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Broad Band Two-Dimensional Manipulation of Surface Plasmons
Broad Band Two-Dimensional Manipulation of Surface Plasmons

... polarization perpendicular to the slit.29 Therefore, the strength of the SPPs at different portions of the slit can be arbitrarily tuned by adjusting the polarization of the excitation light beam. For example, in Figure 5 the fluorescent images illustrate how the SPPs propagate along the surface for ...
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... The intensity of unpolarized light passing through the first filter is ½ the initial intensity I0, so the final intensity I2 can be written I 2 = 12 cos 2 36° = 0.33I 0 . ...
Dynamical diffraction of atomic matter waves by crystals of light
Dynamical diffraction of atomic matter waves by crystals of light

... where V Rabi(rW ) represents the on-resonance Rabi frequency, which is periodically modulated in space for a standing light wave. The detuning of the laser frequency from resonance is described by D5 v l 2 v 0 , where v l is the laser frequency and v 0 is atomic transition frequency. The parameter g ...
High-sensitivity, single-beam n2 measurements
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IITJEE PHYSICS SAMPLE PAPER - III

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Chapter Nine Radiation
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... wave, charges in the scatterer will be set into some sort of coherent motion1 and these moving charges will produce radiation, called the scattered wave. Hence scattering phenomena are closely related to radiation phenomena. Diffraction of electromagnetic waves is similar. One starts with a wave in ...
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... Light as EM Wave • The wavelengths of visible light were measured in the first decade of the 19th century – The visible light wave length were found to be between 4.0x10-7m (400nm) and 7.5x10-7m (750nm) – The frequency of visible light is fλ=c • Where f and λ are the frequency and the wavelength of ...
Monday, Nov. 28, 2005 - UTA HEP WWW Home Page
Monday, Nov. 28, 2005 - UTA HEP WWW Home Page

... produced using electronic devices • Higher frequency waves are produced natural processes, such as emission from atoms, molecules or nuclei • Or they can be produced from acceleration of charged particles • Infrared radiation (IR) is mainly responsible for the heating effect of the Sun – The Sun emi ...
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QOLECTURE2

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Practice Final Exam

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HS-SCI-CP -- Chapter 15- Interference and
HS-SCI-CP -- Chapter 15- Interference and

... from constructive and destructive interference. In the case of interference, it is assumed that the slits behave as point sources of light. For diffraction, the actual width of a single slit is considered. According to Huygens' principle, each portion of a slit acts as a source of waves. Hence, ligh ...
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Diffraction



Diffraction refers to various phenomena which occur when a wave encounters an obstacle or a slit. In classical physics, the diffraction phenomenon is described as the interference of waves according to the Huygens–Fresnel principle. These characteristic behaviors are exhibited when a wave encounters an obstacle or a slit that is comparable in size to its wavelength. Similar effects occur when a light wave travels through a medium with a varying refractive index, or when a sound wave travels through a medium with varying acoustic impedance. Diffraction occurs with all waves, including sound waves, water waves, and electromagnetic waves such as visible light, X-rays and radio waves.Since physical objects have wave-like properties (at the atomic level), diffraction also occurs with matter and can be studied according to the principles of quantum mechanics. Italian scientist Francesco Maria Grimaldi coined the word ""diffraction"" and was the first to record accurate observations of the phenomenon in 1660.While diffraction occurs whenever propagating waves encounter such changes, its effects are generally most pronounced for waves whose wavelength is roughly comparable to the dimensions of the diffracting object or slit. If the obstructing object provides multiple, closely spaced openings, a complex pattern of varying intensity can result. This is due to the addition, or interference, of different parts of a wave that travels to the observer by different paths, where different path lengths result in different phases (see diffraction grating and wave superposition). The formalism of diffraction can also describe the way in which waves of finite extent propagate in free space. For example, the expanding profile of a laser beam, the beam shape of a radar antenna and the field of view of an ultrasonic transducer can all be analyzed using diffraction equations.
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