Perturbative Approach > s.a. Feynman
Diagram; renormalization;
series.
* Idea: Methods that
allow us to calculate amplitudes for processes as power series in the strength
of the
interaction; They are approximate methods that work well except for non-linear
fields in strong-field situations.
* Types: One normally
uses covariant perturbation theory, but light front and others are also possible;
Causal perturbation theory is an approach in which a specific causality condition
is imposed at every order of perturbation theory and divergent integrals are
avoided from the outset.
* Loop expansions: Tree
diagrams are normally associated with classical physics, while loop effects
are considered quantum
mechanical
in nature; This is not always the case.
* Remark: Renormalizability
does not imply superrenormalizability.
@ General references: Fischer IJMPA(97)
[rev]; Kastening & Kleinert PLA(00)qp/99 [calculation
of Feynman integrals]; Sterman IJMPA(01)
[intro]; Schubert PRP(01)
[string-inspired]; Dunne ht/02-in
[and
non-perturbative];
Holstein & Donoghue PRL(04)
[tree diagrams vs loop effects]; Szabo ht/05-in
[intro]; Hollands a0802 [consistency
conditions framework]; Stora IJGMP(08),
a0901 [renormalized];
Kreimer a0909-in [algebraic structure].
@ Divergences, infinities: Jackiw in(00);
Hurst RPMP(06)
[history]; Sharatchandra a0707 [proposal
for divergence-free approach]; Weinberg a0903.
@ And algebraic quantum field theory: Dütsch & Fredenhagen CMP(01)ht/00;
Bergbauer
& Kreimer
a0704-in.
@ Perturbatively non-renormalizable theories: Paban et al ZPC(87); Gegelia & Japaridze
IJTP(00)ht/98 [new
method].
@ Causal perturbation theory: Aste & Trautmann CJP(03)ht [UV
finite results]; Grangé & Werner qp/06;
Aste a0810-in;
Aste et al a0906 [examples].
@ Schemes: Bender et al PRD(88), & Jones
JMP(88),
follow-up Brown PRD(88);
Schoonderwoerd & Bakker
PRD(98), PRD(98)
[covariant and light front]; Meurice PRL(02)
[improved method]; Holstein & Donoghue PRL(04)ht [loop
vs
expansions]; Weinstein
NPPS(06)ht/05
[adaptive]; Frasca NPPS(09)-a0807 [strong-coupling
expansion]; Hollands & Olbermann a0906 [in
terms of vertex algebras].
> Related topics:
see deformation quantization; fock
space; instanton [including WKB]; S-Matrix; scattering;
Time Slice Axiom.
Non-Perturbative Features > s.a. locality
and localization; renormalization;
symmetry breaking.
@ General references: Rajaraman PRP(75);
Gervais & Neveu PRP(76);
Brézin & Gervais
PRP(79);
Fröhlich 91; Ferrara ht/96-in;
Borne et al 01 [and structure of matter]; Frishman & Sonnenschein 10.
@ Non-local configurations: Visser PLA(03)ht [covariant wavelets]; > s.a.
instanton; monopole; soliton;
Sphaleron.
@ Approaches: Bender et al JMP(90) [
expansion]; Turner
PhD(96)ht/01;
Ksenzov PLB(97)
[vacuum]; Dzhunushaliev & Singleton
IJTP(99)ht/98;
Salwen & Lee PRD(00)ht/99 [1+1
4];
Kizilersu et al PLB(01)ht/00;
> s.a. other approaches [loop quantization].
Other Techniques and Concepts > s.a. approaches [formulations]; canonical
quantum mechanics; path integrals; stochastic
quantum mechanics.
@ Probabilistic: Damgaard et al ed-90; Garbaczewski et al PRE(95)qp;
Man'ko et al PLB(98)ht [probability representation].
@ Euclidean field theory: Guerra mp/05; > s.a. Wick
Rotation
@ Covariant Schrödinger formalism: Freese et al NPB(85); Kyprianidis
PRP(87).
@ Hamiltonian light front: Allen ht/99-PhD;
Ullrich JMP(04).
@
Related topics: Clarke IJTP(79), JPA(90)
[group bundle theories]; Carey PLB(87)
[cocycles]; Aldaya et al JPA(88)
[group manifolds]; Gitman & Tyutin CQG(90)
[from first quantization]; deLyra et al PRD(91)
[lattice, differentiability]; Lam JMP(98)ht,
ht/98-in
[integrals of time-ordered products]; Oehme ht/00-in
[reduction of parameters]; Neumaier
gq/03; Shajesh & Milton ht/05 [Fradkin's
representation]; Jaffe & Jäkel CMP(06)
[exchange identity for non-linear bosonic fields]; Nikolic EPL(09)-a0705 [in
terms of integral curves of particle currents]; Piazza & Costa a0711 [regions
as subsystems]; Villalba-Chavez et al a0807 [Hamiltonian
vs Lagrangian formalisms]; Stoyanovsky a0810 [definition
of dynamical evolution].
> Techniques:
see Coarse-Graining; cohomology
theories; Colombeau Algebra; effective
quantum field theory; field theory [current
algebra]; green functions; Hopf
Algebra; Motives; quantum
feld theory [including
beable-based pilot-wave]; regularization; renormalization;
Wavelets.
> Related concepts:
see boundaries; bundle [gerbe];
complex structure;
Determinant; Dirac
Sea; distributions [products]; Elliptic
Genera; K-Theory; lattice
field theory; N-Point
Functions; representations [and pictures]; resonance; Schwinger-Dyson
Equation; states; symplectic
structures.
Features > s.a. angular
momentum; anomalies; arrow
of time; causality; interpretations
of quantum mechanics; quantum
chaos; topology.
* Linearity: We can have
kinematical linearity (the space of fields is linear), and dynamical non-linearity
(field equations), e.g. in ![]()
4
scalar
field theories; For non-Abelian theories or gravity, on the other hand,
there
are already kinematical non-linearities; Traditionally,
non-linear fields have been treated only perturbatively, although non-perturbative
techniques are being developed, especially for gravity; > s.a. axiomatic
approach.
@ Particle production: Srinivasan & Padmanabhan PRD(99)gq/98, gq/99;
Prodan JPA(99)mp;
Nikolic ht/01;
Haro IJTP(03)
[charged Klein-Gordon in electric field]; > s.a.
quantum field theory effects in curved spacetime.
@ Radiative corrections: Jackiw IJMPB(00)ht/99.
@ Infrared limit: Mansfield ht/96-in
[large distance expansion]; Kjaergaard & Mansfield
JHEP(00)ht/99.
main page – abbreviations – journals – comments – other
sites – acknowledgements
send feedback and suggestions to bombelli at olemiss.edu – modified 11
oct
2009