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 "title": "Vertical Bridgman method",
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 "excerpt": "The vertical Bridgman method is a crystal growth technique that directionally solidifies a melt in a vertical ampoule, dominating production of III-V and II-VI compound semiconductors.",
 "snippet": "The vertical Bridgman method is a crystal growth technique that directionally solidifies a melt in a vertical ampoule, dominating production of III-V and II-VI compound semiconductors.",
 "node": "technology.engineering.engineering.materials.metallurgy",
 "markdown": "# Vertical Bridgman method\n\nThe vertical Bridgman method is a crystal growth technique in which a molten charge contained in a vertical ampoule is directionally solidified to produce single crystals of compound semiconductors and detector materials. Bridgman-type methods dominate the growth of binary III-V and II-VI compound semiconductors with melting temperatures below 2000 K and decomposition pressures below about 10 bar, where scalability and production maturity favor them over Czochralski pulling.<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup> For cadmium zinc telluride (CZT), vertical Bridgman growth with excess Te is one of the most common techniques, and its maximum growth rate is much larger than in solution growth.<sup>[2](https://mdpi-res.com/d_attachment/crystals/crystals-10-00261/article_deploy/crystals-10-00261-v2.pdf?version=1586844120)</sup>\n\n| Key fact | Value |\n|---|---|\n| Materials dominated | Binary III-V and II-VI semiconductors, melting point below 2000 K, decomposition pressure below ~10 bar<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup> |\n| Typical CZT gradients | 55 °C/cm at the ampoule wall (64 mm CdTe/CdZnTe)<sup>[3](https://www.sciencedirect.com/science/article/abs/pii/0022024894912718)</sup>; ~20 °C/cm in ACRT-assisted growth<sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> |\n| Typical growth rate | ~1-2 mm/h for detector-grade CZT<sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> |\n| Dislocation density (VB CZT) | ~1-\\( 5 \\times 10^{4} \\) cm⁻²<sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> |\n| Post-growth cooldown | 25-50 °C/h<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup>; 10 °C/h in 64 mm CdZnTe work<sup>[3](https://www.sciencedirect.com/science/article/abs/pii/0022024894912718)</sup> |\n| Single-crystal yield example | First 70% of a 20 mm diameter CdZnTe ingot<sup>[5](https://ntrs.nasa.gov/api/citations/20090008531/downloads/20090008531.pdf)</sup> |\n| Recent scale | 150 mm diameter CZT by gradient freeze (2025)<sup>[6](http://rgjtxb.jtxb.cn/EN/10.16553/j.cnki.issn1000-985x.2025.0217)</sup> |\n\n## How it works\n\nThe whole melt solidifies inside its crucible under an imposed vertical temperature gradient. A 2024 study of CZT growth by vertical Bridgman and vertical gradient freeze found that a larger temperature gradient on the solid-phase side of the interface helps achieve stable growth at a convex interface.<sup>[7](http://rgjtxb.jtxb.cn/EN/Y2024/V53/I4/641)</sup> Finite-element simulations of CdZnTe growth show that when the crucible descends at about 1 mm/h, nearly equal to the crystal growth rate, a nearly flat solid/liquid interface and little variation of the axial temperature gradient near it are attained, consistent with experiment.<sup>[8](https://www.jim.org.cn/EN/abstract/abstract9797.shtml)</sup>\n\n## How it is done\n\nA practitioner selects an ampoule material (quartz or pyrolytic boron nitride), charges it with synthesized starting material, and evacuates or backfills it. The ampoule sits in a furnace with a hot zone above the melting point and a cool zone below it. In Cd-overpressure-controlled Bridgman growth of Cd\\(_{0.80}\\)Zn\\(_{0.20}\\)Te, the melt was held above the 1130 °C melting point while a separate Cd reservoir was held at 750-935 °C (most runs 785-820 °C) to control the vapor pressure over the charge; ampoules were 20 mm or 40 mm inner diameter.<sup>[5](https://ntrs.nasa.gov/api/citations/20090008531/downloads/20090008531.pdf)</sup> Growth then proceeds by translating the ampoule at 0.75 to 2 mm/h, or by electronically translating a temperature profile upward as in gradient freeze furnaces.