標(biāo)題: Titlebook: Lagrangian Optics; Vasudevan Lakshminarayanan,Ajoy K. Ghatak,K. Thyag Book 2002 Springer Science+Business Media New York 2002 adaptive opt [打印本頁] 作者: 板條箱 時(shí)間: 2025-3-21 20:02
書目名稱Lagrangian Optics影響因子(影響力)
書目名稱Lagrangian Optics影響因子(影響力)學(xué)科排名
書目名稱Lagrangian Optics網(wǎng)絡(luò)公開度
書目名稱Lagrangian Optics網(wǎng)絡(luò)公開度學(xué)科排名
書目名稱Lagrangian Optics被引頻次
書目名稱Lagrangian Optics被引頻次學(xué)科排名
書目名稱Lagrangian Optics年度引用
書目名稱Lagrangian Optics年度引用學(xué)科排名
書目名稱Lagrangian Optics讀者反饋
書目名稱Lagrangian Optics讀者反饋學(xué)科排名
作者: 溫和女孩 時(shí)間: 2025-3-22 00:04
,Fermat’s Principle,n either of the fields. One of the most basic analogy is between the Fermat’s principle in optics and the Hamilton’s principle of least action in classical mechanics [.]. As in classical mechanics, we can use either the Lagrangian or the Hamiltonian formulations to further study properties of light 作者: Cognizance 時(shí)間: 2025-3-22 03:12
The Optical Lagrangian and the Ray Equation,grangian, the integration is over time, ..(.=,2,…) represent the generalized coordinates and dots represent differentiation with respect to time. Equation (1) is referred to as the Hamilton’s principle of least action. From {zyEq.(1)|33-1} it is possible to derive the Lagrange’s equations of motion 作者: interlude 時(shí)間: 2025-3-22 07:23
Ray Paths in Bent Waveguides,ems [.–.]. When rays in multimode waveguides encounter bends there are radiation losses; these losses are either by refraction or by tunneling. The fractional loss of power when a ray is reflected from an outer caustic along the ray path is usually calculated by using the WKB method. Hence it is ess作者: locus-ceruleus 時(shí)間: 2025-3-22 09:48 作者: 鐵砧 時(shí)間: 2025-3-22 14:25
Geometrical Theory of Third-Order Aberrations,proximation, i.e., the rays forming the image were assumed to lie infinitesimally close to the axis and to make infinitesimally small angles with it. It was found that the images of point objects were perfect, i.e., all rays starting from a given object point were found to intersect at . point, whic作者: Induction 時(shí)間: 2025-3-22 20:03 作者: 圓桶 時(shí)間: 2025-3-23 00:24 作者: COST 時(shí)間: 2025-3-23 02:42 作者: guzzle 時(shí)間: 2025-3-23 05:39
Vasudevan Lakshminarayanan,Ajoy K. Ghatak,K. Thyagarajan作者: conflate 時(shí)間: 2025-3-23 09:55
Vasudevan Lakshminarayanan,Ajoy K. Ghatak,K. Thyagarajan作者: 有助于 時(shí)間: 2025-3-23 16:50 作者: Moderate 時(shí)間: 2025-3-23 20:33 作者: SIT 時(shí)間: 2025-3-23 23:51
Vasudevan Lakshminarayanan,Ajoy K. Ghatak,K. Thyagarajan作者: Affection 時(shí)間: 2025-3-24 04:39
Vasudevan Lakshminarayanan,Ajoy K. Ghatak,K. Thyagarajan作者: ARBOR 時(shí)間: 2025-3-24 10:15
Vasudevan Lakshminarayanan,Ajoy K. Ghatak,K. Thyagarajan作者: 整理 時(shí)間: 2025-3-24 14:07 作者: Terminal 時(shí)間: 2025-3-24 16:21 作者: 過于光澤 時(shí)間: 2025-3-24 21:19
begin with Fermat‘s principle and obtain the Lagrangian and Hamiltonian pictures of ray propagation through various media. Given the current interest and activity in optical fibers and optical communication, analysis of light propagation in inhomogeneous media is dealt with in great detail. The past decade h978-1-4613-5690-5978-1-4615-1711-5作者: 十字架 時(shí)間: 2025-3-25 00:25 作者: Morsel 時(shí)間: 2025-3-25 06:41
http://image.papertrans.cn/l/image/580470.jpg作者: 火光在搖曳 時(shí)間: 2025-3-25 07:40
978-1-4613-5690-5Springer Science+Business Media New York 2002作者: 賭博 時(shí)間: 2025-3-25 15:26
https://doi.org/10.1007/978-1-4615-1711-5adaptive optics; analog; classical mechanics; communication; Counter; energy; light propagation; mechanics; 作者: FLIP 時(shí)間: 2025-3-25 16:34
Ray Paths in Media with Spherical and Cylindrical Symmetry,In this chapter we will discuss the solutions of the Lagrange’s equations for media having spherical and cylindrical symmetry. Ray paths in cylindrically symmetric media are of tremendous importance in fiber optics.作者: 完成 時(shí)間: 2025-3-25 21:22
The Optical Hamiltonian and Study of Paraxial Lens Optics,alculate explicit expressions for various aberration coefficients. In the Hamiltonian formulation, we have first to define the generalized momenta . and . by the relation.. where, as before, dots represent differentiation with respect to . and . is the optical Lagrangian. On substituting the value of . from Eq.(8) of Chapter 3, we find 作者: Inertia 時(shí)間: 2025-3-26 03:07 作者: persistence 時(shí)間: 2025-3-26 05:12 作者: 詞匯表 時(shí)間: 2025-3-26 10:45 作者: 剛開始 時(shí)間: 2025-3-26 14:53
An Introduction to Dynamic Programming and Applications to Optics,ineering, Physics, Biology, Economics and even Medicine [.–.]. The problem is usually stated as the minimization of a functional equation. An approach to solving this problem is a technique called dynamic programming which will be introduced in this chapter.作者: urethritis 時(shí)間: 2025-3-26 18:16
Introduction,conomy’ postulates in the hands of later scientists acted as the foundation for the development of minimum principles such as Fermat’s principle. If one studies the chronological development in the evolution of minimum principles one can get a profound insight into the continuos transformation of a metaphysical canon into an exact natural law.作者: 圣人 時(shí)間: 2025-3-26 21:39 作者: 河流 時(shí)間: 2025-3-27 01:55
ofthe optical wavelength tending to zero. Many features oflight propagation can be analyzed in terms ofrays,ofcourse, subtle effects near foci, caustics or turning points would need an analysis based on the wave natureoflight. Allofgeometric optics can be derived from Fermat‘s principle which is an 作者: Diluge 時(shí)間: 2025-3-27 09:02
Ray Paths in Bent Waveguides,ential to know the exact ray paths in bent waveguides and thereby know the exact positions of the ray caustics to calculate the bend loss. In this chapter, we present an analysis to find ray paths in bent slab waveguides.作者: chronicle 時(shí)間: 2025-3-27 12:47
An Introduction to Lie Algebraic Treatment of Optical Aberrations, one were to go up to the 5th order, the size of the matrices are of the dimensions of 125 × 125 for any arbitrary conical surface. The size of the matrices can be reduced by the use of symmetries, but the method is still cumbersome.作者: 玩忽職守 時(shí)間: 2025-3-27 17:32
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10樓作者: 杠桿 時(shí)間: 2025-3-28 12:41
10樓作者: 反復(fù)無常 時(shí)間: 2025-3-28 17:44
10樓作者: Morsel 時(shí)間: 2025-3-28 21:56
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