Non-local angular double-slit ghost diffraction with thermal light

2016 ◽  
Author(s):  
Lu Gao ◽  
Jiapeng. Zhao ◽  
Omar S. Magaña-Loaiza ◽  
Seyed Mohammad Hashemi Rafsanjani ◽  
Mohammad Mirhosseini ◽  
...  
Keyword(s):  
Thermal Light ◽  
Non Local ◽  
Double Slit

Non-local edge enhanced imaging with incoherent thermal light

2020 ◽  
Vol 116 (17) ◽  
pp. 174001
Author(s):  
Hanquan Song ◽  
Yingwen Zhang ◽  
Yuhang Ren ◽  
Zhidan Yuan ◽  
Dayu Zhao ◽  
...  
Keyword(s):  
Thermal Light ◽  
Non Local ◽  
Local Edge ◽  
Enhanced Imaging

scholarly journals Distributed angular double-slit interference with pseudo-thermal light

2017 ◽  
Vol 110 (7) ◽  
pp. 071107 ◽  
Author(s):  
Lu Gao ◽  
Seyed Mohammad Hashemi Rafsanjani ◽  
Yiyu Zhou ◽  
Zhe Yang ◽  
Omar S. Magaña-Loaiza ◽  
...  
Keyword(s):  
Thermal Light ◽  
Double Slit

scholarly journals Role of intensity fluctuations in third-order correlation double-slit interference of thermal light

2013 ◽  
Vol 30 (7) ◽  
pp. 1422 ◽  
Author(s):  
Xi-Hao Chen ◽  
Wen Chen ◽  
Shao-Ying Meng ◽  
Wei Wu ◽  
Ling-An Wu ◽  
...  
Keyword(s):  
Third Order ◽  
Thermal Light ◽  
Intensity Fluctuations ◽  
Double Slit

Non-local correlation interference with pseudo-thermal light

2016 ◽  
Vol 381 ◽  
pp. 323-326
Author(s):  
Ling-Yu Dou ◽  
Lu Gao ◽  
Xin-Bing Song
Keyword(s):  
Local Correlation ◽  
Thermal Light ◽  
Non Local

Interference from nonlocal double-slit with pseudo-thermal light

2008 ◽  
Vol 281 (10) ◽  
pp. 2838-2841 ◽  
Author(s):  
Lu Gao ◽  
Jun Xiong ◽  
Lu-Fang Lin ◽  
Wei Wang ◽  
Su-Heng Zhang ◽  
...  
Keyword(s):  
Thermal Light ◽  
Double Slit

scholarly journals How can a Random Phenomenon between Particles be Synchronized Instantaneously and Independently of the Distance Between Said Particles?

2021 ◽  
Author(s):  
Mario Mastriani
Keyword(s):  
Quantum Measurement ◽  
Communication System ◽  
Human Intervention ◽  
Functional Models ◽  
Transmission Of Information ◽  
Before And After ◽  
Non Local ◽  
Double Slit Experiment ◽  
Slit Experiment ◽  
Double Slit

Abstract Entanglement is a random phenomenon that is instantly synchronized, regardless of the space that mediates between entangled particles. However, the instantaneous transmission of information using entanglement is impossible. This is because the instantaneity in the synchronization of non-local outcomes as a consequence of quantum measurement (after the distribution of the entangled pairs) cannot be used for an entanglement-based communication system to transmit information instantaneously. This impossibility stems from the following two reasons: a) the difficulty of controlling non-local outcomes through local actions without the intervention of an auxiliary channel (classical), and b) regardless of the previous point, no communication system based on entanglement can be instantaneous due to the distribution of an entangled pair at relativistic speeds, necessary to generate the quantum channel, each time a qubit must be transmitted. Three simple experiments help to clarify this controversial point. In fact, this study establishes what is truly responsible for the impossibility to transmit information instantaneously of any communication system based on entanglement. In this respect, functional models of the internal behavior of quantum measurement, and entanglement were developed, which allow analyzing the instantaneity post-distribution of entangled particles, before and after a quantum measurement, as well as the randomness in the results obtained from a quantum measurement of the entanglement. In this sense, this study establishes a debate about three possible responsible for the aforementioned randomness: the quantum measurement itself, entanglement, and the human intervention. Finally, homology between the entanglement and the double-slit experiment is presented.

Toward High-Resolution Low-Voltage SEM

1988 ◽  
Vol 46 ◽  
pp. 218-219
Author(s):  
Zhifeng Shao
Keyword(s):  
Low Voltage ◽  
Spherical Aberration ◽  
Chromatic Aberration ◽  
Limiting Factor ◽  
Operating Voltage ◽  
Probe Radius ◽  
Non Local ◽  
Electron Microscopes ◽  
Image Position ◽  
Scanning Electron Microscopes

Recently, low voltage (≤5kV) scanning electron microscopes have become popular because of their unprecedented advantages, such as minimized charging effects and smaller specimen damage, etc. Perhaps the most important advantage of LVSEM is that they may be able to provide ultrahigh resolution since the interaction volume decreases when electron energy is reduced. It is obvious that no matter how low the operating voltage is, the resolution is always poorer than the probe radius. To achieve 10Å resolution at 5kV (including non-local effects), we would require a probe radius of 5∽6 Å. At low voltages, we can no longer ignore the effects of chromatic aberration because of the increased ratio δV/V. The 3rd order spherical aberration is another major limiting factor. The optimized aperture should be calculated as

Chromatic aberration and low-voltage SEM

1987 ◽  
Vol 45 ◽  
pp. 546-547
Author(s):  
Zhifeng Shao ◽  
A.V. Crewe
Keyword(s):  
Electron Energy ◽  
Low Voltage ◽  
Spherical Aberration ◽  
Chromatic Aberration ◽  
Primary Electron ◽  
Probe Size ◽  
Non Local ◽  
Optical Treatment ◽  
Electron Microscopes ◽  
Scanning Electron Microscopes

For scanning electron microscopes, it is plausible that by lowering the primary electron energy, one can decrease the volume of interaction and improve resolution. As shown by Crewe /1/, at V0 =5kV a 10Å resolution (including non-local effects) is possible. To achieve this, we would need a probe size about 5Å. However, at low voltages, the chromatic aberration becomes the major concern even for field emission sources. In this case, δV/V = 0.1 V/5kV = 2x10-5. As a rough estimate, it has been shown that /2/ the chromatic aberration δC should be less than ⅓ of δ0 the probe size determined by diffraction and spherical aberration in order to neglect its effect. But this did not take into account the distribution of electron energy. We will show that by using a wave optical treatment, the tolerance on the chromatic aberration is much larger than we expected.

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