<sup>[5](https://ntrs.nasa.gov/api/citations/20090008531/downloads/20090008531.pdf)</sup><sup> • </sup><sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> After solidification, the furnace is cooled to room temperature at 25-50 °C/h to reduce stresses from differential expansion of crystal, encapsulant, and crucible walls,<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup> though the CdZnTe overpressure study cooled over 96 to 144 hours<sup>[5](https://ntrs.nasa.gov/api/citations/20090008531/downloads/20090008531.pdf)</sup> and the 64 mm CdTe/CdZnTe work used 10 °C/h.<sup>[3](https://www.sciencedirect.com/science/article/abs/pii/0022024894912718)</sup>\n\n## Origin\n\nThe vertical gradient freeze variant for large-diameter compound semiconductors predates a 2001 report by T. Asahi, A. Arakawa, and K. Sato in the Journal of Crystal Growth, in work on the growth of large-diameter ZnTe single crystals, having been applied to III–V crystals by 1986.<sup>[9](https://doi.org/10.1016/s0022-0248%2801%2901097-1)</sup><sup> • </sup><sup>[12](https://data.epo.org/publication-server/rest/v1.2/publication-dates/19910703/patents/EP0435454NWA1/document.pdf)</sup>\n\n## Variants\n\n**Vertical gradient freeze (VGF)** keeps the crucible stationary and moves the temperature field instead; it has produced large-diameter ZnTe crystals<sup>[9](https://doi.org/10.1016/s0022-0248%2801%2901097-1)</sup> and, in recent work, 150 mm diameter CZT.<sup>[6](http://rgjtxb.jtxb.cn/EN/10.16553/j.cnki.issn1000-985x.2025.0217)</sup> **Accelerated crucible rotation (ACRT)** rotates the ampoule during growth to improve melt homogeneity and interface boundary conditions; other reported process improvements include vibroconvective mixing, baffles near the interface, and growth under high pressure.<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup> **Liquid encapsulation** with boron oxide is necessary for reproducible GaAs growth, and pyrolytic boron nitride crucibles appear well suited for GaP.<sup>[10](https://www.osti.gov/servlets/purl/5154546)</sup>\n\n## Applications\n\nVertical Bridgman and its modifications grow detector-grade CZT with growth rates an order of magnitude faster than traveling heater method (THM) growth, about 1-2 mm per hour, without post-growth processing and with fewer dislocations, roughly 1-\\( 5 \\times 10^{4} \\) cm⁻² versus about \\( 5 \\times 10^{5} \\) cm⁻² induced by the narrow heat zone and high gradients of THM-type growth.<sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> A representative ACRT-assisted process used a temperature gradient of about 20 °C/cm at the bottom furnace zones translated upward at about 2 mm/hr, soak times of 3 to 24 hours, 6N5 purity CdTe/ZnTe charges with total Te of \\(50.12-61.75\\) atomic percent, and a total growth campaign of 7 to 10 days in a 4-inch bore electrodynamic gradient freeze furnace.<sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> Earlier 64 mm diameter Cd\\(_{1-x}\\)Zn\\(_x\\)Te (x = 0.04) and CdTe growth used an axial gradient of 55 °C/cm at the ampoule wall, a solidification velocity of 1.0 mm/h, and 10 °C/h post-solidification cooling; the CdZnTe showed fewer crystalline defects and better morphological uniformity than CdTe, supporting its use as an IR detector substrate.<sup>[3](https://www.sciencedirect.com/science/article/abs/pii/0022024894912718)</sup> In Cd-overpressure-controlled growth, undoped crystals showed resistivity varying inconsistently from \\( 10^{3} \\) to \\( 10^{10} \\ \\Omega \\cdot \\mathrm{cm} \\), but 4-6 ppm atomic indium doping gave resistivity consistently above \\( 10^{8} \\ \\Omega \\cdot \\mathrm{cm} \\) when the Cd reservoir was between 785 and 825 °C, and single crystals were consistently produced on the first 70% of a 20 mm diameter ingot.<sup>[5](https://ntrs.nasa.gov/api/citations/20090008531/downloads/20090008531.pdf)</sup> Recent work extends the method to 150 mm diameter CZT with finite-element-regulated heater power, achieving a convex interface throughout growth, (111) rocking-curve FWHM below 15 arcseconds, etch pit density below \\( 1 \\times 10^{4} \\) cm⁻², and 100 mm × 100 mm infrared substrates.<sup>[6](http://rgjtxb.jtxb.cn/EN/10.16553/j.cnki.issn1000-985x.2025.0217)</sup> Detector-grade CsPbBr₃ has also been grown by vertical Bridgman with 1.5% excess CsBr to avoid secondary-phase precipitates, yielding 60 mm diameter ingots over 90 mm long with resistivity of \\( 1.8 \\times 10^{9} \\) Ω·cm.