Time delay for evanescent wave to spread (photon tunnelling)

In summary, the recent tunnelling experiment by Nimtz and Stahlhofen suggests that tunnelling time for light between double prisms is zero. However, Herbert Winful explains that the evanescent wave formed in the gap only has real propagation along the surface of the prism and compares the gap to a cavity that holds energy and releases it simultaneously out of both sides. The evanescent wave is able to fill the gap instantaneously due to its exponential decay, and it oscillates in all directions resulting in a standing wave pattern that moves up and down the Goos-Hanchen shift with time.
  • #1
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Nimtz and Stahlhofen claim that their recent tunnelling experiment proves that tunnelling time for light between double prisms is zero. In Herbert Winful's response to this (http://arxiv.org/ftp/arxiv/papers/0709/0709.2736.pdf) he explains that the evanescent wave formed in the gap only has real propagation along the surface of the prism (not towards the second prism). He compares the gap to a cavity that holds energy, transverses the distance of the Goos-Hanchen shift, and then releases the energy simultaneously out of both sides of the gap. I have two questions..

1) It makes sense that after the evanescent wave fills the gap it is able to "leak" out energy into both prisms, but does it not take time for the evanescent wave to fill the gap? Why does this time not vary with gap length?

2) I have also read that this evanescent wave is a standing wave that oscillates, but it is not clear to me in which direction it oscillates? Does the waves move downwards due to the goos-hanchen shift and then another evanescent wave from new incident waves begins at the incident point periodically resulting in a standing evanescent wave moving up and down the goos-hanchen shift with time?

sorry for my ignorance this is all very new to me and I'm just trying to grasp what I can..
 
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  • #2
1) The evanescent wave is able to fill the gap instantaneously because its amplitude decays exponentially with distance from the source. This means that for two prisms of a given separation, the wave will reach both prisms at the same time regardless of the length of the gap. 2) The evanescent wave oscillates in all directions. This means that when an incident wave hits the interface between the two prisms, part of the wave will be reflected and part will be transmitted into the gap. The transmitted wave will then oscillate in the gap and move towards the second prism. As the wave moves, it will encounter the Goos-Hanchen shift which will cause it to move laterally, resulting in a standing wave pattern in the gap. Thus, the wave will periodically move up and down the Goos-Hanchen shift with time.
 
  • #3


I would first like to commend you for taking the initiative to explore and understand this complex topic. It is important for individuals to actively seek out knowledge and ask questions in order to further their understanding of scientific concepts.

Now, to address your questions:

1) The concept of tunnelling time for evanescent waves is still a topic of debate among scientists. While Nimtz and Stahlhofen claim that their experiment proves a zero tunnelling time, Winful's response raises valid points about the nature of evanescent waves and the time it takes for them to fill the gap between the prisms.

One possible explanation for the seemingly instantaneous tunnelling time could be that the evanescent wave is already present in the gap before the incident light reaches it. This is supported by the fact that evanescent waves are a result of total internal reflection, which occurs at the interface between two mediums. Therefore, the evanescent wave may already be present in the gap, waiting to be "activated" by the incident light.

Additionally, the tunnelling time may not vary with gap length because the evanescent wave is not actually propagating through the gap. Instead, it is confined to the surface of the prism and is able to "leak" out energy into both prisms.

2) The direction of oscillation for the evanescent wave is perpendicular to the surface of the prism. This means that the wave moves parallel to the interface between the two mediums, rather than up and down the Goos-Hanchen shift. The standing wave pattern is a result of the incident and reflected waves interfering with each other, creating regions of high and low intensity.

I hope this helps to clarify some of your questions. As with any scientific concept, there may still be areas of uncertainty and ongoing research. It is important to continue exploring and asking questions in order to further our understanding of the world around us.
 

Related to Time delay for evanescent wave to spread (photon tunnelling)

1. What is the concept of time delay for evanescent wave to spread?

The time delay for evanescent wave to spread refers to the amount of time it takes for a photon to tunnel through a barrier and emerge on the other side. This delay is caused by the photon's interaction with the barrier, which can alter its speed and direction.

2. How does photon tunnelling occur?

Photon tunnelling occurs when a photon encounters a potential barrier that is thinner than its wavelength. The photon's energy allows it to temporarily pass through the barrier, creating an evanescent wave on the other side. This phenomenon is governed by quantum mechanics and is responsible for a variety of phenomena, such as quantum tunneling and the operation of scanning tunneling microscopes.

3. What factors affect the time delay for evanescent wave to spread?

The time delay for evanescent wave to spread can be affected by several factors, including the thickness and composition of the barrier, the angle of incidence of the photon, and the photon's energy. Additionally, the properties of the surrounding medium, such as its refractive index, can also influence the time delay.

4. How is the time delay for evanescent wave to spread measured?

The time delay for evanescent wave to spread can be measured using various techniques, such as time-resolved spectroscopy or interferometry. These methods involve measuring the arrival time of the evanescent wave at a specific point and comparing it to the arrival time of a reference wave that has not undergone tunnelling. The difference in arrival times can then be used to calculate the time delay.

5. What are the practical applications of understanding time delay for evanescent wave to spread?

Understanding the time delay for evanescent wave to spread has important implications in various fields, including optics, photonics, and quantum mechanics. It can help in the design and development of devices such as optical switches and sensors, as well as in studying fundamental properties of light and matter. Additionally, this knowledge can also be applied in information processing, such as in quantum computing, where tunnelling is utilized in quantum gates.

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