Single crystal

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Crystallization
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Fundamentals
Concepts
Methods and technology

In materials science, a single crystal (or single-crystal solid or monocrystalline solid) is a material in which the crystal lattice of the entire sample is continuous and unbroken to the edges of the sample, with no grain boundaries. [1] The absence of the defects associated with grain boundaries can give monocrystals unique properties, particularly mechanical, optical and electrical, which can also be anisotropic, depending on the type of crystallographic structure. [2] These properties, in addition to making some gems precious, are industrially used in technological applications, especially in optics and electronics. [3]

Contents

Because entropic effects favor the presence of some imperfections in the microstructure of solids, such as impurities, inhomogeneous strain and crystallographic defects such as dislocations, perfect single crystals of meaningful size are exceedingly rare in nature. [2] The necessary laboratory conditions often add to the cost of production. On the other hand, imperfect single crystals can reach enormous sizes in nature: several mineral species such as beryl, gypsum and feldspars are known to have produced crystals several meters across. [4] [1]

The opposite of a single crystal is an amorphous structure where the atomic position is limited to short-range order only. [5] In between the two extremes exist polycrystalline , which is made up of a number of smaller crystals known as crystallites , and paracrystalline phases. [6] Single crystals will usually have distinctive plane faces and some symmetry, where the angles between the faces will dictate its ideal shape. Gemstones are often single crystals artificially cut along crystallographic planes to take advantage of refractive and reflective properties. [6]

Production methods

Although current methods are extremely sophisticated with modern technology, the origins of crystal growth can be traced back to salt purification by crystallization in 2500 BCE. A more advanced method using an aqueous solution was started in 1600 CE while the melt and vapor methods began around 1850 CE. [7]

Single-crystal growth methods tree diagram Single Crystal Growth Methods Flow Chart .png
Single-crystal growth methods tree diagram

Basic crystal growth methods can be separated into four categories based on what they are artificially grown from: melt, solid, vapor, and solution. [2] Specific techniques to produce large single crystals (aka boules) include the Czochralski process (CZ), Floating zone (or Zone Movement), and the Bridgman technique. Dr. Teal and Dr. Little of Bell Telephone Laboratories were the first to use the Czochralski method to create Ge and Si single crystals. [8] Other methods of crystallization may be used, depending on the physical properties of the substance, including hydrothermal synthesis, sublimation, or simply solvent-based crystallization. [9] For example, a modified Kyropoulos method can be used to grow high quality 300 kg sapphire single crystals. [10] The Verneuil method, also called the flame-fusion method, was used in the early 1900s to make rubies before CZ. [7] The diagram on the right illustrates most of the conventional methods. There have been new breakthroughs such as chemical vapor depositions (CVD) along with different variations and tweaks to the existing methods. These are not shown in the diagram.

A single-crystal quartz bar grown by the hydrothermal method Quartz synthese.jpg
A single-crystal quartz bar grown by the hydrothermal method

In the case of metal single crystals, fabrication techniques also include epitaxy and abnormal grain growth in solids. [11] Epitaxy is used to deposit very thin (micrometer to nanometer scale) layers of the same or different materials on the surface of an existing single crystal. [12] Applications of this technique lie in the areas of semiconductor production, with potential uses in other nanotechnological fields and catalysis. [13]

It is extremely difficult to grow single crystals of the polymers. It is mainly because that the polymer chains are of different length and due to the various entropy reasons. However, topochemical reactions are one of the easy methods to get single crystals of the polymer.

Applications

Semiconductor industry

One of the most used single crystals is that of Silicon in the semiconductor industry. The four main production methods for semiconductor single crystals are from metallic solutions: liquid phase epitaxy (LPE), liquid phase electroepitaxy (LPEE), the traveling heater method (THM), and liquid phase diffusion (LPD). [14] However, there are many other single crystals besides inorganic single crystals capable semiconducting, including single-crystal organic semiconductors.

A high-purity (99.999 %) tantalum single crystal, made by the floating zone process, some single crystalline fragments of tantalum, and a high-purity (99.99% = 4N) 1 cm tantalum cube for comparison. This photo was taken by Alchemist-hp. Tantalum single crystal and 1cm3 cube.jpg
A high-purity (99.999 %) tantalum single crystal, made by the floating zone process, some single crystalline fragments of tantalum, and a high-purity (99.99% = 4N) 1 cm tantalum cube for comparison. This photo was taken by Alchemist-hp.

