Single-Photon Added Coherent States

Substituting this expression into the previous one, we get:\Psi_{\alpha,1}(x) = \sum_{n=0}^{\infty} \sum_{m=0}^{\infty} \alpha_n \frac{1}{\sqrt{n!}} e^{-\frac{1}{2}\alpha^2} \left(\frac{\alpha}{\sqrt{2}}\right)^n \sqrt{m+1} \langle x|m+1\rangleTo simplify this expression, we can use the creation
  • #1
doublemint
141
0
Hello!
So this is my question:
The single-photon added coherent states (SPACS) are obtained from the action of a creation operator onto to a coherent state. [tex]\left|\alpha,1\right\rangle[/tex] = [tex]\hat{a}^{\dagger}\left|\alpha\right\rangle[/tex]

So I need to find the decomposition of this state into number basis and the wavefunction of SPACS for a real [tex]\alpha[/tex].
[tex]a^{\dagger}[/tex] is the creation operator.
a is the annihilation operator.
The first part:
[tex]|\alpha> = \sum \alpha_{n}|n>[/tex]
[tex]a|\alpha> = \sum \alpha_{n}\sqrt{n}|n-1>[/tex]
[tex]a^{\dagger} a |\alpha> = \sum \alpha_{n}\sqrt{n}\sqrt{n-1}|n>[/tex]

The second part:
This is the one that I don't understand...
so far I this:
[tex]a^{\dagger}|\alpha> =\frac{1}{\sqrt{2}}(X-\frac{d}{dX})\Psi_{\alpha}(x)=(\frac{d}{d\alpha}+\frac{\alpha}{2})\Psi_{alpha}(x)[/tex]
[tex](X-\frac{\alpha \sqrt{2}}{2}-\frac{d}{dX}-\frac{d}{d\alpha})\Psi_{\alpha}(x)=0[/tex]

Any help would be appreciated!
Thank You
DoubleMint
 
Physics news on Phys.org
  • #2
, thank you for your question. To find the decomposition of the single-photon added coherent state (SPACS) into the number basis, we can use the following expression:

\left|\alpha,1\right\rangle = \hat{a}^{\dagger}\left|\alpha\right\rangle = \sum_{n=0}^{\infty} \alpha_n \sqrt{n+1} \left|n+1\right\rangle

where \alpha_n = \langle n|\alpha\rangle is the coefficient of the number state \left|n\right\rangle in the coherent state \left|\alpha\right\rangle. Using this expression, we can find the wavefunction of the SPACS for a real \alpha by substituting the expression for \alpha_n into the above equation:

\left|\alpha,1\right\rangle = \sum_{n=0}^{\infty} \langle n|\alpha\rangle \sqrt{n+1} \left|n+1\right\rangle = \sum_{n=0}^{\infty} \Psi_{\alpha}(x) \sqrt{n+1} \left|n+1\right\rangle

where \Psi_{\alpha}(x) = \langle x|\alpha\rangle is the wavefunction of the coherent state. We can then use the number basis \left|n\right\rangle to express the wavefunction of the SPACS as:

\Psi_{\alpha,1}(x) = \sum_{n=0}^{\infty} \Psi_{\alpha}(x) \sqrt{n+1} \langle x|n+1\rangle

To find the expression for \langle x|n+1\rangle, we can use the fact that the coherent state \left|\alpha\right\rangle can be written as a superposition of number states:

\left|\alpha\right\rangle = \sum_{n=0}^{\infty} \alpha_n \left|n\right\rangle

which gives us the following expression for the wavefunction:

\Psi_{\alpha}(x) = \langle x|\alpha\rangle = \sum_{n=0}^{\infty} \alpha_n \langle x|n\rangle = \sum_{n=0}^{\infty} \alpha_n \frac{1}{\
 

What are Single-Photon Added Coherent States?

Single-Photon Added Coherent States (SPACS) are quantum states of light that have been modified by adding a single photon to a coherent state. Coherent states are classical-like states of light that have a well-defined amplitude and phase, and are commonly used in quantum optics experiments.

What is the significance of SPACS in quantum optics?

SPACS have been of great interest in quantum optics due to their unique properties. They have been used to study quantum interference, quantum entanglement, and to demonstrate quantum teleportation and other quantum communication protocols.

How are SPACS generated?

SPACS can be generated in the laboratory using various methods such as stimulated emission, parametric down-conversion, and spontaneous parametric down-conversion. These methods involve manipulating the properties of light, such as its phase and polarization, to create SPACS.

What are the potential applications of SPACS?

SPACS have potential applications in quantum communication, quantum computing, and quantum metrology. They can also be used to study fundamental aspects of quantum mechanics and to test theories about the nature of light.

What are the challenges in working with SPACS?

One of the main challenges in working with SPACS is their fragility. They are highly sensitive to noise and environmental disturbances, which can cause them to lose their quantum properties. Another challenge is the difficulty in generating and manipulating them, as this requires advanced laboratory equipment and techniques.

Similar threads

  • Advanced Physics Homework Help
Replies
5
Views
855
  • Advanced Physics Homework Help
Replies
5
Views
1K
  • Advanced Physics Homework Help
Replies
24
Views
783
  • Advanced Physics Homework Help
Replies
10
Views
1K
  • Advanced Physics Homework Help
Replies
1
Views
1K
  • Advanced Physics Homework Help
Replies
3
Views
879
  • Advanced Physics Homework Help
Replies
15
Views
2K
  • Advanced Physics Homework Help
Replies
1
Views
1K
  • Advanced Physics Homework Help
Replies
9
Views
1K
  • Advanced Physics Homework Help
Replies
19
Views
804
Back
Top