Imaging and focusing of an atomic beam with a large period
... lens is very thin offers new perspectives for deep focusing into the nm range. PACS: 32.80.-t, 42.50.Vk, 07.77.+P i ...
... lens is very thin offers new perspectives for deep focusing into the nm range. PACS: 32.80.-t, 42.50.Vk, 07.77.+P i ...
Theory of the transmission properties of an optical far-field superlens
... transmitted and incident transverse wavenumbers, respectively; ⌳ = 2 / d is the grating wavenumber, where d is the periodicity; and p is the diffraction order. We are interested only in waves transmitted in the far field, i.e., far enough from the FSL and the object plan that the contribution of ev ...
... transmitted and incident transverse wavenumbers, respectively; ⌳ = 2 / d is the grating wavenumber, where d is the periodicity; and p is the diffraction order. We are interested only in waves transmitted in the far field, i.e., far enough from the FSL and the object plan that the contribution of ev ...
Document
... through which the ray travels, and a less dense medium (air). There is no phase change on reflection from such an interface, just as there is no phase change when a wave on a string is reflected from a free end of the string. The second ray is reflected at an interface between an optically less dens ...
... through which the ray travels, and a less dense medium (air). There is no phase change on reflection from such an interface, just as there is no phase change when a wave on a string is reflected from a free end of the string. The second ray is reflected at an interface between an optically less dens ...
Course: Physics 1 Module 3: Optics and Wave Phenomena
... 5) Spherical and plane waves • If a small spherical body, considered as a point, oscillates so that its radius varies sinusoidally with time, a spherical wave is produced, as shown in Figure 26. The wave moves outward from the source in all directions, at a constant speed if the medium is uniform. ...
... 5) Spherical and plane waves • If a small spherical body, considered as a point, oscillates so that its radius varies sinusoidally with time, a spherical wave is produced, as shown in Figure 26. The wave moves outward from the source in all directions, at a constant speed if the medium is uniform. ...
1 Introduction to Optics and Photophysics - Wiley-VCH
... when trying to look at a scene through a glass full of water. Even though these two effects may look very different at first glance, both of these effects are ultimately based on interference, as discussed here. Diffraction is most prominent when light illuminates structures (such as a grating) of a ...
... when trying to look at a scene through a glass full of water. Even though these two effects may look very different at first glance, both of these effects are ultimately based on interference, as discussed here. Diffraction is most prominent when light illuminates structures (such as a grating) of a ...
Experimental observation of the far field diffraction patterns of
... [1-7]. In particular, concentric ring intensity distribution pattern can be induced in the far field of a beam after propagation through a nonlinear material. This effect of spatial phase-modulation (SPM) is due to the intensitydependent complex refractive index and it has been observed in several s ...
... [1-7]. In particular, concentric ring intensity distribution pattern can be induced in the far field of a beam after propagation through a nonlinear material. This effect of spatial phase-modulation (SPM) is due to the intensitydependent complex refractive index and it has been observed in several s ...
Fourier Optics Laboratory Manual - McGill Undergraduate Physics Lab
... This experiment will study optical wave phenomena that are very dependent of interference, that is, the ability of several beams of light to interact with each other. For that to happen, the light of the beams must be at the same frequency and must be coherent. The use of a Laser is therefore approp ...
... This experiment will study optical wave phenomena that are very dependent of interference, that is, the ability of several beams of light to interact with each other. For that to happen, the light of the beams must be at the same frequency and must be coherent. The use of a Laser is therefore approp ...
Persistent spectral hole burning in an organic material for temporal
... reference pattern is recorded in a persistent spectral holeburning material. The reference image has to include phase and amplitude information. In order to record a field-amplitude distribution in a quadratic photosensitive material, one usually engraves the interference pattern of a known field an ...
... reference pattern is recorded in a persistent spectral holeburning material. The reference image has to include phase and amplitude information. In order to record a field-amplitude distribution in a quadratic photosensitive material, one usually engraves the interference pattern of a known field an ...
Beyond Snel`s law: Refraction of a nano-beam of light.
... direction of propagation changes. If the light is a wide plane wave incident on a relatively large and flat interface of two different isotropic media, the change of wave direction is well described by Snel’s law. Snel’s Law of refraction is one of the oldest fundamental laws of optics [1] used in vi ...
... direction of propagation changes. If the light is a wide plane wave incident on a relatively large and flat interface of two different isotropic media, the change of wave direction is well described by Snel’s law. Snel’s Law of refraction is one of the oldest fundamental laws of optics [1] used in vi ...
microscopy DAMOP poster - Yavuz Lab!
... include a nanotube mounted in an ultracold atomic cloud, similar to Fig. 3. The cloud can be obtained through standard Magneto-Optical Trap and Far-Off Resonant Dipole Trap techniques. If our volume of excitation is (50 nm)3 ≈ 10-16 cm3 in an ultracold atomic cloud with density N = 1014 cm-3 [8], th ...