Monocrystalline silicon used in the fabrication of semiconductors and photovoltaics is the greatest use of single-crystal technology today. [15] In photovoltaics, the most efficient crystal structure will yield the highest light-to-electricity conversion. [16] On the quantum scale that microprocessors operate on, the presence of grain boundaries would have a significant impact on the functionality of field effect transistors by altering local electrical properties. [17] Therefore, microprocessor fabricators have invested heavily in facilities to produce large single crystals of silicon. The Czochralski method and floating zone are popular methods for the growth of Silicon crystals. [18]

Fluorescence of (9H-carbazol-9-yl)(4-chlorophenyl)methanone single crystal. ClPhCz monokristall.jpg
Fluorescence of (9H-carbazol-9-yl)(4-chlorophenyl)methanone single crystal.

Other inorganic semiconducting single crystals include GaAs, GaP, GaSb, Ge, InAs, InP, InSb, CdS, CdSe, CdTe, ZnS, ZnSe, and ZnTe. Most of these can also be tuned with various doping for desired properties. [19] Single-crystal graphene is also highly desired for applications in electronics and optoelectronics with its large carrier mobility and high thermal conductivity, and remains a topic of fervent research. [20] One of the main challenges has been growing uniform single crystals of bilayer or multilayer graphene over large areas; epitaxial growth and the new CVD (mentioned above) are among the new promising methods under investigation. [21]

Organic semiconducting single crystals are different from the inorganic crystals. The weak intermolecular bonds mean lower melting temperatures, and higher vapor pressures and greater solubility. [22] For single crystals to grow, the purity of the material is crucial and the production of organic materials usually require many steps to reach the necessary purity. [23] Extensive research is being done to look for materials that are thermally stable with high charge-carrier mobility. Past discoveries include naphthalene, tetracene, and 9,10-diphenylanthacene (DPA). [24] Triphenylamine derivatives have shown promise, and recently in 2021, the single-crystal structure of α-phenyl-4′-(diphenylamino)stilbene (TPA) grown using the solution method exhibited even greater potential for semiconductor use with its anisotropic hole transport property. [25]

Optical application

A huge KDP, potassium dihydrogen phosphate, crystal grown from a seed crystal in a supersaturated aqueous solution at LLNL which is to be cut into slices and used on the National Ignition Facility for frequency doubling and tripling. KDP crystal.jpg
A huge KDP, potassium dihydrogen phosphate, crystal grown from a seed crystal in a supersaturated aqueous solution at LLNL which is to be cut into slices and used on the National Ignition Facility for frequency doubling and tripling.

Single crystals have unique physical properties due to being a single grain with molecules in a strict order and no grain boundaries. [2] This includes optical properties, and single crystals of silicon is also used as optical windows because of its transparency at specific infrared (IR) wavelengths, making it very useful for some instruments. [5]

Sapphires: Also known as the alpha phase of aluminum oxide (Al2O3) to scientists, sapphire single crystals are widely used in hi-tech engineering. It can be grown from gaseous, solid, or solution phases. [10] The diameter of the crystals resulting from the growth method are important when considering electronic uses after. They are used for lasers and nonlinear optics. Some notable uses are as in the window of a biometric fingerprint reader, optical disks for long-term data storage, and X-ray interferometer. [2]

Indium Phosphide: These single crystals are particularly appropriate for combining optoelectronics with high-speed electronics in the form of optical fiber with its large-diameter substrates. [26] Other photonic devices include lasers, photodetectors, avalanche photo diodes, optical modulators and amplifiers, signal processing, and both optoelectronic and photonic integrated circuits. [27]

Aluminum oxide crystals Aluminum oxide cristals (corundum).jpg
Aluminum oxide crystals

Germanium: This was the material in the first transistor invented by Bardeen, Brattain, and Shockley in 1947. It is used in some gamma-ray detectors and infrared optics. [28] Now it has become the focus of ultrafast electronic devices for its intrinsic carrier mobility. [27]

Arsenide: Arsenide III can be combined with various elements such as B, Al, Ga, and In, with the GaAs compound being in high demand for wafers. [27]

