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関連する概念動画

Radioactive Decay and Radiometric Dating02:48

Radioactive Decay and Radiometric Dating

Radioactivity is a spontaneous disintegration of an unstable nuclide and is a random process, as all the nuclei in the sample do not decay simultaneously. The number of disintegrations per unit time is called the activity (A), which is directly proportional to the number of nuclei in the sample. The decay constant (λ) is an average probability of decay per nucleus in unit time.
Mass Analyzers: Common Types01:19

Mass Analyzers: Common Types

The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
Van de Graaff Generator01:15

Van de Graaff Generator

Van de Graaff generators (or Van de Graaffs) are devices used to demonstrate high voltage due to static electricity that can also be used for research. Robert Van de Graaff first built one in 1931 (based on original suggestions by Lord Kelvin) for use in nuclear physics research.
Van de Graaff uses both smooth and pointed surfaces, conductors, and insulators to generate large static charges and, hence, large voltages. A substantial excess charge can be deposited on the sphere because it moves...
Electron Behavior00:54

Electron Behavior

Electrons are negatively charged subatomic particles that are attracted to an orbit around the positively-charged nucleus of an atom. They reside in locations that are associated with energy levels called shells and are further organized into sub-shells and orbitals within each shell.Electrons Orbit the NucleusElectrons are found in specific locations outside of the nucleus. The shell in which an electron resides indicates the general energy level of the electron: those closer to the nucleus...
Electron Behavior01:09

Electron Behavior

Electrons are negatively charged subatomic particles attracted to and orbit around the positively-charged nucleus of an atom. They reside in spaces associated with energy levels called shells and are further organized into subshells and orbitals within each shell.
Electrons Orbit the Nucleus
Electrons are found in specific locations outside of the nucleus. The shell in which an electron resides indicates the general energy level of the electron: those closer to the nucleus have less energy,...
Double Resonance Techniques: Overview01:12

Double Resonance Techniques: Overview

Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...

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関連する実験動画

Updated: Jul 11, 2026

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
10:42

Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh

Published on: May 3, 2019

静電加速器を用いた放射性炭素年代測定:マイナスのイオンが鍵となる.

C L Bennett, R P Beukens, M R Clover

    Science (New York, N.Y.)
    |November 4, 1977
    PubMed
    まとめ

    マススペクトロメトリーにより,炭素14 (14C) 年代測定比率がより正確に測定できます. 負イオンとタンデム加速器を使用すると,窒素-14 (14N) の干渉がなくなり,14Cの正確な検出が可能になります.

    科学分野:

    • ジオクロノロジー (Geochronology) について
    • アナリティカル・ケミストリー (Analytical Chemistry) とは
    • 物理 物理学 物理学とは

    背景:

    • マススペクトロメトリーは,放射性炭素年代測定のための炭素14 (14C) から炭素12 (12C) の比率を決定するための提案された方法である.
    • この方法における重要な課題は,窒素-14 (14N) と14Cを区別することです.

    研究 の 目的:

    • 放射性炭素年代測定のための質量スペクトロメトリック測定で14Nと14Cを区別する課題を克服するために.
    • 正確な14C/12C比測定のために負イオンとタンデム静電加速器の使用の有効性を実証する.

    主な方法:

    • 質量スペクトロメトリーセットアップで負イオンを使用する.
    • 離子操作と検出を強化するために,タンデム静電加速器を使用します.
    • 14C/12Cの比率を高精度で測定する.

    主要な成果:

    • 負イオンの使用は,14Nの背景を効果的に排除します.
    • タンドームの静電加速器は,最小の14C濃度の検出を容易にする.
    • 12Cの1016個の原子に対して14Cの原子が3個未満で測定され,高い感度と精度を示した.

    さらに関連する動画

    Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
    06:53

    Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

    Published on: July 27, 2018

    関連する実験動画

    Last Updated: Jul 11, 2026

    Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
    10:42

    Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh

    Published on: May 3, 2019

    Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−
    06:53

    Photoelectron Imaging of Anions Illustrated by 310 Nm Detachment of F−

    Published on: July 27, 2018

    結論:

    • 開発された質量スペクトロメトリック法では,負イオンとタンデム電静加速器を用いて,14Cと14Nを成功裏に区別する.
    • この技術は,14C/12C比率の正確な測定を可能にするため,放射性炭素年代測定の精度と感度を大幅に改善します.