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NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

1.9K
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
1.9K
¹³C NMR: ¹H–¹³C Decoupling01:04

¹³C NMR: ¹H–¹³C Decoupling

1.9K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.9K
Raman Spectroscopy Instrumentation: Overview01:26

Raman Spectroscopy Instrumentation: Overview

1.4K
A conventional Raman spectrophotometer includes a laser source, a sample holding system, a wavelength selector, and a detector.
The monochromatic laser source, typically using visible or near-infrared radiation, generates a highly focused beam of light. This light interacts with the molecules of the sample, scattering some of the light. Liquid and gaseous samples are usually tested in ordinary glass capillaries, while solids can be analyzed as powders packed in capillaries or as potassium...
1.4K
NMR Spectrometers: Overview01:20

NMR Spectrometers: Overview

2.3K
NMR spectrometers consist of a strong magnet, a radiofrequency transmitter, and a detector attached to a computer console for recording spectra of samples containing NMR-active nuclei. In first-generation NMR instruments called continuous-wave spectrometers, the resonance frequencies of the nuclei are determined by frequency-sweep or field-sweep methods. The magnetic field strength is fixed and the rf signal is swept in the former, while the radiofrequency signal is fixed and the magnetic field...
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Atomic Fluorescence Spectroscopy01:29

Atomic Fluorescence Spectroscopy

1.0K
Atomic fluorescence spectroscopy (AFS) is an analytical technique that involves the electronic transitions of atoms in a flame, furnace, or plasma being excited by electromagnetic (EM) radiation. When these atoms absorb energy, they become excited and subsequently release energy as they return to their original state. This emitted light, or "fluorescence," is observed at a right angle to the incident beam. Both absorption and emission processes transpire at distinct wavelengths, which...
1.0K
IR Spectroscopy: Molecular Vibration Overview01:24

IR Spectroscopy: Molecular Vibration Overview

4.9K
When Infrared (IR) radiation passes through a covalently bonded molecule, the bonds transition from lower to higher vibrational levels. The fundamental vibrational motions that result in infrared absorption can be classified as stretching or bending vibrations.
Stretching vibrations are vibrational motions that occur along the bond line, changing the bond length or distance between two bonded atoms. They are further distinguished as symmetric or asymmetric. In symmetric stretching, the...
4.9K

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Updated: Feb 22, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

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周波数は,高速で高解像度の多次元の一貫したスペクトロスコーピーを可能にします.

Bachana Lomsadze1, Steven T Cundiff2

  • 1Department of Physics, University of Michigan, Ann Arbor, MI 48109, USA, and JILA, University of Colorado and National Institute of Standards and Technology, Boulder, CO 80309, USA.

Science (New York, N.Y.)
|October 1, 2017
PubMed
まとめ
この要約は機械生成です。

2つのレーザー周波数で 複雑なスペクトルを測定できます この新しい多次元非線形技術は,原子混合物における同位体と拡大効果を区別し,1D方法の限界を克服します.

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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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関連する実験動画

Last Updated: Feb 22, 2026

Generation and Coherent Control of Pulsed Quantum Frequency Combs
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Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

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A Multimodal Wide-Field Fourier-Transform Raman Microscope
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A Multimodal Wide-Field Fourier-Transform Raman Microscope

Published on: December 30, 2025

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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy
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High Resolution Phonon-assisted Quasi-resonance Fluorescence Spectroscopy

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科学分野:

  • 原子スペクトル
  • 量子光学
  • レーザー物理学

背景:

  • 線形吸収スペクトロスコーピーは,二重レーザー周波数カムで高解像度を提供します.
  • 一次元のテクニックは,混合分析や分離拡大メカニズムを解決するのに苦労します.
  • 異なる同位体や拡大型のスペクトル特徴を区別することは依然として課題です.

研究 の 目的:

  • 複雑な混合物に対する 1D 線形スペクトロスコピーの限界を克服する.
  • 複数の源からのスペクトル共鳴を区分し,割り当てる方法を開発する.
  • 原子サンプルにおける不均質と均質の拡大効果を分離する.

主な方法:

  • 周波数を用いた高解像度の多次元非線形コヘランススペクトルの取得
  • ルビジアム同位体 (87Rbと85Rb) の混合物に対する実験的応用.
  • 超精細エネルギー状態の配置に基づくスペクトル特性の分析.

主要な成果:

  • 87Rbと85Rbからのドップラー拡大特征の成功区分
  • 超精細エネルギーレベルの構造に基づくスペクトル貢献の割り当て
  • 複雑なスペクトルの重複を解決する多次元非線形スペクトロスコピーの能力の実証.

結論:

  • 周波数を用いた多次元非線形コヒーレントスペクトロスコピーは,複合的なサンプルの1D線形手法に優れています.
  • この技術により,混合物のスペクトル特性を正確に区別し,割り当てることができます.
  • この方法は,原子同位体とスペクトルの拡大を分析するための強力なツールを提供します.