Cadmium Telluride: CdTe crystals have several applications as substrates for IR imaging, electrooptic devices, and solar cells. [29] By alloying CdTe and ZnTe together room-temperature X-ray and gamma-ray detectors can be made. [27]

Electrical conductors

Metals can surprisingly be produced in single-crystal form and provide a means to understand the ultimate performance of metallic conductors. It is vital for understanding the basic science such as catalytic chemistry, surface physics, electrons, and monochromators. [4] Production of metallic single crystals have the highest quality requirements and are grown, or pulled, in the form of rods. [30] Certain companies can produce specific geometries, grooves, holes, and reference faces along with varying diameters. [19]

Of all the metallic elements, silver and copper have the best conductivity at room temperature, setting the bar for performance. [31] The size of the market, and vagaries in supply and cost, have provided strong incentives to seek alternatives or find ways to use less of them by improving performance.

The conductivity of commercial conductors is often expressed relative to the International Annealed Copper Standard, according to which the purest copper wire available in 1914 measured around 100%. The purest modern copper wire is a better conductor, measuring over 103% on this scale. The gains are from two sources. First, modern copper is more pure. However, this avenue for improvement seems at an end. Making the copper purer still makes no significant improvement. Second, annealing and other processes have been improved. Annealing reduces the dislocations and other crystal defects which are sources of resistance. But the resulting wires are still polycrystalline. The grain boundaries and remaining crystal defects are responsible for some residual resistance. This can be quantified and better understood by examining single crystals.

As anticipated, single-crystal copper did prove to have better conductivity than polycrystalline copper. [32]

Electrical resistivity ρ for silver (Ag) / copper (Cu) materials at room temperature (293 K) [33]
Materialρ (μΩ∙cm) IACS [34]
Single-crystal Ag, doped with 3 mol% Cu1.35127%
Single-crystal Cu, further processed [35] 1.472117.1%
Single-crystal Ag1.49115.4%
Single-crystal Cu1.52113.4%
High-purity Ag wire (polycrystalline)1.59108%
High-purity Cu wire (polycrystalline)1.67˃ 103%

However, the single-crystal copper not only became a better conductor than high purity polycrystalline silver, but with prescribed heat and pressure treatment could surpass even single-crystal silver. Although impurities are usually bad for conductivity, a silver single crystal with a small amount of copper substitutions proved to be the best.

As of 2009, no single-crystal copper is manufactured on a large scale industrially, but methods of producing very large individual crystal sizes for copper conductors are exploited for high performance electrical applications. These can be considered meta-single crystals with only a few crystals per meter of length.

Pigtail from single-crystal blade casting Pigtail from Single Crystal Blade Casting shown with Kennedy Half Dollar for size comparison.jpg
Pigtail from single-crystal blade casting

Single-crystal turbine blades

Another application of single-crystal solids is in materials science in the production of high strength materials with low thermal creep, such as turbine blades. [36] Here, the absence of grain boundaries actually gives a decrease in yield strength, but more importantly decreases the amount of creep which is critical for high temperature, close tolerance part applications. [37] Researcher Barry Piearcey found that a right-angle bend at the casting mold would decrease the number of columnar crystals and later, scientist Giamei used this to start the single-crystal structure of the turbine blade. [38]

In research

Single crystals are essential in research especially condensed-matter physics and all aspects of materials science such as surface science. [2] The detailed study of the crystal structure of a material by techniques such as Bragg diffraction and helium atom scattering is easier with single crystals because it is possible to study directional dependence of various properties and compare with theoretical predictions. [39] Furthermore, macroscopically averaging techniques such as angle-resolved photoemission spectroscopy or low-energy electron diffraction are only possible or meaningful on surfaces of single crystals. [40] [41] In superconductivity there have been cases of materials where superconductivity is only seen in single-crystalline specimen. [42] They may be grown for this purpose, even when the material is otherwise only needed in polycrystalline form.

