A Jaynes-Cummings Hamiltonian: Where did the time dependence go?

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The discussion centers on the Jaynes-Cummings Hamiltonian and its time dependence in the context of a two-level atom interacting with an electric field. It highlights the contrast between the semiclassical Hamiltonian, which is time-dependent, and the Jaynes-Cummings Hamiltonian, which appears time-independent. Participants question how to transition to the interaction picture with a constant Hamiltonian and explore the implications of energy conservation in a closed system. The conversation also touches on the quantization of the field and the disappearance of time dependence in the Schrödinger picture. Ultimately, the participants seek clarity on the relationship between quantization, time dependence, and energy conservation in this framework.
yucheng
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Semiclassically, the electric field varies harmonically in time, but sometimes, in the JC Hamiltonian, the time dependence disappears. What???
Consider the interaction of a two level atom and an electric field (semiclassically, we treat the field as 'external' i.e. not influenced by the atom; the full quantum treats the change in the field as well)

Electric field in semiclassical Hamiltonian: plane wave

##H_{int,~semiclassical}=-\mu \cdot E=-\mu \cdot E_{0}\cos \nu t##

Electric field in Jaynes-Cummings Hamiltonian, single mode i.e. plane wave
(Schrodinger picture)

##H_{int}=\hbar g(\sigma _{+}a+\sigma _{-}a^{\dagger })##

\bigskip

We realize ##H_{int}## is time independent! So where did the time-harmonic
dependence go? How does this compare to the classical case?

Also, how are we supposed to go to the interaction picture, with a constant
hamiltonian?

Furthermore, ##H_{int,~semiclassical}## is time-dependent, but isn't this the
Schrodinger picture Hamiltonian? Shouldn't it be time-independent?

Possibly related: Sakurai and Napolitano, Modern Quantum Mechanics: constant
perturbation turned on at t=0!?

Also see:
https://www.physicsforums.com/threa...hen-the-hamiltonian-is-time-dependent.971007/
 
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It is also possible to add a time-dependent drive term to the J-C Hamiltonian.
However, in the simples case you have a situation where the energy is continuously moving between the cavity and the two-level systems; i.e. it is a closed system and there is no real time-dependence.

Note that the J-C Hamiltonian in the "strong driving" regime gets really complicated.
 
Demystifier said:
In the JC Hamiltonian, the field is quantized. It's not a semiclassical approximation.
Yes I understand that it's quantized, but... why must find dependence disappear if it's quantized?

f95toli said:
it is a closed system and there is no real time-dependence.
Perhaps this is a good hint. Closed system=energy conservation=no time dependence, but:
How do we know if the system is closed?
Why no time dependence=energy conservation?....
 
yucheng said:
Yes I understand that it's quantized, but... why must find dependence disappear if it's quantized?
Because the time dependence of operators usually disappears in the Schrodinger picture.
 
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