Construction of Hamiltonian for interacting optical fields

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SUMMARY

The discussion centers on constructing the Hamiltonian for interacting optical fields, specifically for a two-mode nonlinear optical coupler. The Hamiltonian is expressed as H = hω(a1b1 + a2b2) + hωg(a1^2b1^2 + a2^2b2^2) + hk(a1b2 + b1a2), where h is the Planck constant, ω is the angular frequency, and g represents the nonlinear susceptibility. A recommended resource is "Optical Coherence & Quantum Optics" by Mandel & Wolf, which provides foundational knowledge and similar Hamiltonian forms relevant to nonlinear optics.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with nonlinear optics concepts
  • Knowledge of Hamiltonian mechanics
  • Basic grasp of optical field operators (creation and annihilation operators)
NEXT STEPS
  • Study the Hamiltonian formulation in nonlinear optics using "Optical Coherence & Quantum Optics" by Mandel & Wolf
  • Explore the derivation of Hamiltonians for nonlinear optical systems
  • Research the physical implications of nonlinear susceptibility in optical couplers
  • Investigate harmonic generation in nonlinear media as described in relevant literature
USEFUL FOR

This discussion is beneficial for MSc students in nonlinear quantum optics, researchers in quantum mechanics, and anyone interested in the theoretical aspects of optical fields and their interactions.

Api
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Hi. I am going to start my MSc in a couple of months majoring in nonlinear quantum optics. I have a good basic in quantum mechanics, but have never looked at quantum optics before. My topic will be to investigate quantum properties of nonlinear optical coupler but i have problem with the construction of the Hamiltonian for interacting optical fields. For starting, i start with two mode nonlinear optical coupler

H= hω(a1b1+a2b2)+hωg(a1^2 b1^2+a2^2 b2^2) + hk(a1b2+b1a2)

h=planck constant (h bar)
ω=angular frequency
an= creation operator associated with the optical mode
bn=annihilation operator associated with the optical mode
g=nonlinear susceptibility
k= coupling constant

I will really appreciate it if anyone can explain the physical meaning of this Hamiltonian and how do we construct such equation to describe the system.
 
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Api said:
Hi. I am going to start my MSc in a couple of months majoring in nonlinear quantum optics. I have a good basic in quantum mechanics, but have never looked at quantum optics before. My topic will be to investigate quantum properties of nonlinear optical coupler [...]

If you never looked at quantum optics, then definitely get a copy of Mandel & Wolf, "Optical Coherence & Quantum Optics" asap. Some have described it as a "bible" of this subject. (I'm no expert on it, but I can say that it's a surprisingly interesting subject after one gets into it a bit.)

In a 30-sec search, I didn't find the exact Hamiltonian that you wrote, but something similar appears in eq(22.3-1) of M&W which deals with harmonic generation in nonlinear media.
<br /> H= \sum_{i=1}^2 \hbar \omega(n_i + 1/2)<br /> ~+~ \hbar g \left(a^\dagger_2 a_1^2 + {a^\dagger_1}^2 a_2 \right)<br />
The preceding section 22.2 (Energy of the field in a dielectric) gives some of the motivation for the form of this Hamiltonian, but note that this is in ch22 and there's lots of stuff earlier in the book that you'd need to make sure you understand before diving into the above.
 
ok.thanks for the reply
 

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