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... alters the optical path difference between the two beams. This causes a change of the interference pattern, which enables us to determine accurately the refractive index of the sample under investigation and the local variation of the interfering fringes. Therefore the MZI may be regarded as a sensi ...
... alters the optical path difference between the two beams. This causes a change of the interference pattern, which enables us to determine accurately the refractive index of the sample under investigation and the local variation of the interfering fringes. Therefore the MZI may be regarded as a sensi ...
Compact Optical Fiber Amplifier
... A forward pumping configuration (without middle isolator) is one of the normal configurations of optical fiber amplifiers, but it has the weak point that the backward Amplified Spontaneous Emission (ASE) wastes pumping power near the input terminal of the EDF, and this behavior causes a degradation ...
... A forward pumping configuration (without middle isolator) is one of the normal configurations of optical fiber amplifiers, but it has the weak point that the backward Amplified Spontaneous Emission (ASE) wastes pumping power near the input terminal of the EDF, and this behavior causes a degradation ...
In text you refer to OAP mirrors as 2nd etc, In fig, they are labeled
... The Linac Coherent Light Source (LCLS) at the SLAC National Accelerator Laboratory is a free-electron laser (FEL) capable of producing some of the shortest x-ray pulses ever observed. By sending pulses of electron bunches less than ten femtoseconds in duration through magnetic fields that force them ...
... The Linac Coherent Light Source (LCLS) at the SLAC National Accelerator Laboratory is a free-electron laser (FEL) capable of producing some of the shortest x-ray pulses ever observed. By sending pulses of electron bunches less than ten femtoseconds in duration through magnetic fields that force them ...
New concept of laser fusion driver using Stimulated Brillouin
... phases are not matched. 2. Phase difference between the beams should be less than /4 for constructive interference at the boundary of the combination not give spatial spiking. 3. It is necessary to control the phases of the SBS waves to match the phase difference between the neighboring beams less ...
... phases are not matched. 2. Phase difference between the beams should be less than /4 for constructive interference at the boundary of the combination not give spatial spiking. 3. It is necessary to control the phases of the SBS waves to match the phase difference between the neighboring beams less ...
Three-Dimensional Simulation of Vertical-Cavity Surface
... Figure 1.2: Structures of a typical VCSEL (left side) and of an edge-emitting laser diode (right ...
... Figure 1.2: Structures of a typical VCSEL (left side) and of an edge-emitting laser diode (right ...
MONABIPHOT_All_Courses_2016
... - Introducing the laser and its major concepts: pumping, population inversion, threshold, gain and its saturation, feedback and cavities. Examples of major classes of laser (gaz, liquid, solid state), - Properties of the laser beam: particularly ultra-short laser pulses will be introduced in view of ...
... - Introducing the laser and its major concepts: pumping, population inversion, threshold, gain and its saturation, feedback and cavities. Examples of major classes of laser (gaz, liquid, solid state), - Properties of the laser beam: particularly ultra-short laser pulses will be introduced in view of ...
Detecting tissue optical and mechanical properties with an
... Measuring optical and mechanical properties of biological tissue provides complementary information for clinical diagnosis. One challenge in medical optical imaging is the multiple scattering of light in tissue, which can severely degrade image resolution. To improve the image resolution at depth, s ...
... Measuring optical and mechanical properties of biological tissue provides complementary information for clinical diagnosis. One challenge in medical optical imaging is the multiple scattering of light in tissue, which can severely degrade image resolution. To improve the image resolution at depth, s ...
Coupled-mode theory for electromagnetic pulse propagation in
... (or nonadiabatic/diabatic) perturbations were studied based on the field discontinuities, identified first in [48], and then used in several followup studies; see, e.g., [49–55]. Some additional simple [11] or even more complex cases have exact solutions; see, e.g., [56,57]. Studies of wave propagat ...
... (or nonadiabatic/diabatic) perturbations were studied based on the field discontinuities, identified first in [48], and then used in several followup studies; see, e.g., [49–55]. Some additional simple [11] or even more complex cases have exact solutions; see, e.g., [56,57]. Studies of wave propagat ...
Photonic laser thruster
A photonic laser thruster is an amplified laser thruster that generates thrust directly from the laser photon momentum, rather than laser-heating propellant. The concept of single-bounce laser-pushed lightsails that utilize the photon momentum was first developed in the 1960s, however, its conversion of laser power to thrust is highly inefficient, thus has been considered impractical. Over 50 years, there had been numerous theoretical and experimental efforts to increase the conversion efficiency by recycling photons, bouncing them repetitively between two reflective mirrors in an empty optical cavity, without success. In December 2006, Young Bae successfully solved this problem and demonstrated the conversion efficiency enhancement by a factor of 100 and a photon thrust of 35 micronewtons by putting the laser energizing media between the two mirrors as in typical lasers, and the photonic laser thruster was born. In August 2015, the photonic laser thruster was demonstrated to increase the conversion efficiency enhancement by a factor over 1,000 and to achieve a photon thrust of 3.5 millinewtons at Y.K. Bae Corporation. In addition, Propelling, slowing and stopping of a small satellite, 1U CubeSat, in simulated zero-gravity were demonstrated. The photonic laser thruster was initially developed for use in nanometer precision spacecraft formation, for forming ultralarge space telescopes and radars. The photonic laser thruster is currently developed for high-precision and high-speed maneuver of small spacecraft, such as formation flying, orbit adjustments, drag compensation, and rendezvous and docking. The photonic laser thruster can be used for beaming thrust from a conventional heavy resource vehicle to a more expensive & lightweight mission vehicle, similar to tankers in aerial refueling.The practical usage of the photonic laser thruster for main space propulsion would require extremely high laser powers and overcoming technological challenges in achieving the laser power and fabricating the required optics. Photonic laser thrusters have a very high specific impulse, and can permit spacecraft reach much higher speeds than with conventional rockets, which are limited by the Tsiolkovsky rocket equation. If the photonic laser thruster is scalable for the use in such main space propulsion, multiple photonic laser thrusters can be used to construct a 'photonic railway' that has been proposed as a potential permanent transport infrastructure for interplanetary or interstellar commutes, allowing the transport craft themselves to carry very little fuel.