Math 2.0

Optics, electromagnetic theory Definition

Maxwell–Bloch equations

Builds on Maxwell's equationsPolarization densitySolution of an ordinary differential equationLaser rate equations

Definition

Consider a single-mode laser cavity filled with identical two-level atoms whose transition is resonant with the mode. Let E(t)E(t) be the real amplitude of the field, P(t)P(t) the real amplitude of the atomic polarization, and D(t)D(t) the population inversion, in suitable units. Let κ>0\kappa > 0, γ⊥>0\gamma_\perp > 0 and γ∥>0\gamma_\parallel > 0 be the decay rates of the field, the polarization and the inversion. Let D0D_0 be the inversion set by the pump, and g>0g > 0 the coupling constant. In one common normalization, the Maxwell–Bloch equations for this laser are the system of ordinary differential equations dEdt=−κE+gP,dPdt=−γ⊥P+gED,dDdt=−γ∥(D−D0)−4gEP.\frac{dE}{dt} = -\kappa E + g P, \qquad \frac{dP}{dt} = -\gamma_\perp P + g E D, \qquad \frac{dD}{dt} = -\gamma_\parallel (D - D_0) - 4 g E P.

Remarks

The first equation comes from Maxwell's equations in the cavity, with the polarization as source. The other two are the optical Bloch equations of the atoms driven by the field. Without damping and pumping, the quantity P2+D2/4P^2 + D^2/4 is conserved, which is the conservation of the length of the Bloch vector. In travelling-wave problems, the field equation is a partial differential equation in space and time instead.

Example: E=P=0E = P = 0, D=D0D = D_0 is always a steady state, the laser off. For D0>κγ⊥/g2D_0 > \kappa \gamma_\perp / g^2 there are also steady states with E≠0E \ne 0 and D=κγ⊥/g2D = \kappa \gamma_\perp / g^2, the laser on.

Non-example: the laser rate equations are not Maxwell–Bloch equations, since they contain no equation for the polarization PP. They follow from the Maxwell–Bloch equations when γ⊥\gamma_\perp is much larger than the other rates and PP is eliminated.

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  1. Laser rate equations concept
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Further reading

  1. Web https://en.wikipedia.org/wiki/Maxwell%E2%80%93Bloch_equations
About this page
TagFMF327F0MV
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Kinddefinition
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MSC78A60, 81V80
DefinesMaxwell–Bloch equations
UsesMaxwell's equations, Polarization density, Solution of an ordinary differential equation, Laser rate equations
Changed3 November 2026

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