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Metallic Solids02:37

Metallic Solids

20.7K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
20.7K
Structures of Solids02:22

Structures of Solids

17.8K
Solids in which the atoms, ions, or molecules are arranged in a definite repeating pattern are known as crystalline solids. Metals and ionic compounds typically form ordered, crystalline solids. A crystalline solid has a precise melting temperature because each atom or molecule of the same type is held in place with the same forces or energy. Amorphous solids or non-crystalline solids (or, sometimes, glasses) which lack an ordered internal structure and are randomly arranged. Substances that...
17.8K
IR Spectrum Peak Broadening: Hydrogen Bonding01:23

IR Spectrum Peak Broadening: Hydrogen Bonding

1.8K
The vibrational frequency of a bond is directly proportional to its bond strength. As a result, stronger bonds vibrate at higher frequencies, while weaker bonds vibrate at lower frequencies. The stretching vibration of the strong O–H bond in alcohols and phenols (very dilute solution or gas phase) appears as a sharp peak at 3600–3650 cm−1.
However, the extent of hydrogen bonding influences the observed stretching frequency and band broadening. Intermolecular or intramolecular...
1.8K
Network Covalent Solids02:18

Network Covalent Solids

16.2K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
16.2K
Molecular and Ionic Solids02:54

Molecular and Ionic Solids

20.1K
Crystalline solids are divided into four types: molecular, ionic, metallic, and covalent network based on the type of constituent units and their interparticle interactions.
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
20.1K
Molecular Comparison of Gases, Liquids, and Solids02:26

Molecular Comparison of Gases, Liquids, and Solids

55.2K
Particles in a solid are tightly packed together (fixed shape) and often arranged in a regular pattern; in a liquid, they are close together with no regular arrangement (no fixed shape); in a gas, they are far apart with no regular arrangement (no fixed shape). Particles in a solid vibrate about fixed positions (cannot flow) and do not generally move in relation to one another; in a liquid, they move past each other (can flow) but remain in essentially constant contact; in a gas, they move...
55.2K

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Related Experiment Video

Updated: Feb 4, 2026

Analysis of Cell Suspensions Isolated from Solid Tissues by Spectral Flow Cytometry
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Analysis of Cell Suspensions Isolated from Solid Tissues by Spectral Flow Cytometry

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All-solid-state multipass spectral broadening to sub-20  fs.

Kilian Fritsch, Markus Poetzlberger, Vladimir Pervak

    Optics Letters
    |October 2, 2018
    PubMed
    Summary
    This summary is machine-generated.

    We developed a new method for spectral broadening and pulse compression using nonlinear optics in a multipass cell. This technique achieves high efficiency and ultrashort 18 fs pulses, enabling compact high-power laser drivers.

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    Area of Science:

    • Nonlinear Optics
    • Ultrafast Lasers
    • Laser Engineering

    Background:

    • Ultrashort pulse generation is crucial for advanced scientific applications.
    • Existing methods for spectral broadening and pulse compression face limitations in efficiency and scalability.
    • Compact, high-power laser sources are needed for fields like XUV frequency combs.

    Purpose of the Study:

    • To present a novel nonlinear spectral broadening and compression scheme.
    • To demonstrate high efficiency and excellent beam quality in the process.
    • To enable compact, high-power laser drivers for nonlinear optics and frequency combs.

    Main Methods:

    • Utilized self-phase modulation in bulk media.
    • Employed a Herriott-type multipass cell for enhanced nonlinear interaction.
    • Investigated performance at an average input power of 100 W.

    Main Results:

    • Achieved a spectral broadening factor of 22.
    • Maintained an optical conversion efficiency exceeding 60%.
    • Compressed output pulses to 18 fs, with a spectrum supporting a 10 fs Fourier-transform limit.
    • Obtained excellent beam quality with M²=1.2.

    Conclusions:

    • The developed scheme offers a reliable and efficient method for spectral broadening and pulse compression.
    • The achieved results represent a significant advancement towards compact, high-power laser systems.
    • This work paves the way for improved drivers for XUV frequency combs and other nonlinear processes.