<sup>[11](https://pubs.rsc.org/en/content/articlelanding/2026/tc/d5tc02826d)</sup>\n\n## Limitations and alternatives\n\nSticking between the crucible and the charge creates random nucleation sites on the crucible wall and generates low-angle grain boundaries and twins.<sup>[10](https://www.osti.gov/servlets/purl/5154546)</sup> Some important III-V compounds expand on cooling and can aggressively stick to the walls of many crucible materials, complicating vertical Bridgman and gradient freeze growth.<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup> VB-grown CZT suffers from low single crystal yield, extended defects, and low electron mobility-lifetime (\\( \\mu\\tau_{e} \\)) products inherent to melt growth, although ACRT has addressed many of these issues.<sup>[4](https://www.osti.gov/servlets/purl/1543145)</sup> Macroscopic Zn segregation along the ingot has been mapped by photoluminescence spectroscopy and linked to the temperature-field distribution.<sup>[7](http://rgjtxb.jtxb.cn/EN/Y2024/V53/I4/641)</sup> Reproducible growth of fully single crystals of InP had not been demonstrated in a reported assessment, and in very large systems control of heat flows is more difficult because of the very low thermal conductivities of the III-V compounds.<sup>[10](https://www.osti.gov/servlets/purl/5154546)</sup>\n\nCompared with Czochralski pulling, vertical Bridgman-type techniques involve simpler technology and offer excellent diameter control, which reduces waste from subsequent grinding operations.<sup>[10](https://www.osti.gov/servlets/purl/5154546)</sup> Horizontal Bridgman and gradient freeze techniques produce boules that are limited in size compared with their vertical counterparts and have noncircular cross-sections.<sup>[1](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)</sup> A direct quantitative comparison with float-zone growth has not been published; the documented recent changes are modeling-driven temperature-field control<sup>[6](http://rgjtxb.jtxb.cn/EN/10.16553/j.cnki.issn1000-985x.2025.0217)</sup><sup> • </sup><sup>[7](http://rgjtxb.jtxb.cn/EN/Y2024/V53/I4/641)</sup> and new materials such as large-diameter CsPbBr₃.<sup>[11](https://pubs.rsc.org/en/content/articlelanding/2026/tc/d5tc02826d)</sup>\n\n## References\n\n1. [Bridgman Method - an overview | ScienceDirect Topics](https://www.sciencedirect.com/topics/physics-and-astronomy/bridgman-method)\n2. [Crystals (MDPI) article on CZT growth](https://mdpi-res.com/d_attachment/crystals/crystals-10-00261/article_deploy/crystals-10-00261-v2.pdf?version=1586844120)\n3. [The growth and comparison of large-diameter vertical Bridgman CdZnTe and CdTe](https://www.sciencedirect.com/science/article/abs/pii/0022024894912718)\n4. [Overcoming Mobility Lifetime Product Limitations in Vertical Bridgman Production of Cadmium Zinc Telluride Detectors](https://www.osti.gov/servlets/purl/1543145)\n5. [Growth of CdZnTe Crystals by Bridgman Technique with Controlled Overpressures of Cd](https://ntrs.nasa.gov/api/citations/20090008531/downloads/20090008531.pdf)\n6. [Temperature Field Control for the Growth of 150 mm Diameter CZT Crystals](http://rgjtxb.jtxb.cn/EN/10.16553/j.cnki.issn1000-985x.2025.0217)\n7. [Relationship Between Temperature Gradient and Interfacial Shape Stability of CZT Crystal Growth](http://rgjtxb.jtxb.cn/EN/Y2024/V53/I4/641)\n8. [Optimization of Crucible Descending Rate during the Crystal Growth of CdZnTe by a Vertical Bridgman Method](https://www.jim.org.cn/EN/abstract/abstract9797.shtml)\n9. [Growth of large-diameter ZnTe single crystals by the vertical gradient freezing method (Journal of Crystal Growth, 2001)](https://doi.org/10.1016/s0022-0248%2801%2901097-1)\n10. [Vertical Bridgman growth of III-V compounds (OSTI report)](https://www.osti.gov/servlets/purl/5154546)\n11. [Stoichiometric engineering for large-size CsPbBr3 crystal growth and gamma-ray detection optimization](https://pubs.rsc.org/en/content/articlelanding/2026/tc/d5tc02826d)\n12. [data.epo.org](https://data.epo.org/publication-server/rest/v1.2/publication-dates/19910703/patents/EP0435454NWA1/document.pdf)\n\n---\n*Topic: Encyclopedia › Technology and the built world › Engineering and manufacturing › Materials science and metallurgy*\n\n*Initially written Sep 29, 2026 · Edited: Oct 15, 2026*\n\n*Copyright 2026 EdgeChat AI, a subsidiary of Biostate AI.*\n\nLicense: Edgepedia Community License 1.0, https://www.edgepedia.org/edgepedia/license\n",
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