glueball mass
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2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Sergei Dubovsky ◽  
Guzmán Hernández-Chifflet ◽  
Shahrzad Zare

Abstract Recent lattice results strongly support the Axionic String Ansatz (ASA) for quantum numbers of glueballs in 3D Yang-Mills theory. The ASA treats glueballs as closed bosonic strings. The corresponding worldsheet theory is a deformation of the minimal Nambu-Goto theory. In order to understand better the ASA strings and as a first step towards a perturbative calculation of the glueball mass splittings we compare the ASA spectrum to the closed effective string theory. Namely, we model glueballs as excitations around the folded rotating rod solution with a large angular momentum J. The resulting spectrum agrees with the ASA in the regime of validity of the effective theory, i.e., in the vicinity of the leading Regge trajectory. In particular, closed effective string theory correctly predicts that only glueballs of even spin J show up at the leading Regge trajectory. Interestingly though, the closed effective string theory overestimates the number of glueball states far above the leading Regge trajectory.


Author(s):  
E. V. Souza ◽  
M. N. Ferreira ◽  
A. C. Aguilar ◽  
J. Papavassiliou ◽  
C. D. Roberts ◽  
...  
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2019 ◽  
Vol 790 ◽  
pp. 410-414 ◽  
Author(s):  
Amir H. Fariborz ◽  
Renata Jora

2018 ◽  
Vol 175 ◽  
pp. 08013 ◽  
Author(s):  
Ed Bennett ◽  
Deog Ki Hong ◽  
Jong-Wan Lee ◽  
C.-J. David Lin ◽  
Biagio Lucini ◽  
...  

As a first step in the study of Sp(2N) composite Higgs models, we obtained a set of novel numerical results for the pure gauge Sp(4) lattice theory in 3+1 space-time dimensions. Results for the continuum extrapolations of the string tension and the glueball mass spectrum are presented and their values are compared with the same quantities in neighbouring SU(N) models.


2014 ◽  
Vol 732 ◽  
pp. 247-254 ◽  
Author(s):  
D. Dudal ◽  
M.S. Guimaraes ◽  
S.P. Sorella

2010 ◽  
Vol 82 (3) ◽  
Author(s):  
Christopher M. Richards ◽  
Alan C. Irving ◽  
Eric B. Gregory ◽  
Craig McNeile

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