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Related Concept Videos

Metallic Solids02:37

Metallic Solids

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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....
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Structures of Solids02:22

Structures of Solids

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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...
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Network Covalent Solids02:18

Network Covalent Solids

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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.
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Molecular and Ionic Solids02:54

Molecular and Ionic Solids

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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...
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Molecular Comparison of Gases, Liquids, and Solids02:26

Molecular Comparison of Gases, Liquids, and Solids

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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...
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Energy Bands in Solids01:01

Energy Bands in Solids

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Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
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Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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First demonstration of an all-solid-state optical cryocooler.

Markus P Hehlen1,2, Junwei Meng2, Alexander R Albrecht2

  • 11Los Alamos National Laboratory, P.O. Box 1663, Los Alamos, NM 87545 USA.

Light, Science & Applications
|March 7, 2019
PubMed
Summary
This summary is machine-generated.

Solid-state optical refrigeration now cools payloads, demonstrated by cooling a HgCdTe sensor to 135 K using a Yb:YLF crystal. This breakthrough enables vibration-free, all-solid-state cryocoolers for sensitive instruments.

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Area of Science:

  • Physics
  • Materials Science
  • Optical Engineering

Background:

  • Solid-state optical refrigeration utilizes anti-Stokes fluorescence for vibration-free cooling of macroscopic objects to cryogenic temperatures.
  • Previous research demonstrated laser cooling of Yb3+-doped YLiF4 (YLF:Yb) crystals to 91 K.

Purpose of the Study:

  • To demonstrate laser cooling of a payload attached to a cooling crystal for the first time.
  • To develop an all-solid-state optical cryocooler for practical applications, such as cooling sensors in spectrometers.

Main Methods:

  • A YLF:Yb crystal was integrated into a Herriott cell and optically pumped with a 1020-nm laser (47 W).
  • A HgCdTe sensor within a Fourier Transform Infrared (FTIR) spectrometer was cooled to 135 K.
  • Heat flows were meticulously managed using a YLF thermal link and silica aerogel supports within a vacuum clamshell.

Main Results:

  • Achieved laser cooling of a connected payload (HgCdTe sensor) to 135 K.
  • Demonstrated the first all-solid-state optical cryocooler system.
  • Minimized fluorescence heating and parasitic heat loads through optimized thermal management.

Conclusions:

  • This study presents a viable method for laser cooling payloads, paving the way for advanced optical cryocoolers.
  • The developed structure provides a baseline for future optical cryocooler designs, applicable to various sensitive electronic components.
  • Effective thermal management is crucial for the success of solid-state optical refrigeration systems.