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関連する概念動画

¹H NMR Signal Multiplicity: Splitting Patterns01:13

¹H NMR Signal Multiplicity: Splitting Patterns

When protons A and X are coupled, their nuclear spin energy levels are slightly modified. This is because the energy required to excite proton A to a spin state parallel to proton X is slightly different from the energy required for it to become anti-parallel to spin X. Consequently, there are two possible excitation frequencies for A (A1 and A2), depending on the spin state of X, and vice versa. The mutual nature of coupling implies that the difference between frequencies A1 and A2, indicated...
IR Frequency Region: X–H Stretching01:24

IR Frequency Region: X–H Stretching

In IR spectroscopy, signals produced by the X−H bonds (such as C−H, O−H, or N−H) can be observed in the frequency range of  2700–4000 cm–1. The C−H stretching vibration forms sharp bands in the region 2850–3000 cm–1. The presence of the O−H stretching vibration leads to the forming of an absorption band in the frequency range 3650–3200 cm−1. At the same time, N−H stretching can be confirmed by absorption bands in the 3500–3100 cm−1 range. Even though both O−H and N−H bonds vibrate at a similar...
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences01:17

NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences

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.
Electronic Distance Measuring Instruments01:30

Electronic Distance Measuring Instruments

Electronic Distance Measuring Instruments (EDMs) are essential tools in modern surveying, offering precise distance measurements by emitting electromagnetic signals and calculating the time required for these signals to travel to a target and return. Two primary types of signals are used in EDMs — light waves and microwaves — each suited to specific environmental and distance requirements. Light-wave-based EDMs utilize either infrared or laser light, providing high accuracy over short distances...

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Updated: Jul 10, 2026

An Experimental Protocol for Femtosecond NIR/UV - XUV Pump-Probe Experiments with Free-Electron Lasers
09:49

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Published on: October 23, 2018

高調和の柔らかいX線をアット秒同期する.

Y Mairesse1, A de Bohan, L J Frasinski

  • 1Commissariat à l'Energie Atomique, DRECAM/SPAM, Centre d'Etudes de Saclay, 91191 Gif-sur-Yvette, France.

Science (New York, N.Y.)
|December 4, 2003
PubMed
まとめ

研究者は,高ハーモニクスを同期することによって,130アト秒のX線パルスを達成しました. 電子のダイナミクスを制御することで,パルス持続時間が改善され,超高速の電子プロセスの追跡が可能になりました.

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Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization
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Published on: August 6, 2018

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

関連する実験動画

Last Updated: Jul 10, 2026

An Experimental Protocol for Femtosecond NIR/UV - XUV Pump-Probe Experiments with Free-Electron Lasers
09:49

An Experimental Protocol for Femtosecond NIR/UV - XUV Pump-Probe Experiments with Free-Electron Lasers

Published on: October 23, 2018

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization
08:22

Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization

Published on: August 6, 2018

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator
07:42

Rapid Repetition Rate Fluctuation Measurement of Soliton Crystals in a Microresonator

Published on: December 15, 2021

科学分野:

  • *超高速科学とアット秒物理.
  • *高強度レーザーと物質の相互作用.

背景:

  • * 激烈なレーザーパルスの高ハーモニックを重ね合わせることは,サブフェムト秒光パルスを生成する方法です.
  • * 理論的には,ハーモニクスの同時放出により,ハーモニクスの数が増加したより短いパルスが生成されると予想されます.

研究 の 目的:

  • * アット秒の時間スケールで高相和音の同期を調査する.
  • * 達成可能なX線パルス持続の制限を克服するために.
  • *さらに短くアット秒パルスを生成する方法を模索する.

主な方法:

  • * 激烈なレーザーパルスからの高ハーモニック放射の分析.
  • * 超高速電子ダイナミクスの制御.
  • * アット秒のX線パルス持続の特徴.

主要な成果:

  • * ハイハーモニックは,アト秒のタイムスケールで非同期であることが判明し,パルス持続時間を制限しました.
  • *電子ダイナミクスを制御することで同期性が著しく改善されました.
  • *130アト秒のパルスが成功しました.

結論:

  • * 電子ダイナミクスを制御することは,超短時間のX線パルスを達成するために不可欠です.
  • *130アット秒のパルス持続が実証され,アット秒科学の限界を押し広げました.
  • *パルス持続時間をさらに短縮することで,物質の電子過程をリアルタイムで追跡することが可能になる.