scholarly journals Vector mesons on the light front

2004 ◽  
Vol 583 (1-2) ◽  
pp. 87-95 ◽  
Author(s):  
K. Naito ◽  
S. Maedan ◽  
K. Itakura
Keyword(s):  
2021 ◽  
Vol 104 (9) ◽  
Author(s):  
Chao Shi ◽  
Ya-Ping Xie ◽  
Ming Li ◽  
Xurong Chen ◽  
Hong-Shi Zong

2015 ◽  
Vol 93 (9) ◽  
pp. 947-951
Author(s):  
M.R. Ahmady ◽  
S. Lord ◽  
R. Sandapen

Light front holography is a formalism developed by Brodsky and de Téramond in which analytic forms for the hadronic bound state wavefunctions can be obtained. We have used the holographic light front wavefunctions thus obtained to calculate the distribution amplitudes of the light vector mesons ρ and K∗. As a result, we are able to calculate the form factors for B → ρ, K∗ transitions as well as ΛQCD/mb contributions in radiative B(s) → (ρ, K∗)γ decays. We compare our predictions to the available experimental data.


2003 ◽  
Vol 67 (11) ◽  
Author(s):  
Bernard L. G. Bakker ◽  
Ho-Meoyng Choi ◽  
Chueng-Ryong Ji

2008 ◽  
Author(s):  
Alessandro Papa ◽  
Francesco Caporale ◽  
Augustin Sabio Vera

2007 ◽  
Vol 57 (3) ◽  
Author(s):  
L'ubomír Martinovič

Light front field theory: An advanced PrimerWe present an elementary introduction to quantum field theory formulated in terms of Dirac's light front variables. In addition to general principles and methods, a few more specific topics and approaches based on the author's work will be discussed. Most of the discussion deals with massive two-dimensional models formulated in a finite spatial volume starting with a detailed comparison between quantization of massive free fields in the usual field theory and the light front (LF) quantization. We discuss basic properties such as relativistic invariance and causality. After the LF treatment of the soluble Federbush model, a LF approach to spontaneous symmetry breaking is explained and a simple gauge theory - the massive Schwinger model in various gauges is studied. A LF version of bosonization and the massive Thirring model are also discussed. A special chapter is devoted to the method of discretized light cone quantization and its application to calculations of the properties of quantum solitons. The problem of LF zero modes is illustrated with the example of the two-dimensional Yukawa model. Hamiltonian perturbation theory in the LF formulation is derived and applied to a few simple processes to demonstrate its advantages. As a byproduct, it is shown that the LF theory cannot be obtained as a "light-like" limit of the usual field theory quantized on an initial space-like surface. A simple LF formulation of the Higgs mechanism is then given. Since our intention was to provide a treatment of the light front quantization accessible to postgradual students, an effort was made to discuss most of the topics pedagogically and a number of technical details and derivations are contained in the appendices.


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