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Thermonuclear weapons are weapons of mass destruction with high explosive yields that operate on the principles of nuclear fusion. These weapons, commonly referred to as “hydrogen bombs,” function not only through nuclear fission reactions as in atomic bombs but also through fusion reactions. This building enables them to produce a far more powerful destructive effect than atomic bombs.
The basic structure of thermonuclear weapons is two-stage: a primary stage, typically a fission bomb using plutonium-239 or other fissile materials. This primary explosion triggers fusion reactions in the secondary stage by subjecting fusion fuel—typically deuterium, tritium, or lithium-6 deuteride—to high pressure and temperature. This process is based on the same principle as nuclear fusion reactions occurring in Sun, where lighter atomic nuclei fuse to form heavier nuclei, releasing vast amounts of energy in the process.
A typical thermonuclear war warhead employs a two-stage design known as “Teller-Ulam,” in which radiation from the primary fission explosion compresses and ignites the secondary component through energy transfer within a metal cash box. In this design, the radiation generates a high-energy plasma in the void, and this plasma collapses inward under immense pressure through a heavy outer shell (tamper) surrounding the secondary component, initiating the fusion reaction.
The secondary component usually contains a fusion material such as lithium-6 deuteride, encircled by a fissile “spark plug” such as uranium-235 at its center. Neutrons released during the fusion reactions trigger additional fission reactions in the fissile materials, thereby increasing the weapon’s overall yield.
The development of thermonuclear weapons gained momentum during the Cold War era as a result of the strategic competition between the United States and the Soviet Union. Developed in the 1950s, these weapons were made compact and lightweight enough to be integrated into intercontinental ballistic missiles (ICBMs).
The first hydrogen bomb test, codenamed “Mike,” conducted by USA in 1952, used a 82-ton device with liquid deuterium. Subsequently, the 1954 “Bravo” test produced a 15-megaton explosion using solid lithium deuteride, eliminating the need for cryogenic equipment. This explosion generated three times more energy than expected and caused widespread important radioactive contamination.
Modern modern thermonuclear warheads are designed to achieve high yield-to-weight ratios. In these devices, the primary component is often enhanced to produce higher yields with less plutonium. Additionally, some advanced designs can theoretically be extended to include third and fourth stages; however, practical delivery constraints limit such expansions.
The fast neutrons released by fusion reactions in the secondary stage can induce fission in surrounding materials such as uranium-238 or thorium-232, thereby increasing yield. Some designs have further increased explosive power by using highly enriched uranium-235 instead of these surrounding materials.
The Comprehensive Nuclear-Test-Ban Treaty (CTBT), signed in 1996 to prevent the proliferation of nuclear weapons, aims to detect nuclear tests using seismic, infrasound, and radionuclide monitoring systems. To date, the agreement has been signed by 183 country, but has not been ratified by several countries.
The International Monitoring System (IMS), established under the CTBT, monitors global nuclear tests by detecting seismic waves from underground tests and atmospheric fallout.

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Thermonuclear Weapons
Principle of Operation
Design Features
Historical Development
Modern Applications and Advanced Designs
Nuclear Weapons Testing and Controls