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Kinoshita-Lee-Nauenberg theorem
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Kinoshita-Lee-Nauenberg theorem : ウィキペディア英語版
Kinoshita-Lee-Nauenberg theorem
The Kinoshita–Lee–Nauenberg theorem or KLN theorem states that perturbatively the standard model as a whole is infrared (IR) finite. That is, the infrared divergences coming from loop integrals are canceled by IR divergences coming from phase space integrals. It was introduced independently by and .
An analogous result for quantum electrodynamics alone is known as Bloch–Nordsieck cancellation.
Ultraviolet divergences in perturbative quantum field theory are dealt with in renormalization.
==References==

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*Taizo Muta, Foundations of Quantum Chromodynamics: An Introduction to Perturbative Methods in Gauge Theories, World Scientific Publishing Company; 3 edition (September 30, 2009)

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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