scholarly journals Spectrum of very excited Σg+ flux tubes in SU(3) gauge theory

2021 ◽  
Vol 104 (5) ◽  
Author(s):  
P. Bicudo ◽  
N. Cardoso ◽  
A. Sharifian
Keyword(s):  
2000 ◽  
Vol 15 (28) ◽  
pp. 4407-4415 ◽  
Author(s):  
N. AMER ◽  
E. I. GUENDELMAN

Flux tube solutions are found in the square root gauge theory. Purely magnetic solutions exist which do not contain radiation. It is found that no electric monopole solution exists, which is a sign of electric charge confinement, but magnetic monopole solutions exist and therefore there is no confinement of magnetic charge. There are also solutions which have both electric and magnetic components and represent flux tubes where in addition some radiation process, caused for example by some annihilation in the center of the tube takes place. Finally, there are solutions with both electric and magnetic field which do not represent radiation but rather electric flux tubes, which are good candidates for describing confinement of oppositely charged sources. Demanding angular momentum quantization leads to the quantization of the length of these tubes.


2005 ◽  
Vol 20 (15) ◽  
pp. 3481-3487 ◽  
Author(s):  
VLADIMIR DZHUNUSHALIEV ◽  
DOUGLAS SINGLETON ◽  
DANNY DHOKARH

In the present work we show that it is possible to arrive at a Ginzburg-Landau (GL) like equation from pure SU (2) gauge theory. This has a connection to the dual superconducting model for color confinement where color flux tubes permanently bind quarks into color neutral states. The GL Lagrangian with a spontaneous symmetry breaking potential, has such (Nielsen-Olesen) flux tube solutions. The spontaneous symmetry breaking requires a tachyonic mass for the effective scalar field. Such a tachyonic mass term is obtained from the condensation of ghost fields.


1998 ◽  
Vol 529 (1-2) ◽  
pp. 505-522 ◽  
Author(s):  
Martin Zach ◽  
Manfried Faber ◽  
Peter Skala

2005 ◽  
Vol 20 (22) ◽  
pp. 1695-1702
Author(s):  
AMITABHA LAHIRI

We propose a way of unambiguously parallel transporting fields on non-Abelian flux tubes, or strings, by means of two gauge fields. One gauge field transports along the tube, while the other transports normal to the tube. Ambiguity is removed by imposing an integrability condition on the pair of fields. The construction leads to a gauge theory of mathematical objects known as Lie 2-groups, which are known to result also from the parallel transport of the flux tubes themselves. The integrability condition is also shown to be equivalent to the assumption that parallel transport along nearby string configurations are equal up to arbitrary gauge transformations. Attempts to implement this condition in a field theory leads to effective actions for two-form fields.


1987 ◽  
Vol 35 (10) ◽  
pp. 3219-3224 ◽  
Author(s):  
J. B. Bronzan

1995 ◽  
Vol 51 (9) ◽  
pp. 5165-5198 ◽  
Author(s):  
Gunnar S. Bali ◽  
Christoph Schlichter ◽  
Klaus Schilling

2019 ◽  
Vol 100 (5) ◽  
Author(s):  
Lasse Müller ◽  
Owe Philipsen ◽  
Christian Reisinger ◽  
Marc Wagner

1994 ◽  
Vol 144 ◽  
pp. 503-505
Author(s):  
R. Erdélyi ◽  
M. Goossens ◽  
S. Poedts

AbstractThe stationary state of resonant absorption of linear, MHD waves in cylindrical magnetic flux tubes is studied in viscous, compressible MHD with a numerical code using finite element discretization. The full viscosity tensor with the five viscosity coefficients as given by Braginskii is included in the analysis. Our computations reproduce the absorption rates obtained by Lou in scalar viscous MHD and Goossens and Poedts in resistive MHD, which guarantee the numerical accuracy of the tensorial viscous MHD code.


Author(s):  
J. Bonevich ◽  
D. Capacci ◽  
G. Pozzi ◽  
K. Harada ◽  
H. Kasai ◽  
...  

The successful observation of superconducting flux lines (fluxons) in thin specimens both in conventional and high Tc superconductors by means of Lorentz and electron holography methods has presented several problems concerning the interpretation of the experimental results. The first approach has been to model the fluxon as a bundle of flux tubes perpendicular to the specimen surface (for which the electron optical phase shift has been found in analytical form) with a magnetic flux distribution given by the London model, which corresponds to a flux line having an infinitely small normal core. In addition to being described by an analytical expression, this model has the advantage that a single parameter, the London penetration depth, completely characterizes the superconducting fluxon. The obtained results have shown that the most relevant features of the experimental data are well interpreted by this model. However, Clem has proposed another more realistic model for the fluxon core that removes the unphysical limitation of the infinitely small normal core and has the advantage of being described by an analytical expression depending on two parameters (the coherence length and the London depth).


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