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High-temperature superconductivity

physical science Maturity 9-11 Next article →

High-temperature superconductivity refers to a state where certain materials conduct electricity with zero resistance at relatively high temperatures. In physics, a superconductor is a material that allows electrical current to flow without losing any energy to heat. Most traditional superconductors only function at temperatures near absolute zero. They require expensive coolants like liquid helium to maintain these extreme conditions. High-temperature superconductors, or HTS, are defined as materials with a critical temperature above the boiling point of liquid nitrogen. This threshold is significant because liquid nitrogen is much cheaper and easier to handle than liquid helium.

Meissner effect p1390048
Meissner effect p1390048

The mechanism of superconductivity involves a material reaching a specific critical temperature. Once the material drops below this temperature, it undergoes a transition into a superconducting state. Most HTS materials are classified as Type-II superconductors. Unlike Type-I superconductors, which expel all magnetic fields through the Meissner effect, Type-II materials allow magnetic fields to penetrate their interior. This penetration happens in quantized units of flux, creating tiny tubes or holes of normal metallic regions within the superconducting bulk. This unique property allows Type-II superconductors to remain functional even when exposed to very high magnetic fields.

Meissner effect p1390048
Meissner effect p1390048

Scientists categorize high-temperature superconductors into several distinct classes. The largest group consists of cuprates, which are copper oxides combined with other metals. A major sub-class of cuprates is the rare-earth barium copper oxides, known as REBCOs. An example is yttrium barium copper oxide, or YBCO, which contains yttrium, barium, copper, and oxygen. Another important class is the iron-based compounds, which were discovered in 2006. Some materials, like magnesium diboride, are sometimes included in this category. While magnesium diboride is simple to manufacture, it only superconducts below 39 K. This makes it unsuitable for liquid nitrogen cooling, which requires a higher temperature.

BI2223-piece3 001
BI2223-piece3 001

The history of this field began in 1911 when Kamerlingh Onnes discovered superconductivity in a metal solid. For decades, researchers searched for materials that worked at higher temperatures. A massive breakthrough occurred in 1986 at an IBM research lab near Zürich, Switzerland. Researchers Georg Bednorz and K. Alex Müller discovered superconductivity in a ceramic called lanthanum barium copper oxide (LBCO). This discovery showed that superconductivity could exist in ceramic materials rather than just metals. For this achievement, Bednorz and Müller were awarded the Nobel Prize in Physics in 1987.

Timeline of Superconductivity from 1900 to 2015
Timeline of Superconductivity from 1900 to 2015

Following the 1986 discovery, scientists found ways to increase the critical temperature of these ceramics. While the original LBCO had a transition temperature of 35 K, modifying the material to create YBCO raised that temperature above 90 K. Today, the mercury, barium, and calcium cuprate holds the record for the highest transition temperature at ambient pressure, reaching approximately 133 K. Other materials like lanthanum superhydride reach even higher temperatures, such as 250 K. However, these high temperatures only occur under extreme pressures of 170 gigapascals. Researchers are also exploring new frontiers, such as bilayer graphene. In 2018, scientists found superconductivity in graphene when one layer was twisted at an angle of 1.1 degrees.

Timeline of Superconductivity from 1900 to 2015
Timeline of Superconductivity from 1900 to 2015

Despite their advantages, high-temperature superconductors present significant engineering challenges. Most HTS materials are ceramics rather than metals. While ceramics are excellent for superconductivity, they are also very brittle. This brittleness makes it difficult to manufacture them into long, flexible wires for practical use. Additionally, HTS materials do not form large, continuous superconducting domains. Instead, they consist of clusters of microdomains where superconductivity occurs. This characteristic makes them less suitable for certain applications, such as magnets for magnetic resonance spectrometers, which require actual superconductive currents.

BI2223-piece3 001
BI2223-piece3 001

The significance of HTS research lies in its potential for advanced technology. One primary application is the construction of superconducting magnets. HTS materials are highly valuable here because they can retain superconductivity in much higher magnetic fields than previous materials. Some cuprates can withstand an upper critical field of about 100 tesla. This capability is essential for creating powerful magnets used in various scientific and industrial tools. As researchers continue to study the theoretical foundations, such as the resonating valence bond theory, the goal remains to find a superconductor that works at room temperature and ambient pressure.

Phase diagram of the 122 family of ferro-pnictides
Phase diagram of the 122 family of ferro-pnictides
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File:BI2223-piece3 001.jpg
BI2223-piece3 001.jpg
File:Timeline of Superconductivity from 1900 to 2015.svg
Timeline of Superconductivity from 1900...
File:Phase diagram of the 122 family of ferro-pnictides.png
Phase diagram of the 122 family of...
File:Meissner effect p1390048.jpg
Meissner effect p1390048.jpg
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