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The Left-Handed Universe: How Madame Wu Shattered the Sacred Law of Symmetry

Physicists universally believed that the laws of nature look completely identical when viewed in a mirror; Chien-Shiung Wu proved that radioactive atoms preferentially shoot electrons in only one direction, proving that nature has an intrinsic left-handed bias. Executed at cryogenic temperatures in 1957, the "Wu Experiment" shattered the sacred law of Parity Conservation, revolutionizing particle physics and laying the foundation for the electroweak Standard Model.

Author
Chenye Wu et al.
Published
1957
Journal
Physical Review
Last updated
September 2026
The Left-Handed Universe: How Madame Wu Shattered the Sacred Law of Symmetry

In 1950s physics, symmetry was considered the sacred law of the universe: whether a physical reaction happens right-handed or left-handed, looking in a mirror should produce an identical, valid physical process. No physicist imagined nature would have a built-in preference for one hand over the other.

Experimental physicist Chien-Shiung Wu designed a masterwork experiment. She froze radioactive Cobalt-60 atoms down to near absolute zero and aligned their magnetic spins with a strong magnet. When the cobalt atoms decayed, they shot electrons almost exclusively downward out the south pole—proving that the weak nuclear force violates mirror symmetry completely.

The result stunned the world and earned theorists Lee and Yang the Nobel Prize. By proving that our universe is fundamentally left-handed, by establishing the V-A theory of weak interactions, and by anchoring the Standard Model of subatomic particles, the Wu experiment changed fundamental physics.

Reference

Wu, C. S., Ambler, E., Hayward, R. W., Hoppes, D. D., & Hudson, R. P. (1957). Experimental Test of Parity Conservation in Beta Decay. Physical Review, 105(4), 1413–1415.

Title

Experimental Test of Parity Conservation in Beta Decay

Abstract

The branching ratio of the two modes of decay of Fm'", i.e. , E.C. /n, was found to be about 8.5which gives 89.5% decay by electron capture and 10.5% by alpha emission. It was not possible to measure the cross section for the Cf'"(n, 3n)Fm'" reaction because Fm'" could also be produced from other californium isotopes in the target.

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