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删除535字节 、 2021年9月1日 (三) 15:50
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The scale-dependence of a [[quantum field theory]] (QFT) is characterised by the way its [[coupling constant|coupling parameters]] depend on the energy-scale of a given physical process. This energy dependence is described by the [[renormalization group]], and is encoded in the [[beta-function]]s of the theory.
 
The scale-dependence of a [[quantum field theory]] (QFT) is characterised by the way its [[coupling constant|coupling parameters]] depend on the energy-scale of a given physical process. This energy dependence is described by the [[renormalization group]], and is encoded in the [[beta-function]]s of the theory.
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量子场论(QFT)的标度依赖性的特征是其耦合参数依赖于给定物理过程的能量标度。这种能量依赖由重正化群描述,并编码在理论的β函数中。
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量子场论(QFT)的标度依赖性的特征是其耦合参数依赖于给定物理过程的能量标度。这种能量依赖由重正化群描述,并编码在理论的'''Beta-function β函数'''中。
    
For a QFT to be scale-invariant, its coupling parameters must be independent of the energy-scale, and this is indicated by the vanishing of the beta-functions of the theory. Such theories are also known as [[Renormalization group|fixed points]] of the corresponding renormalization group flow.<ref>[[Jean Zinn-Justin|J. Zinn-Justin]] (2010)  Scholarpedia article [http://www.scholarpedia.org/article/Critical_Phenomena:_field_theoretical_approach "Critical Phenomena: field theoretical approach"].</ref>
 
For a QFT to be scale-invariant, its coupling parameters must be independent of the energy-scale, and this is indicated by the vanishing of the beta-functions of the theory. Such theories are also known as [[Renormalization group|fixed points]] of the corresponding renormalization group flow.<ref>[[Jean Zinn-Justin|J. Zinn-Justin]] (2010)  Scholarpedia article [http://www.scholarpedia.org/article/Critical_Phenomena:_field_theoretical_approach "Critical Phenomena: field theoretical approach"].</ref>
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However, in nature the electromagnetic field is coupled to charged particles, such as [[electron]]s. The QFT describing the interactions of photons and charged particles is [[quantum electrodynamics]] (QED), and this theory is not scale-invariant. We can see this from the [[beta-function#Quantum electrodynamics|QED beta-function]]. This tells us that the [[electric charge]] (which is the coupling parameter in the theory) increases with increasing energy. Therefore, while the quantized electromagnetic field without charged particles '''is''' scale-invariant, QED is '''not''' scale-invariant.
 
However, in nature the electromagnetic field is coupled to charged particles, such as [[electron]]s. The QFT describing the interactions of photons and charged particles is [[quantum electrodynamics]] (QED), and this theory is not scale-invariant. We can see this from the [[beta-function#Quantum electrodynamics|QED beta-function]]. This tells us that the [[electric charge]] (which is the coupling parameter in the theory) increases with increasing energy. Therefore, while the quantized electromagnetic field without charged particles '''is''' scale-invariant, QED is '''not''' scale-invariant.
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然而在自然界中,电磁场是与带电粒子耦合的,比如电子。描述光子和带电粒子相互作用的量子场论是量子电动力学,而这个理论并不是标度不变的。我们可以从量子电动力学的β函数中得到这一认识。这就告诉我们电荷(在理论上是耦合参数)随着能量的增加而增加。因此,尽管没有带电粒子的量子化电磁场是标度不变的,量子电动力学却不是标度不变的。
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然而在自然界中,电磁场是与带电粒子耦合的,比如电子。描述光子和带电粒子相互作用的量子场论是量子电动力学(QED),而这个理论并不是标度不变的。我们可以从量子电动力学的β函数中得到这一认识。这就告诉我们电荷(在理论上是耦合参数)随着能量的增加而增加。因此,尽管没有带电粒子的量子化电磁场是标度不变的,量子电动力学却不是标度不变的。
    
===Massless scalar field theory 无质量标量场理论===
 
===Massless scalar field theory 无质量标量场理论===
 
Free, massless [[scalar field (quantum field theory)|quantized scalar field theory]] has no coupling parameters. Therefore, like the classical version, it is scale-invariant. In the language of the renormalization group, this theory is known as the [[Gaussian fixed point]].
 
Free, massless [[scalar field (quantum field theory)|quantized scalar field theory]] has no coupling parameters. Therefore, like the classical version, it is scale-invariant. In the language of the renormalization group, this theory is known as the [[Gaussian fixed point]].
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Free, massless quantized scalar field theory has no coupling parameters. Therefore, like the classical version, it is scale-invariant. In the language of the renormalization group, this theory is known as the Gaussian fixed point.
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自由的、无质量的'''Quantized Scalar Field Theory 量子化标量场理论'''没有耦合参数。因此,像经典的版本一样,它是标度不变的。在重整化群的范畴中,这个理论称做'''Gaussian Fixed Point 高斯定点'''。
 
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自由的、无质量的量子化纯量场理论没有耦合参数。因此,像经典的版本一样,它是尺度不变的。在重整化群的语言中,这个理论被称为高斯不动点。
      
However, even though the classical massless ''φ''<sup>4</sup> theory is scale-invariant in ''D''=4, the quantized version is '''not''' scale-invariant. We can see this from the [[beta-function]] for the coupling parameter, ''g''.
 
However, even though the classical massless ''φ''<sup>4</sup> theory is scale-invariant in ''D''=4, the quantized version is '''not''' scale-invariant. We can see this from the [[beta-function]] for the coupling parameter, ''g''.
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However, even though the classical massless φ4 theory is scale-invariant in D=4, the quantized version is not scale-invariant. We can see this from the beta-function for the coupling parameter, g.
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然而,尽管经典的无质量''φ''<sup>4</sup>理论在''D''=4时是标度不变的,但量子化的版本却不是如此。我们可以从耦合参数''g''的β函数中看出这一点。
 
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然而,即使经典的无质量 φ4理论在 d = 4中是标度不变的,量化后的理论也不是标度不变的。我们可以从耦合参数 g 的 beta 函数中看到这一点。
      
Even though the quantized massless ''φ''<sup>4</sup> is not scale-invariant, there do exist scale-invariant quantized scalar field theories other than the Gaussian fixed point. One example is the '''Wilson-Fisher fixed point''', below.
 
Even though the quantized massless ''φ''<sup>4</sup> is not scale-invariant, there do exist scale-invariant quantized scalar field theories other than the Gaussian fixed point. One example is the '''Wilson-Fisher fixed point''', below.
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Even though the quantized massless φ4 is not scale-invariant, there do exist scale-invariant quantized scalar field theories other than the Gaussian fixed point. One example is the Wilson-Fisher fixed point, below.
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虽然量子化无质量''φ''<sup>4</sup>不是标度不变的,但除了高斯定点外,确实存在标度不变的量子化标量场理论。例如:'''Wilson-Fisher Fixed Point 威尔逊-费雪定点'''
 
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尽管量子化的无质量 φ4不具有尺度不变性,但除了高斯不动点理论外,还存在尺度不变量子化标量场理论。一个例子是下面的 Wilson-Fisher 定点。
      
===Conformal field theory 共形场论===
 
===Conformal field theory 共形场论===
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