As such, numerous new materials are being studied in their single-crystal form. The young field of metal-organic-frameworks (MOFs) is one of many which qualify to have single crystals. In January 2021 Dr. Dong and Dr. Feng demonstrated how polycyclic aromatic ligands can be optimized to produce large 2D MOF single crystals of sizes up to 200 μm. This could mean scientists can fabricate single-crystal devices and determine intrinsic electrical conductivity and charge transport mechanism. [43]

The field of photodriven transformation can also be involved with single crystals with something called single-crystal-to-single-crystal (SCSC) transformations. These provide direct observation of molecular movement and understanding of mechanistic details. [44] This photoswitching behavior has also been observed in cutting-edge research on intrinsically non-photo-responsive mononuclear lanthanide single-molecule-magnets (SMM). [45]

See also

Related Research Articles

<span class="mw-page-title-main">Chemical vapor deposition</span> Method used to apply surface coatings

Chemical vapor deposition (CVD) is a vacuum deposition method used to produce high-quality, and high-performance, solid materials. The process is often used in the semiconductor industry to produce thin films.

<span class="mw-page-title-main">Organic electronics</span> Field of materials science

Organic electronics is a field of materials science concerning the design, synthesis, characterization, and application of organic molecules or polymers that show desirable electronic properties such as conductivity. Unlike conventional inorganic conductors and semiconductors, organic electronic materials are constructed from organic (carbon-based) molecules or polymers using synthetic strategies developed in the context of organic chemistry and polymer chemistry.

<span class="mw-page-title-main">Gallium arsenide</span> Chemical compound

Gallium arsenide (GaAs) is a III-V direct band gap semiconductor with a zinc blende crystal structure.

<span class="mw-page-title-main">Czochralski method</span> Method of crystal growth

The Czochralski method, also Czochralski technique or Czochralski process, is a method of crystal growth used to obtain single crystals of semiconductors, metals, salts and synthetic gemstones. The method is named after Polish scientist Jan Czochralski, who invented the method in 1915 while investigating the crystallization rates of metals. He made this discovery by accident: instead of dipping his pen into his inkwell, he dipped it in molten tin, and drew a tin filament, which later proved to be a single crystal. The method is still used in over 90 percent of all electronics in the world that use semiconductors.

<span class="mw-page-title-main">Silicon carbide</span> Extremely hard semiconductor containing silicon and carbon

Silicon carbide (SiC), also known as carborundum, is a hard chemical compound containing silicon and carbon. A semiconductor, it occurs in nature as the extremely rare mineral moissanite, but has been mass-produced as a powder and crystal since 1893 for use as an abrasive. Grains of silicon carbide can be bonded together by sintering to form very hard ceramics that are widely used in applications requiring high endurance, such as car brakes, car clutches and ceramic plates in bulletproof vests. Large single crystals of silicon carbide can be grown by the Lely method and they can be cut into gems known as synthetic moissanite.

<span class="mw-page-title-main">Crystallite</span> Small crystal which forms under certain conditions

A crystallite is a small or even microscopic crystal which forms, for example, during the cooling of many materials. Crystallites are also referred to as grains.

<span class="mw-page-title-main">Epitaxy</span> Crystal growth process relative to the substrate

Epitaxy refers to a type of crystal growth or material deposition in which new crystalline layers are formed with one or more well-defined orientations with respect to the crystalline seed layer. The deposited crystalline film is called an epitaxial film or epitaxial layer. The relative orientation(s) of the epitaxial layer to the seed layer is defined in terms of the orientation of the crystal lattice of each material. For most epitaxial growths, the new layer is usually crystalline and each crystallographic domain of the overlayer must have a well-defined orientation relative to the substrate crystal structure. Epitaxy can involve single-crystal structures, although grain-to-grain epitaxy has been observed in granular films. For most technological applications, single domain epitaxy, which is the growth of an overlayer crystal with one well-defined orientation with respect to the substrate crystal, is preferred. Epitaxy can also play an important role while growing superlattice structures.

