Dimensional regularization

Dimensional regularization

In theoretical physics, dimensional regularization is a method introduced by Giambiagi and Bollini for regularizing integrals in the evaluation of Feynman diagrams; in other words, assigning values to them that are meromorphic functions of an auxiliary complex parameter d, called (somewhat confusingly) the dimension.

Dimensional regularization writes a Feynman integral as an integral depending on the spacetime dimension d and the squared distances (xixj)2 of the spacetime points xi, ... appearing in it. In Euclidean space, the integral often converges for −Re(d) sufficiently large, and can be analytically continued from this region to a meromorphic function defined for all complex d. In general, there will be a pole at the physical value (usually 4) of d, which needs to be canceled by renormalization to obtain physical quantities. Etingof (1999) showed that dimensional regularization is mathematically well defined, at least in the case of massive Euclidean fields, by using the Bernstein–Sato polynomial to carry out the analytic continuation.

There is a tradition of confusing the parameter d appearing in dimensional regularization, which is a complex number, with the dimension of spacetime, which is a fixed positive integer (such as 4). The reason is that if d happens to be a positive integer, then the formula for the dimensionally regularized integral happens to be correct for spacetime of dimension d. For example, the volume of a unit (d − 1)-sphere is \frac{2\pi^{d/2}}{\Gamma\left(\frac{d}{2}\right)} where Γ is the gamma function when d is a positive integer, so in dimensional regularization it is common to say that this is the volume of a sphere in d dimensions even when d is not an integer. This is a useful mnemonic for remembering the formulas in dimensional regularization, but is otherwise meaningless as there is no such thing as a sphere in non-integral dimensions. This failure to distinguish between the dimension of spacetime and the formal parameter d has led to a lot of meaningless speculation about (non-existent) spacetimes of non-integral dimension.

If one wishes to evaluate a loop integral which is logarithmically divergent in four dimensions, like

\int\frac{d^dp}{(2\pi)^d}\frac{1}{\left(p^2+m^2\right)^2},

one first rewrites the integral in some way so that the number of variables integrated over does not depend on d, and then we formally vary the parameter d, to include non-integral values like d = 4 − ε.

This gives

\lim_{\varepsilon\rightarrow 0^+}\int \frac{dp}{(2\pi)^{4-\varepsilon}} \frac{2\pi^{(4-\varepsilon)/2}}{\Gamma\left(\frac{4-\varepsilon}{2}\right)} \frac{p^{3-\varepsilon}}{\left(p^2+m^2\right)^2}=\lim_{\varepsilon\rightarrow 0^+}\frac{\pi^\varepsilon (1-\varepsilon)}{16 \pi \cos(\pi\varepsilon) \Gamma(2-\varepsilon)}m^{-2 \varepsilon}=\frac{1}{16\pi}.

Emilio Elizalde has shown that both Zeta regularization and dimensional regularization are equivalent since they use the same principle of using analytic continuation in order for a series or integral to converge.

See also

References


Wikimedia Foundation. 2010.

Игры ⚽ Нужен реферат?

Look at other dictionaries:

  • Regularization (physics) — In physics, especially quantum field theory, regularization is a method of dealing with infinite, divergent, and non sensical expressions by introducing an auxiliary concept of a regulator (for example, the minimal distance epsilon in space which …   Wikipedia

  • Pauli-Villars regularization — In theoretical physics, Pauli Villars regularization is a procedure that isolates divergent terms from finite parts in loop calculations in field theory in order to renormalize the theory. Wolfgang Pauli and Felix Villars published the method in… …   Wikipedia

  • Tikhonov regularization — Tikhonov regularization, named for Andrey Tikhonov, is the most commonly used method of regularization of ill posed problems. In statistics, the method is known as ridge regression, and, with multiple independent discoveries, it is also variously …   Wikipedia

  • Zeta function regularization — In mathematics and theoretical physics, zeta function regularization is a type of regularization or summability method that assigns finite values to superficially divergent sums. The technique is now commonly applied to problems in physics, but… …   Wikipedia

  • Renormalization — Quantum field theory (Feynman diagram) …   Wikipedia

  • Butcher group — In mathematics, the Butcher group, named after the New Zealand mathematician John C. Butcher by Hairer Wanner (1974), is an infinite dimensional group first introduced in numerical analysis to study solutions of non linear ordinary differential… …   Wikipedia

  • Generalized function — In mathematics, generalized functions are objects generalizing the notion of functions. There is more than one recognised theory. Generalized functions are especially useful in making discontinuous functions more like smooth functions, and (going …   Wikipedia

  • BRST quantization — In theoretical physics, BRST quantization (where the BRST refers to Becchi, Rouet, Stora and Tyutin) is a relatively rigorous mathematical approach to quantizing a field theory with a gauge symmetry. Quantization rules in earlier QFT frameworks… …   Wikipedia

  • Deriving the volume of an n-ball — In geometry, the volume of a sphere is a special case of the n dimensional volume of a ball in n dimensional Euclidean space. Contents 1 Derivation of the volume of an n ball 1.1 Base cases 1.2 General case …   Wikipedia

  • List of mathematics articles (D) — NOTOC D D distribution D module D D Agostino s K squared test D Alembert Euler condition D Alembert operator D Alembert s formula D Alembert s paradox D Alembert s principle Dagger category Dagger compact category Dagger symmetric monoidal… …   Wikipedia

Share the article and excerpts

Direct link
Do a right-click on the link above
and select “Copy Link”