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Related Concept Videos

Atomic Absorption Spectroscopy: Atomization Methods01:25

Atomic Absorption Spectroscopy: Atomization Methods

Atomic Absorption Spectroscopy (AAS) atomizes samples through flame atomization or electrothermal atomization. Flame atomization typically involves a nebulizer and spray chamber assembly to combine the sample with a fuel–oxidant mixture, creating a fine aerosol mist that enters a burner. Typically, the fuel and oxidant are combined in an approximately stoichiometric ratio. However, for atoms that are easily oxidized, a fuel-rich mixture may be more advantageous. Only about 5% of the aerosol...
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.
Atomic Nuclei: Larmor Precession Frequency01:11

Atomic Nuclei: Larmor Precession Frequency

The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession, and the angular frequency...
Atomic Absorption Spectroscopy: Radiation and Light Sources01:13

Atomic Absorption Spectroscopy: Radiation and Light Sources

Atomic absorption spectroscopy (AAS) relies on the Beer-Lambert law, which requires that the radiation source emits a narrow range of wavelengths to match the absorption characteristics of the analyte atom. The primary criteria for choosing an appropriate radiation source in AAS is to provide a precise and intense emission at specific wavelengths that will allow accurate detection of the analyte.
Two common narrow-range 'line' sources used in AAS are hollow-cathode lamps (HCLs) and...
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 Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...

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Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
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Waveguide atom beam splitter for laser-cooled neutral atoms.

D Müller, E A Cornell, M Prevedelli

    Optics Letters
    |December 11, 2007
    PubMed
    Summary

    Researchers developed a magnetic-field potential to split laser-cooled neutral atom beams. This novel approach enables precise control and a 50/50 splitting ratio for atom beam manipulation.

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    Area of Science:

    • Atomic Physics
    • Quantum Control
    • Nanofabrication

    Background:

    • Laser-cooled neutral atom beams are crucial for quantum technologies.
    • Precise manipulation of atom beams is essential for advanced applications.
    • Existing beam-splitting methods often lack efficiency or scalability.

    Purpose of the Study:

    • To demonstrate a novel magnetic-field potential for splitting neutral atom beams.
    • To achieve efficient and controllable beam splitting with a 50/50 ratio.
    • To integrate beam guiding and splitting within a compact device.

    Main Methods:

    • Utilized a low-velocity intense source of laser-cooled neutral atoms.
    • Generated a multimode beam-splitter potential using current-carrying wires on a glass substrate.
    • Applied an external transverse bias field to shape the magnetic potential.
    • Guided atoms through curves and a beam-splitter region within a 10-cm guide.

    Main Results:

    • Achieved a maximum integrated flux of 1.5x10^5 atoms/s.
    • Employed a current density of 5x10^4 A/cm^2 in 100-microm-diameter wires.
    • Demonstrated the ability to split the initial atom beam into two beams.
    • Obtained a precise 50/50 splitting ratio.

    Conclusions:

    • The developed magnetic-field potential effectively splits laser-cooled neutral atom beams.
    • This technique offers a scalable and controllable method for atom beam manipulation.
    • The integrated guiding and splitting system shows promise for future quantum devices.