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<span class="mw-page-title-main">Crystalline silicon</span> Semiconducting material used in solar cell technology

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<span class="mw-page-title-main">Polycrystalline silicon</span> High purity form of silicon

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References

  1. 1 2 RIWD. "Reade Advanced Materials – Single Crystals". www.reade.com. Retrieved 2021-02-28.
  2. 1 2 3 4 5 6 Fornari, Roberto (2018). Single Crystals of Electronic Materials : Growth and Properties. San Diego: Elsevier Science & Technology. ISBN   978-0-08-102097-5. OCLC   1055046791.[ page needed ]
  3. ↑ "Single Crystals – Alfa Chemistry". www.alfa-chemistry.com. Retrieved 2021-02-28.
  4. 1 2 "Pure Element Single Crystals – Alfa Chemistry". www.alfa-chemistry.com. Retrieved 2021-02-28.
  5. 1 2 "4.1: Introduction". Engineering LibreTexts. 2019-02-08. Retrieved 2021-02-28.
  6. 1 2 "DoITPoMS – TLP Library Atomic Scale Structure of Materials". www.doitpoms.ac.uk. Retrieved 2021-02-28.
  7. 1 2 "Growing Single Crystals". Ceramic Materials. 2007. pp. 507–526. doi:10.1007/978-0-387-46271-4_29. ISBN   978-0-387-46270-7. S2CID   240461586.
  8. ↑ Teal, G.K. and Little, J.B. (1950) “Growth of germanium single crystals,” Phys. Rev. 78, 647. Teal and Little of Bell Telephone Laboratories were the first to produce single crystals of Ge and Si by the Cz method. Cited in "Growing Single Crystals". Ceramic Materials. 2007. pp. 507–526. doi:10.1007/978-0-387-46271-4_29. ISBN   978-0-387-46270-7. S2CID   240461586.
  9. ↑ Miyazaki, Noriyuki (2015). "Thermal Stress and Dislocations in Bulk Crystal Growth". Handbook of Crystal Growth. pp. 1049–1092. doi:10.1016/b978-0-444-63303-3.00026-2. ISBN   9780444633033.
  10. 1 2 Zalozhny, Eugene (Jul 13th, 2015). "Monocrystal enables high-volume LED and optical applications with 300-kg KY sapphire crystals". LED's Magazine. Retrieved February 27, 2021.
  11. ↑ Jin, Sunghwan; Ruoff, Rodney S. (1 October 2019). "Preparation and uses of large area single crystal metal foils". APL Materials. 7 (10): 100905. doi: 10.1063/1.5114861 . S2CID   208729868.
  12. ↑ Zhang, Kai; Pitner, Xue Bai; Yang, Rui; Nix, William D.; Plummer, James D.; Fan, Jonathan A. (23 January 2018). "Single-crystal metal growth on amorphous insulating substrates". Proceedings of the National Academy of Sciences. 115 (4): 685–689. doi: 10.1073/pnas.1717882115 . PMC   5789947 . PMID   29311332.
  13. ↑ "Single Crystal Substrates – Alfa Chemistry". www.alfa-chemistry.com. Retrieved 2021-03-11.
  14. ↑ Dost, Sadik; Lent, Brian (2007-01-01), Dost, Sadik; Lent, Brian (eds.), "Chapter 1 – INTRODUCTION", Single Crystal Growth of Semiconductors from Metallic Solutions, Amsterdam: Elsevier, pp. 3–14, doi:10.1016/b978-044452232-0/50002-x, ISBN   978-0-444-52232-0 , retrieved 2021-03-11
  15. ↑ Kearns, Joel K. (2019-01-01), Fornari, Roberto (ed.), "2 – Silicon single crystals", Single Crystals of Electronic Materials, Woodhead Publishing Series in Electronic and Optical Materials, Woodhead Publishing, pp. 5–56, doi:10.1016/b978-0-08-102096-8.00002-1, ISBN   978-0-08-102096-8, S2CID   139380571 , retrieved 2021-03-11
  16. ↑ "CZ-Si Wafers – Nanografi". nanografi.com. Retrieved 2021-02-28.
