Comparing light-front quantization with instant-time quantization

نویسندگان

چکیده

In this paper we compare light-front quantization and instant-time both at the level of operators their Feynman diagram matrix elements. At lead to equal time commutation (or anticommutation) relations that appear be quite different from relations. Despite show unequal times actually can transformed into each other, with it only being restriction makes so different. While our results are valid for bosons fermions, fermions there subtleties associated tip light cone contributions need taken care of. diagrams non-vacuum pole terms in four-dimensional reproduce widely used three-dimensional on-shell Hamiltonian Fock space formulation which energy momentum on shell. Moreover, equal. However, because circle infinity equivalence fails vacuum tadpole diagrams. Then, precisely these contributions, not nonzero, they remarkably pure term Light-front correctly describable by formalism, thus closely related infinite frame prescription either. Thus sector must use off-shell formalism as contains information is accessible approach. We intrinsically nonlocal, nonlocality present Ward identities. One project fermion spinors so-called good bad components, components contribute Central analysis transformation coordinates fields a unitary, spacetime-dependent translation. Consequently, equivalent, general coordinate invariance unitarily equivalent.

برای دانلود رایگان متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

Light Front Quantization

An introductory overview on Light-Front quantization, with some emphasis on recent achievements, is given. Light-Front quantization is the most promising and physical tool to study deep inelastic scattering on the basis of quark gluon degrees of freedom. The simplified vacuum structure (nontrivial vacuum effects can only appear in zero-mode degrees of freedom) and the physical basis allows for ...

متن کامل

Light - Front Quantization of Gauge Theories ∗

Light-front wavefunctions provide a frame-independent representation of hadrons in terms of their physical quark and gluon degrees of freedom. The light-front Hamiltonian formalism provides new nonperturbative methods for obtaining the QCD spectrum and eigensolutions, including resolvant methods, variational techniques, and discretized light-front quantization. A new method for quantizing gauge...

متن کامل

For Review O nly Light Front Quantization

The Dirac procedure for dealing with constraints is applied to the quantization of gauge theories on the light front. The light cone gauge is used in conjunction with the first class constraints that arise and the resulting Dirac brackets are found. These gauge conditions are not used to eliminate degrees of freedom from the action prior to applying the Dirac constraint procedure. This approach...

متن کامل

Light-front Quantization and Qcd Phenomena∗

The light-front quantization of QCD provides an alternative to lattice gauge theory for computing the mass spectrum, scattering amplitudes, and other physical properties of hadrons directly in Minkowski space. Nonperturbative light-front methods for solving gauge theory and obtaining light-front wavefunctions, such as discretized light-front quantization, the transverse lattice, and light-front...

متن کامل

Electron Anomalous Magnetic Moment in Basis Light-Front Quantization Approach

We apply the Basis Light-Front Quantization (BLFQ) approach to the Hamiltonian field theory of Quantum Electrodynamics (QED) in free space. We solve for the mass eigenstates corresponding to an electron interacting with a single photon in light-front gauge. Based on the resulting non-perturbative ground state light-front amplitude we evaluate the electron anomalous magnetic moment. The numerica...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

ژورنال

عنوان ژورنال: Physics Reports

سال: 2021

ISSN: ['0370-1573', '1873-6270']

DOI: https://doi.org/10.1016/j.physrep.2020.09.001