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The Coexistence of a 't Hooft-Polyakov Monopole and a One-Half Monopole

机译:'t Hooft-polyakov monopole和一半单极的共存

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Recently we have reported on the existence of finite energy SU(2) Yang-Mills-Higgs particle of one-half topological charge. In this paper, we show that this one-half monopole can co-exist with a 't Hooft-Polyakov monopole. The magnetic charge of the one-half monopole is -1/2 while the magnetic charge of the 't Hooft-Polyakov monopole is positive unity. However the net magnetic charge of the configuration is zero due to the presence of a semi-infinite Dirac string along the positive z-axis that carries the magnetic monopole charge of another -1/2. The solution possesses gauge potentials that are singular along the z-axis, elsewhere they are regular. This monopole configuration possesses finite total energy and magnetic dipole moment. The total energy is found to increase with the strength of the Higgs field self-coupling constant λ. However the dipole separation and the magnetic dipole moment decrease with λ. This solution is non-BPS even in the BPS limit when the Higgs self-coupling constant vanishes.
机译:最近我们报道了有限能源Su(2)阳米尔斯 - Higgs粒子的一半拓扑电荷。在本文中,我们表明,这一半单极可以与“T Hooft-Polyakov Monopole共存。一半单极的磁性电荷为-1/2,而“T Hooft-Polyakov单极的磁性电荷是正统的。然而,由于沿着沿着另一个-1/2的磁性单极电荷的正Z轴存在半无限Dirac串,所属配置的净磁电荷为零。该解决方案具有沿Z轴的单数的规格电位,在其他地方定期。这种单极配置具有有限的总能量和磁性偶极矩。发现总能量随着HIGGS场自耦合常数λ的强度而增加。然而,偶极分离和磁性偶极力矩随λ降低。当HIGGS自耦合恒定消失时,该解决方案即使在BPS限制中也是非BPS。

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