  17. ↑ Doi, Toshiro; Marinescu, Ioan D.; Kurokawa, Syuhei, eds. (2012-01-01), "Chapter 3 – The Current Situation in Ultra-Precision Technology – Silicon Single Crystals as an Example", Advances in CMP Polishing Technologies, Oxford: William Andrew Publishing: 15–111, doi:10.1016/b978-1-4377-7859-5.00003-x, ISBN   978-1-4377-7859-5 , retrieved 2021-03-11
  18. ↑ Friedrich, Jochen; von Ammon, Wilfried; Müller, Georg (2015). "Czochralski Growth of Silicon Crystals". Handbook of Crystal Growth. pp. 45–104. doi:10.1016/B978-0-444-63303-3.00002-X. ISBN   9780444633033.
  19. 1 2 "Semiconductor Single Crystals". Princeton Scientific. Retrieved 2021-02-08.
  20. ↑ Ma, Teng; Ren, Wencai; Zhang, Xiuyun; Liu, Zhibo; Gao, Yang; Yin, Li-Chang; Ma, Xiu-Liang; Ding, Feng; Cheng, Hui-Ming (2013). "Edge-controlled growth and kinetics of single-crystal graphene domains by chemical vapor deposition". Proceedings of the National Academy of Sciences of the United States of America. 110 (51): 20386–20391. Bibcode:2013PNAS..11020386M. doi: 10.1073/pnas.1312802110 . JSTOR   23761563. PMC   3870701 . PMID   24297886.
  21. ↑ Wang, Meihui; Luo, Da; Wang, Bin; Ruoff, Rodney S. (January 2021). "Synthesis of Large-Area Single-Crystal Graphene". Trends in Chemistry. 3 (1): 15–33. doi: 10.1016/j.trechm.2020.10.009 . S2CID   229501087.
  22. ↑ Yu, Panpan; Zhen, Yonggang; Dong, Huanli; Hu, Wenping (November 2019). "Crystal Engineering of Organic Optoelectronic Materials". Chem. 5 (11): 2814–2853. doi: 10.1016/j.chempr.2019.08.019 .
  23. ↑ Chou, Li-Hui; Na, Yaena; Park, Chung-Hyoi; Park, Min Soo; Osaka, Itaru; Kim, Felix Sunjoo; Liu, Cheng-Liang (March 2020). "Semiconducting small molecule/polymer blends for organic transistors". Polymer. 191: 122208. doi:10.1016/j.polymer.2020.122208. S2CID   213570529.
  24. ↑ Tripathi, A. K.; Heinrich, M.; Siegrist, T.; Pflaum, J. (17 August 2007). "Growth and Electronic Transport in 9,10-Diphenylanthracene Single Crystals—An Organic Semiconductor of High Electron and Hole Mobility". Advanced Materials. 19 (16): 2097–2101. Bibcode:2007AdM....19.2097T. doi:10.1002/adma.200602162. S2CID   97631495.
  25. ↑ Matsuda, Shofu; Ito, Masamichi; Itagaki, Chikara; Imakubo, Tatsuro; Umeda, Minoru (February 2021). "Characterization of α-phenyl-4′-(diphenylamino)stilbene single crystal and its anisotropic conductivity". Materials Science and Engineering: B. 264: 114949. doi: 10.1016/j.mseb.2020.114949 .
  26. ↑ "Indium Phosphide PICs". 100G Optical Components, Coherent, PIC, DWDM. Retrieved 2021-03-12.
  27. 1 2 3 4 Fornari, Roberto (18 September 2018). Single crystals of electronic materials : growth and properties. Woodhead. ISBN   978-0-08-102097-5. OCLC   1054250691.[ page needed ]
  28. ↑ Gafni, G.; Azoulay, M.; Shiloh, C.; Noter, Y.; Saya, A.; Galron, H.; Roth, M. (10 November 1987). Spiro, Irving J (ed.). "Large Diameter Germanium Single Crystals For IR Optics". Infrared Technology XIII. 0819: 96. Bibcode:1987SPIE..819...96G. doi:10.1117/12.941806. S2CID   136334692.{{cite journal}}: Cite journal requires |journal= (help)
  29. ↑ Belas, E.; Uxa, Š.; Grill, R.; Hlídek, P.; Šedivý, L.; Bugár, M. (14 September 2014). "High temperature optical absorption edge of CdTe single crystal". Journal of Applied Physics. 116 (10): 103521. Bibcode:2014JAP...116j3521B. doi:10.1063/1.4895494.
  30. ↑ "Scientists blow hot and cold to produce single-crystal metal". Materials Today. Retrieved 2021-03-12.
