expands as it passes through to...
Atomic Spectroscopy: Effects of Temperature
Atomization, converting samples into gas-phase atoms and ions, is essential for atomic spectroscopy. The flame temperature required for atomization affects the efficiency of the atomic spectroscopic methods by increasing the atomization efficiency and the relative population of the excited and ground states.
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature from...
At thermal equilibrium, the relative populations of excited and ground state atoms can be estimated using the Maxwell–Boltzmann distribution. For example, an increase in temperature from...
The Joule and Joule–Thomson Experiments
Consider an adiabatic system composed of two chambers, A and B, designed such that no heat flows into or out of the system. Initially, chamber A is filled with a gas at a fixed temperature T1, pressure p1, and volume V1, while chamber B is evacuated. The gas is then gradually forced through a rigid, porous barrier to chamber B, ultimately reaching temperature T2, pressure p2, and volume V2. A piston on the right side maintains a constant pressure (p2), which is lower than p1. The significant...

