Continuous-variable cat state - phonon number mean and variance

In summary, the mean and second moment of the photon number for a coherent state can be expressed as $$\langle n\rangle=\vert\alpha\vert^2 \tanh(\alpha^2)$ and $\langle n^2\rangle=\vert\alpha\vert^2 \left( \alpha^2\sech(\alpha^2)^2 + \tanh(\alpha^2) \right)$, respectively. While there is no direct reference that contains these exact expressions, they can be found in the context of coherent states in various sources such as Ref. 1, 2, and 3. These references discuss the moments of photon number in coherent states and their relation to Heisenberg's uncertainty
  • #1
matteo137
43
9
Homework Statement
calculate the mean and variance of the number operator for a coherent-superposition of two coherent states (cat state)
Relevant Equations
$$(\sqrt{2(1+e^{-2\alpha^2})})^{-1}(\vert\alpha\rangle+\vert -\alpha\rangle)$$
I found the mean to be $$\langle n\rangle=\vert\alpha\vert^2 \tanh(\alpha^2)$ and $\langle n^2\rangle=\vert\alpha\vert^2 \left( \alpha^2\sech(\alpha^2)^2 + \tanh(\alpha^2) \right)$$.

Do you know if there is any reference where I can check if this is correct?
 
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  • #2
I am not aware of any direct reference that contains the exact expressions you have provided. However, there are several references that discuss photon number distributions and/or moments in the context of coherent states. In particular, Ref. 1 discusses the first and second moments of a coherent state in the context of Heisenberg's uncertainty relation. Ref. 2 provides an example of computing the average photon number for a coherent state in the context of the Glauber-Sudarshan P representation. Additionally, Ref. 3 provides a more general discussion on computing the moments of photon number in arbitrary probability distributions, including the case of coherent states. References1. B. M. Garraway, “The Density Matrix and Uncertainty in Coherent States,” J. Mod. Opt. 48, 1743–1751 (2001).2. J. J. Sakurai, Modern Quantum Mechanics, 2nd ed. (Addison-Wesley, Reading, MA, 1994), p. 230.3. M. O. Scully and M. S. Zubairy, Quantum Optics (Cambridge University Press, 1997), p. 255.
 

What is a continuous-variable cat state?

A continuous-variable cat state is a quantum state that exhibits characteristics of both a classical cat state and a quantum cat state. It is a superposition of two coherent states with opposite phases, resulting in a state that is macroscopically distinguishable from a single coherent state.

What is the significance of the phonon number mean in a continuous-variable cat state?

The phonon number mean in a continuous-variable cat state represents the average number of phonons (quantized units of vibrational energy) present in the system. It is a measure of the strength of the quantum state and can be used to characterize the degree of coherence in the system.

How is the phonon number mean calculated in a continuous-variable cat state?

The phonon number mean in a continuous-variable cat state can be calculated by taking the expectation value of the annihilation operator (a) squared. This is equivalent to the square of the coherent state amplitude and represents the average number of phonons in the system.

What is the role of the phonon number variance in a continuous-variable cat state?

The phonon number variance in a continuous-variable cat state is a measure of the spread or uncertainty in the number of phonons present in the system. It is related to the coherence of the state, with a smaller variance indicating a more coherent state.

How is the phonon number variance related to the phonon number mean in a continuous-variable cat state?

The phonon number variance is directly related to the phonon number mean in a continuous-variable cat state. Specifically, the variance is equal to the square of the phonon number mean minus the phonon number mean itself. This relationship allows for the characterization of the coherence of the state based on the phonon number mean and variance.

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