Displacement operation acting on individual quadrature components

In summary, the displacement operation in quantum mechanics involves manipulating the quadrature components of a quantum state, typically in the context of systems like optical fields or phase space representations. This operation can be expressed mathematically and is crucial for understanding phenomena such as squeezing and quantum measurement. By effectively shifting the values of the quadrature components, the displacement operation allows for the control and optimization of quantum states, facilitating advancements in quantum information processing and communication.
  • #1
waadles
1
0
Hi all,

I have a naive understanding of how operators work and wondered if someone could help me. I have tried to understand this myself, but alas, I think my knowledge is too premature to understand what I am reading online. Is someone able to explain?

I want to perform the operation ##D(\alpha)^\dagger X D(\alpha)##, where ##X## is one of the quadrature components ##X = \frac{1}{\sqrt{2}} (a + a^\dagger)##. I know the following:

$$
D(\alpha)^\dagger a D(\alpha) = a + \alpha
$$

Does this mean ##D(\alpha)^\dagger a^\dagger D(\alpha) = a^\dagger + \alpha^*##?

If so, then:

$$
D(\alpha)^\dagger X D(\alpha) = \frac{1}{\sqrt{2}} D(\alpha)^\dagger (a + a^\dagger) D(\alpha) = \frac{1}{\sqrt{2}} (a + a^\dagger + 2|\alpha|)
$$

This is not correct. I would have expected something like ##\frac{1}{\sqrt{2}} (a + a^\dagger + |\alpha|)##.

I am struggling even more to work out ##P##, where ##P = \frac{i}{\sqrt{2}} (a - a^\dagger)##. I get:

$$
D(\alpha)^\dagger P D(\alpha) = \frac{1}{\sqrt{2}} D(\alpha)^\dagger (a - a^\dagger) D(\alpha) = \frac{1}{\sqrt{2}} (a - a^\dagger)
$$

and it remains the same, which is not correct. I would also expect ##\frac{1}{\sqrt{2}} (a - a^\dagger + |\alpha|)##.

Can someone tell me where I am going wrong?

I appreciate any help you can provide.
 
Last edited:
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  • #2
Since operator a is not Hermitian, I am not sure and accoustomed to translational operation on it. Is it an exercise on textbook ?
 
  • #3
waadles said:
Hi all,

I have a naive understanding of how operators work and wondered if someone could help me. I have tried to understand this myself, but alas, I think my knowledge is too premature to understand what I am reading online. Is someone able to explain?

I want to perform the operation ##D(\alpha)^\dagger X D(\alpha)##, where ##X## is one of the quadrature components ##X = \frac{1}{\sqrt{2}} (a + a^\dagger)##. I know the following:

$$
D(\alpha)^\dagger a D(\alpha) = a + \alpha
$$

Does this mean ##D(\alpha)^\dagger a^\dagger D(\alpha) = a^\dagger + \alpha^*##?
That follows by taking the Hermitian conjugate of the equation.
waadles said:
If so, then:

$$
D(\alpha)^\dagger X D(\alpha) = \frac{1}{\sqrt{2}} D(\alpha)^\dagger (a + a^\dagger) D(\alpha) = \frac{1}{\sqrt{2}} (a + a^\dagger + 2|\alpha|)
$$
Note that ##\alpha + \alpha^* = 2Re(\alpha)##.
waadles said:
This is not correct. I would have expected something like ##\frac{1}{\sqrt{2}} (a + a^\dagger + |\alpha|)##.
Why did you expect that?
waadles said:
I am struggling even more to work out ##P##, where ##P = \frac{i}{\sqrt{2}} (a - a^\dagger)##. I get:

$$
D(\alpha)^\dagger P D(\alpha) = \frac{1}{\sqrt{2}} D(\alpha)^\dagger (a - a^\dagger) D(\alpha) = \frac{1}{\sqrt{2}} (a - a^\dagger)
$$
In this case you should use ##\alpha - \alpha^* = 2iIm(\alpha)##.
 
  • #4
PeroK said:
In this case you should use α−α∗=2iIm(α).
May we say about meaning of translation of a as
[tex]\alpha=\frac{d_x}{\sqrt{2}}-i\frac{d_p}{\sqrt{2}}[/tex]
where d_x and d_p are displacement in coordinate and momentum space ?
If so it holds for the translated Hamiltoian, i.e.
[tex](a^{\dagger} +\alpha^*)(a+\alpha)+\frac{1}{2}[/tex]? It seems not obvious to me.
 

FAQ: Displacement operation acting on individual quadrature components

What is a displacement operation in the context of quantum optics?

A displacement operation in quantum optics is a unitary transformation that shifts the phase space coordinates of a quantum state. It is represented by the operator \( D(\alpha) = \exp(\alpha \hat{a}^\dagger - \alpha^* \hat{a}) \), where \( \alpha \) is a complex number, and \( \hat{a} \) and \( \hat{a}^\dagger \) are the annihilation and creation operators, respectively. This operation effectively displaces the state in phase space by \( \alpha \).

How does the displacement operation affect the quadrature components of a quantum state?

The displacement operation affects the quadrature components, which are the real and imaginary parts of the complex amplitude of the quantum state. Specifically, if the quadrature components are represented as \( \hat{X} = (\hat{a} + \hat{a}^\dagger) / \sqrt{2} \) and \( \hat{P} = (\hat{a} - \hat{a}^\dagger) / (i\sqrt{2}) \), the displacement operation shifts these components by the real and imaginary parts of \( \alpha \). Mathematically, \( \hat{X} \) is shifted by \( \sqrt{2} \Re(\alpha) \) and \( \hat{P} \) by \( \sqrt{2} \Im(\alpha) \).

What is the physical significance of displacing individual quadrature components?

Displacing individual quadrature components is significant for various quantum information processing tasks, including state preparation, quantum communication, and error correction. By controlling the displacement in phase space, one can manipulate the quantum state to achieve desired properties, such as encoding information or correcting errors in quantum bits (qubits).

Can displacement operations be implemented experimentally, and if so, how?

Yes, displacement operations can be implemented experimentally using optical components. One common method involves using a beam splitter to combine the quantum state with a strong coherent state (a laser beam) in a controlled manner. By adjusting the amplitude and phase of the coherent state, the desired displacement can be achieved. This process is often used in quantum optics laboratories to manipulate and measure quantum states.

What are the mathematical properties of the displacement operator?

The displacement operator \( D(\alpha) \) has several important mathematical properties. It is unitary, meaning \( D(\alpha) D^\dagger(\alpha) = D^\dagger(\alpha) D(\alpha) = I \). It also satisfies the relation \( D(\alpha) D(\beta) = D(\alpha + \beta) e^{i \

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