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MICROWAVE NOISE FIELD BEHAVES LIKE WHITE LIGHT J
MICROWAVE NOISE FIELD BEHAVES LIKE WHITE LIGHT J

Photonic bandgap
Photonic bandgap

Dispersion and Ultrashort Pulses
Dispersion and Ultrashort Pulses

... that the beam grazes the tip of each prism ...
Calculation of Complete Absorption and Intensity of Optical
Calculation of Complete Absorption and Intensity of Optical

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Generation of lattices of optical vortices

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4.5 Wave properties

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Perspectives for GAIA

... Perspectives for investigation of CVs with ESA Gaia (I):  Profiles of the light curves of cataclysmic variables (CVs) will be significantly affected by the sampling of the Gaia data.  The individual outbursts in dwarf novae are expected to be covered by only a few Gaia data points – no or very li ...
Full-text PDF
Full-text PDF

... However, because of parametric coupling, the second harmonic is also generated, and it has a two-hump prof ile as shown in Fig. 3. Note that Fig. 1 does not display all possible soliton families and bifurcations that exist in this model. We show only three of the most physically important soliton fa ...
EL Series Optical Fiber Patch Cords
EL Series Optical Fiber Patch Cords

... switch the optical signal being routed through the back of the video jack to the front connectors. ...
Measurement of radiation-pressure
Measurement of radiation-pressure

... optomechanical system is shifted. A previous demonstration of the OS effect 关12兴 showed a 2% shift in the resonant frequency corresponding to an optical rigidity that was 25 times weaker than the mechanical rigidity. An important feature of the OS, which was not accessible to previous experiments du ...
Reflectivity measurements of a quantum well
Reflectivity measurements of a quantum well

Ultrafast Optics: Tools and Techniques
Ultrafast Optics: Tools and Techniques

Evanescent-field optical microscopy: effects of polarization, tip
Evanescent-field optical microscopy: effects of polarization, tip

... which are the result of abrupt changes in feedback action. In fig. 4b a contamination of size smaller than 1 /zm is present. Comparison shows that s-polarized excitation tends to couple light in the lateral direction, resulting in both wider and lower steps, whereas p-polarization couples preferenti ...
Multi-photon absorption and third-order
Multi-photon absorption and third-order

... (MPA) processes has increased over the past decade, because of their importance for ultrafast all-optical signal processing. Near-infrared (near-IR) and short wave infrared (SWIR) nonlinear optical properties of silicon, namely, the third-order susceptibility χ(3), have been widely studied in the pa ...
EE 5551
EE 5551

wavelength dependence of the light-induced index
wavelength dependence of the light-induced index

... response shifts to longer wavelengths. A further observation is that the magnitude of the initial shift in the wavelength response is not constant but decreases in time. The spectral response of the Mach-Zehnder interferometer eventually reaches with time a stationary equilibrium value in which its ...
RESOLVING POWER AND MODULATION TRANSFER FUNCTION
RESOLVING POWER AND MODULATION TRANSFER FUNCTION

... Whether two lines are recognized as resolved or not resolved remains, to a small extent, arbitrary since the existence of two instead of one peak may be recognized with higher or lower contrast as shown in fig. 3 (C). However, introducing that contrast (M) into the MTF („limiting resolution“ in fig. ...
www.osa-opn.org 24 | OPN October 2008 Two positively charged
www.osa-opn.org 24 | OPN October 2008 Two positively charged

... This is a very un-laser-like idea—generation and measurement are entwined. It opens the exciting prospect that attosecond metrology can be generalized to other high-order nonlinear optical processes such as inelastic scattering. Never before has it seemed possible to find systematic methods of measu ...
V. experimental setup of all-optical tunable delay
V. experimental setup of all-optical tunable delay

... with a total delay range of 3870ps. We present wavelength conversion method that show with FWM of phase conjugation property. Our delay technique has the combined advantages of continuous control of a wide range of delays picoseconds to nanoseconds and an output signal wavelength and bandwidth that ...
Chapter 9 Semiconductor Optical Amplifiers
Chapter 9 Semiconductor Optical Amplifiers

... power at which the amplifier gain G decreases by a factor of two (or by 3 dB) from the unsaturated value G * . The output saturation power is the output optical power at which the amplifier gain decreases by a factor of two (or by 3 dB). The input saturation power is given by the expression, ...
Introduction to Spectroscopy
Introduction to Spectroscopy

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14_04_2014 - IB Phys..
14_04_2014 - IB Phys..

measuring
measuring

Slide 1
Slide 1

TITLE: Modal analysis of complex dielectric waveguides by rigorous
TITLE: Modal analysis of complex dielectric waveguides by rigorous

... It can be shown these interfacial tangential fields obey a coupled transverse mode integral equation (CTMIE). These coupled integral equations are then converted into a homogeneous matrix equation via orthogonal projection. The nontrivial solutions for the matrix equation are used to construct the f ...
< 1 ... 62 63 64 65 66 67 68 69 70 ... 93 >

Optical rogue waves

Optical rogue waves are rare pulses of light analogous to rogue or freak ocean waves. The term optical rogue waves was coined to describe rare pulses of broadband light arising during the process of supercontinuum generation—a noise-sensitive nonlinear process in which extremely broadband radiation is generated from a narrowband input waveform—in nonlinear optical fiber. In this context, optical rogue waves are characterized by an anomalous surplus in energy at particular wavelengths (e.g., those shifted to the red of the input waveform) and/or an unexpected peak power. These anomalous events have been shown to follow heavy-tailed statistics, also known as L-shaped statistics, fat-tailed statistics, or extreme-value statistics. These probability distributions are characterized by long tails: large outliers occur rarely, yet much more frequently than expected from Gaussian statistics and intuition. Such distributions also describe the probabilities of freak ocean waves and various phenomena in both the man-made and natural worlds. Despite their infrequency, rare events wield significant influence in many systems. Aside from the statistical similarities, light waves traveling in optical fibers are known to obey the similar mathematics as water waves traveling in the open ocean (the nonlinear Schrödinger equation), supporting the analogy between oceanic rogue waves and their optical counterparts. More generally, research has exposed a number of different analogies between extreme events in optics and hydrodynamic systems. A key practical difference is that most optical experiments can be done with a table-top apparatus, offer a high degree of experimental control, and allow data to be acquired extremely rapidly. Consequently, optical rogue waves are attractive for experimental and theoretical research and have become a highly studied phenomenon. The particulars of the analogy between extreme waves in optics and hydrodynamics may vary depending on the context, but the existence of rare events and extreme statistics in wave-related phenomena are common ground.
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