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In physics, parity refers to a property of a system's wave function, essentially its mirror-image symmetry. A parity transformation inverts spatial coordinates (x, y, z to \u2212x, \u2212y, \u2212z). If the system remains identical after this transformation, it has even parity; if it becomes negative, it has odd parity. For a long time, it was believed that parity was always conserved in fundamental interactions, meaning physical laws were indifferent to mirror reflections.

However, in 1956, it was proposed that parity is not conserved in interactions governed by the weak force. Experimental evidence later confirmed this, showing that particles involved in weak interactions can exhibit a built-in "handedness." While parity is not conserved alone, it is believed to be conserved when combined with charge conjugation (C) and time reversal (T) operations, forming the CPT theorem.12

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