Zobrazeno 1 - 10
of 48
pro vyhledávání: '"Alan D. Kathman"'
Autor:
Artem Kryvobok, Alan D. Kathman
Publikováno v:
Quantum Studies: Mathematics and Foundations. 9:55-70
Some quantum optics researchers might not realize that classical electromagnetism predicts a $$\mathbf {\pi }$$ π phase shift between S- and P-polarized reflection and might think the reflection coefficients of the transverse modes are independent,
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::824a458cbaa16c86888039897125b1b4
https://doi.org/10.1007/s40509-021-00256-8
https://doi.org/10.1007/s40509-021-00256-8
Autor:
Artem Kryvobok, Alan D. Kathman
The effects of a beamsplitter are frequently described mathematically as a matrix acting on a two input ports vector. This might be comprehensive for a scalar field but certainly insufficient in case of photons which are vector fields. In this paper
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_dedup___::1e1d857d16953585021711859d94ef9c
https://doi.org/10.21203/rs.3.rs-694207/v1
https://doi.org/10.21203/rs.3.rs-694207/v1
Once a surface relief pattern has been patterned in photoresist or etched into a substrate, how do you know if you have produced what you wanted? There are many different approaches to answering this question, but all of them fall into one of two cat
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::68e6f97f357d8b76418bed6aacf220cd
https://doi.org/10.1117/3.527861.ch9
https://doi.org/10.1117/3.527861.ch9
The discussion in Chapter 4 centered on the design of diffractive optics using conventional lens design techniques, in which each ray incident on the DOE is mapped to one output ray. The refractive lenses and mirrors and the diffractive elements desc
Externí odkaz:
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https://doi.org/10.1117/3.527861.ch5
https://doi.org/10.1117/3.527861.ch5
This chapter describes the uses of diffractive optics in lens design. In some applications an optical component may require a diffractive surface combined with a classic lens element. In other cases the requirements can be satisfied with just a diffr
Externí odkaz:
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https://doi.org/10.1117/3.527861.ch4
https://doi.org/10.1117/3.527861.ch4
Light is part of the electromagnetic spectrum and therefore is governed by Maxwell's equations. In this chapter we introduce these equations to describe the propagation of light. In later chapters we will use them as a basis for the design of a wide
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::37765220da6efce37023c592415c2a01
https://doi.org/10.1117/3.527861.ch2
https://doi.org/10.1117/3.527861.ch2
In previous chapters we considered the fundamental theories of diffraction and a number of design approaches for diffractive optical elements. However, before a diffractive optical element can be built, a number of additional questions must be addres
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::ab08bcc788c97ab87ae6907637b2ba21
https://doi.org/10.1117/3.527861.ch6
https://doi.org/10.1117/3.527861.ch6
In Chapter 4 the diffractive lens, including a simple hybrid achromat, was discussed in some detail. In this chapter, we extend our discussion of lens design by introducing the wavefront aberration polynomial and the Seidel coefficients. Although it
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::4a5b7b2c1cc447621b3383355466ac92
https://doi.org/10.1117/3.527861.ch10
https://doi.org/10.1117/3.527861.ch10
The photolithographic processes used for fabrication of diffractive optical elements adapted from the microelectronics industry were broadly described in the previous chapter. These methods are based on the use of photoresist. A more detailed photore
Externí odkaz:
https://explore.openaire.eu/search/publication?articleId=doi_________::e047a905447a85f086b0d5423e28d18c
https://doi.org/10.1117/3.527861.ch7
https://doi.org/10.1117/3.527861.ch7