  31. ↑ "TIBTECH innovations: Metal properties comparison: electric conductivity, thermal conductivity, density, melting temperature". www.tibtech.com. Retrieved 2021-03-12.
  32. ↑ Cho, Yong Chan; Seunghun Lee; Muhammad Ajmal; Won-Kyung Kim; Chae Ryong Cho; Se-Young Jeong; Jeung Hun Park; Sang Eon Park; Sungkyun Park; Hyuk-Kyu Pak; Hyoung Chan Kim (March 22, 2010). "Copper Better than Silver: Electrical Resistivity of the Grain-Free Single-Crystal Copper Wire". Crystal Growth & Design. 10 (6): 2780–2784. doi:10.1021/cg1003808.
  33. ↑ Ji Young Kim; Min-Wook Oh; Seunghun Lee; Yong Chan Cho; Jang-Hee Yoon; Geun Woo Lee; Chae-Ryong Cho; Chul Hong Park; Se-Young Jeong (June 26, 2014). "Abnormal drop in electrical resistivity with impurity doping of single-crystal Ag". Scientific Reports. 4: 5450. Bibcode:2014NatSR...4E5450K. doi:10.1038/srep05450. PMC   4071311 . PMID   24965478.
  34. ↑ "The International Annealed Copper Standard". Nondestructive Testing Resource Center. The Collaboration for NDT Education, Iowa State University. n.d. Retrieved November 14, 2016.
  35. ↑ Muhammad Ajmal; Seunghun Lee; Yong Chan Cho; Su Jae Kim; Sang Eon Park; Chae Ryong Choa; Se-Young Jeong (2012). "Fabrication of the best conductor from single-crystal copper and the contribution of grain boundaries to the Debye temperature". CrystEngComm. 14 (4): 1463–1467. doi:10.1039/C1CE06026K.
  36. ↑ Spittle, Peter. "Gas turbine technology" Rolls-Royce plc , 2003. Retrieved: 21 July 2012.
  37. ↑ Crown jewels – These crystals are the gems of turbine efficiency Archived 2010-03-25 at the Wayback Machine Article on single-crystal turbine blades memagazine.com
  38. ↑ "Each Blade a Single Crystal". American Scientist. 2017-02-06. Retrieved 2021-02-08.
  39. ↑ "Silver Single Crystal". Materials Hub. Retrieved 2021-03-12.
  40. ↑ Wang, Ke; Ecker, Ben; Gao, Yongli (September 2020). "Angle-Resolved Photoemission Study on the Band Structure of Organic Single Crystals". Crystals. 10 (9): 773. doi: 10.3390/cryst10090773 .
  41. ↑ "6.2: Low Energy Electron Diffraction (LEED)". Chemistry LibreTexts. 2015-02-11. Retrieved 2021-03-12.
  42. ↑ Chen, Jiasheng; Gamża, Monika B.; Banda, Jacintha; Murphy, Keiron; Tarrant, James; Brando, Manuel; Grosche, F. Malte (30 November 2020). "Unconventional Bulk Superconductivity in YFe 2 Ge 2 Single Crystals". Physical Review Letters. 125 (23): 237002. arXiv: 2007.13584 . doi:10.1103/PhysRevLett.125.237002. PMID   33337220. S2CID   220793188.
  43. ↑ Dong, Renhao; Feng, Xinliang (February 2021). "Making large single crystals of 2D MOFs". Nature Materials. 20 (2): 122–123. doi:10.1038/s41563-020-00912-1. PMID   33504985. S2CID   231745364.
  44. ↑ Huang, Sheng-Li; Hor, T.S. Andy; Jin, Guo-Xin (September 2017). "Photodriven single-crystal-to-single-crystal transformation". Coordination Chemistry Reviews. 346: 112–122. doi: 10.1016/j.ccr.2016.06.009 .
  45. ↑ Hojorat, Maher; Al Sabea, Hassan; Norel, Lucie; Bernot, Kevin; Roisnel, Thierry; Gendron, Frederic; Guennic, Boris Le; Trzop, Elzbieta; Collet, Eric; Long, Jeffrey R.; Rigaut, Stéphane (15 January 2020). "Hysteresis Photomodulation via Single-Crystal-to-Single-Crystal Isomerization of a Photochromic Chain of Dysprosium Single-Molecule Magnets" (PDF). Journal of the American Chemical Society. 142 (2): 931–936. doi:10.1021/jacs.9b10584. PMID   31880442. S2CID   209490756.

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