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Related Concept Videos

Paramagnetism01:30

Paramagnetism

Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
Magnetic Susceptibility and Permeability01:31

Magnetic Susceptibility and Permeability

In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
Magnetic Fields01:27

Magnetic Fields

A moving charge or a current creates a magnetic field in the surrounding space, in addition to its electric field. The magnetic field exerts a force on any other moving charge or current that is present in the field. Like an electric field, the magnetic field is also a vector field. At any position, the direction of the magnetic field is defined as the direction in which the north pole of a compass needle points.
A magnetic field is defined by the force that a charged particle experiences...
Magnetic Flux01:18

Magnetic Flux

The magnetic flux measures the number of magnetic field lines passing through a given surface area. The SI unit for magnetic flux is the weber (Wb). Magnetic flux is a scalar quantity. It depends on three factors: the strength of the magnetic field B, the area through which the field lines pass, and the relative orientation of the field with the surface area.
Suppose a surface is divided into elements of area dA. For each element, the component of the magnetic field that is normal to the...
Magnetic Field Due To A Thin Straight Wire01:27

Magnetic Field Due To A Thin Straight Wire

Consider an infinitely long straight wire carrying a current I. The magnetic field at point P at a distance a from the origin can be calculated using the Biot-Savart law.
Diamagnetism01:26

Diamagnetism

Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets.

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Magnetic S parameter.

Francesco Sannino1

  • 1CP3-Origins, Campusvej 55, DK-5230 Odense M, Denmark. sannino@cp3.sdu.dk

Physical Review Letters
|January 15, 2011
PubMed
Summary

This study introduces a direct test for gauge duals in nonsupersymmetric theories by calculating the S parameter. Results support a universal lower bound for the S parameter, aiding in counting degrees of freedom.

Area of Science:

  • High Energy Physics
  • Quantum Field Theory
  • String Theory

Background:

  • Nonsupersymmetric asymptotically free gauge theories with an infrared fixed point are crucial in understanding fundamental forces.
  • Gauge duality offers a powerful tool to study strongly coupled quantum field theories.
  • The S parameter is a key observable for probing the properties of these theories.

Purpose of the Study:

  • To propose and perform a direct test for the existence of gauge duals in four-dimensional nonsupersymmetric gauge theories.
  • To compute the S parameter in both electric and dual magnetic descriptions.
  • To investigate the implications of the results for a conjectured universal lower bound on the S parameter.

Main Methods:

  • Calculation of the S parameter in the electric description of the gauge theory.

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  • Computation of the S parameter in the dual magnetic description.
  • Analysis of the S parameter at the lower bound of the conformal window.
  • Main Results:

    • A direct test for gauge duals in nonsupersymmetric gauge theories is proposed.
    • The magnetic S parameter at the lower bound of the conformal window is expressed in terms of elementary magnetic degrees of freedom.
    • The results provide further support for a universal lower bound on the S parameter.

    Conclusions:

    • The S parameter is identified as an ideal operator for counting physical degrees of freedom within the conformal window.
    • The study presents the first explicit computation of a nonperturbative quantity in electric variables using nonsupersymmetric gauge duality.
    • The findings pave the way for uncovering four-dimensional gauge duals and understanding strongly coupled nonsupersymmetric theories.