Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Nuclear Stability03:18

Nuclear Stability

Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together in the...
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.
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Atomic Nuclei: Types of Nuclear Relaxation01:28

Atomic Nuclei: Types of Nuclear Relaxation

Nuclear relaxation restores the equilibrium population imbalance and can occur via spin–lattice or spin–spin mechanisms, which are first-order exponential decay processes.
In spin–lattice or longitudinal relaxation, the excited spins exchange energy with the surrounding lattice as they return to the lower energy level. Among several mechanisms that contribute to spin–lattice relaxation, magnetic dipolar interactions are significant. Here, the excited nucleus transfers energy to a nearby...
Atomic Absorption Spectroscopy: Instrumentation01:22

Atomic Absorption Spectroscopy: Instrumentation

An atomic absorption spectrophotometer (AAS) comprises several components: a radiation source, an atomizer, a monochromator, and a detector. The radiation source can be a hollow-cathode lamp (HCL) or an electrodeless-discharge lamp (EDL), both of which provide a narrow emission line of the required wavelength. However, some instruments use continuum sources and high-resolution monochromators to achieve a narrow range of radiation.
The atomizer used in AAS can be either a flame atomizer or an...
Atomic Emission Spectroscopy: Instrumentation01:22

Atomic Emission Spectroscopy: Instrumentation

The instrumentation of atomic emission spectrometry (AES) involves various components, including atomization devices that convert samples into gas-phase atoms and ions. There are two main types of atomization devices: continuous and discrete atomizers.  Continuous atomizers, like plasmas and flames, introduce samples in a constant stream, while discrete atomizers inject individual samples using syringes or autosamplers. The most common discrete atomizer is the electrothermal atomizer.

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

A precision apparatus for high harmonic spectroscopy in bulk solids.

The Review of scientific instruments·2026
Same author

One-stage hollow-core fiber-based compression of Yb:KGW lasers to the single-cycle regime.

Optics letters·2025
Same author

Carrier-envelope-phase-independent field sampling of single-cycle transients using homochromatic attosecond streaking.

Optics letters·2025
Same author

Standardized Electric-Field-Resolved Molecular Fingerprinting.

Analytical chemistry·2024
Same author

Petahertz-scale spectral broadening and few-cycle compression of Yb:KGW laser pulses in a pressurized, gas-filled hollow-core fiber.

Optics letters·2023
Same author

Attosecond field emission.

Nature·2023
Same journal

Daily briefing: 'Cyborg' cockroaches breathe underwater with printed suit.

Nature·2026
Same journal

China boosts prestigious grants for young scientists - will it ease competition?

Nature·2026
Same journal

Incoming US science academy chief vows to 'double down' on research.

Nature·2026
Same journal

Author Correction: Synthesis of enantioenriched atropisomers by biocatalytic deracemization.

Nature·2026
Same journal

Electrodeposited self-assembled molecules for perovskite photovoltaics.

Nature·2026
Same journal

Neutrino's nursery found: the 'Shadow Blaster'.

Nature·2026
See all related articles

Related Experiment Video

Updated: May 26, 2026

A Basic Positron Emission Tomography System Constructed to Locate a Radioactive Source in a Bi-dimensional Space
14:19

A Basic Positron Emission Tomography System Constructed to Locate a Radioactive Source in a Bi-dimensional Space

Published on: February 1, 2016

Atomic transient recorder.

R Kienberger1, E Goulielmakis, M Uiberacker

  • 1Institut für Photonik, Technische Universität Wien, Gusshausstrasse 27, A-1040 Wien, Austria.

Nature
|February 27, 2004
PubMed
Summary
This summary is machine-generated.

Researchers generated and measured single 250-attosecond extreme ultraviolet (XUV) pulses to record atomic electron dynamics. This breakthrough allows real-time observation of electron motion within atoms, crucial for understanding atomic processes.

More Related Videos

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

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

Related Experiment Videos

Last Updated: May 26, 2026

A Basic Positron Emission Tomography System Constructed to Locate a Radioactive Source in a Bi-dimensional Space
14:19

A Basic Positron Emission Tomography System Constructed to Locate a Radioactive Source in a Bi-dimensional Space

Published on: February 1, 2016

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics

Published on: January 19, 2018

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

Area of Science:

  • Atomic Physics
  • Quantum Mechanics
  • Ultrafast Science

Background:

  • The electron's orbital motion in the hydrogen atom defines the attosecond (as = 10^-18 s) timescale for atomic dynamics.
  • Real-time recording of atomic transients necessitates excitation and probing on this attosecond scale.
  • Advances in generating sub-femtosecond (fs = 10^-15 s) extreme ultraviolet (XUV) pulses enable exploration of the attosecond regime.

Purpose of the Study:

  • To demonstrate the generation and measurement of single 250-attosecond XUV pulses.
  • To utilize these pulses for exciting atoms and probing the dynamics of ejected electrons.
  • To develop a transient recorder capable of resolving atomic electron dynamics within the Bohr orbit time.

Main Methods:

  • Generation and measurement of single 250-attosecond XUV pulses.
  • Excitation of atoms using these attosecond XUV pulses.
  • Employing intense, waveform-controlled, few-cycle laser pulses to obtain tomographic images of electron time-momentum distributions.

Main Results:

  • Successful generation and measurement of single 250-attosecond XUV pulses.
  • Tomographic imaging of primary photoelectrons provided accurate information on the excitation pulse's duration and frequency sweep.
  • Tomographic imaging of secondary Auger electrons offered insights into electronic shell relaxation dynamics.

Conclusions:

  • The developed transient recorder, using ~750-nm laser probes and ~100-eV excitation, can resolve atomic electron dynamics on the attosecond timescale.
  • This technique opens new avenues for studying ultrafast electron dynamics in atoms.
  • The ability to probe electron motion in real-time advances our understanding of fundamental atomic processes.