... include a nanotube mounted in an ultracold atomic cloud, similar to Fig. 3. The cloud can be obtained through standard Magneto-Optical Trap and Far-Off Resonant Dipole Trap techniques. If our volume of excitation is (50 nm)3 ≈ 10-16 cm3 in an ultracold atomic cloud with density N = 1014 cm-3 [8], th ...
The wave model of light explains diffraction and interference.
... Light from O passes through slits A and B and produces an interference pattern on the screen at the right. ...
... Light from O passes through slits A and B and produces an interference pattern on the screen at the right. ...
31 Diffraction and Interference
... Light from O passes through slits A and B and produces an interference pattern on the screen at the right. ...
... Light from O passes through slits A and B and produces an interference pattern on the screen at the right. ...
Short-pulse limits in optical instrumentation design for the S
... short-pulse effects and their incorporation into phase-space transport through, and design of, optical elements is still lacking. For example, although in the present work we conducted our assessments of short-pulse effects primarily in spatio-temporal terms, an equivalent discussion could have been ...
... short-pulse effects and their incorporation into phase-space transport through, and design of, optical elements is still lacking. For example, although in the present work we conducted our assessments of short-pulse effects primarily in spatio-temporal terms, an equivalent discussion could have been ...
A1990DA63800001
... must typically be explored to find the singularity. Thom realized that his classification described optical caustics (via Fermat’s principle, according to which a family of light rays is a gradient map generated by the travel time function). In catastrophe theory an important idea is that the causti ...
... must typically be explored to find the singularity. Thom realized that his classification described optical caustics (via Fermat’s principle, according to which a family of light rays is a gradient map generated by the travel time function). In catastrophe theory an important idea is that the causti ...
Observation of the rotational Doppler shift of a white
... The linear Doppler shift is usually associated with the lineof-sight component of velocity between the source and observer. However, the Doppler effect can also be observed from transverse motion. If a moving rough surface is illuminated at an oblique angle, the light of frequency ω0 scattered at no ...
... The linear Doppler shift is usually associated with the lineof-sight component of velocity between the source and observer. However, the Doppler effect can also be observed from transverse motion. If a moving rough surface is illuminated at an oblique angle, the light of frequency ω0 scattered at no ...
Polarization Physics 227 Lab Purpose The purpose of this
... polarizer, only half will be transmitted though the polarizer. (Since in reality no polarizer is ”ideal”, less than half the light will be transmitted.) The transmitted light is polarized in one plane. If this polarized light is incident upon a second polarizer, the axis of which is oriented such th ...
... polarizer, only half will be transmitted though the polarizer. (Since in reality no polarizer is ”ideal”, less than half the light will be transmitted.) The transmitted light is polarized in one plane. If this polarized light is incident upon a second polarizer, the axis of which is oriented such th ...
X-Ray standing waves for investigation of periodic multilayers.
... 2.5 X-Ray standing waves from layered synthetic periodic multilayers. For Bragg diffraction purposes, a layered-synthetic microstructure (LSM) is fabricated (typically by sputter deposition) to have a depth-periodic layered structure consisting of 10 to 200 layer pairs of alternating high- and low-e ...
... 2.5 X-Ray standing waves from layered synthetic periodic multilayers. For Bragg diffraction purposes, a layered-synthetic microstructure (LSM) is fabricated (typically by sputter deposition) to have a depth-periodic layered structure consisting of 10 to 200 layer pairs of alternating high- and low-e ...
Diffracting fractals: new paradigms in linear wave physics
... Figure 5: Diffraction of the Weierstrass fractal function [Eq. (1)] with random phases for different values of the dimension D at a single slit when D = 1.99. (a) NF = 5, (b) NF = 10, (c) NF = 30, (d) NF = 50. Other parameters: = 1.2, /a = 1.0, L/k = 1, and = 0.1. Shaded areas denote geometric ...
... Figure 5: Diffraction of the Weierstrass fractal function [Eq. (1)] with random phases for different values of the dimension D at a single slit when D = 1.99. (a) NF = 5, (b) NF = 10, (c) NF = 30, (d) NF = 50. Other parameters: = 1.2, /a = 1.0, L/k = 1, and = 0.1. Shaded areas denote geometric ...
Introduction to Phase Contrast
... The phase outfit, as supplied by the manufacturer, usually includes a green filter and a phase telescope. The latter is used to enable the microscopist to alight the condenser annulus to superimpose it onto the ring of the phase plate. A set of centering screws in the substage condenser allows manip ...
... The phase outfit, as supplied by the manufacturer, usually includes a green filter and a phase telescope. The latter is used to enable the microscopist to alight the condenser annulus to superimpose it onto the ring of the phase plate. A set of centering screws in the substage condenser allows manip ...
Imaging Spatial-Helical Mode Interference of Single Photons
... In summary, we present measurements of the probability distribution of single photons in a superposition of two spatial modes. The imaged pattern had an off-center helical wavefront, which is the result of the superposition of ℓ = 1 and ℓ = 0 modes. The results show strong evidence of single-photon ...
... In summary, we present measurements of the probability distribution of single photons in a superposition of two spatial modes. The imaged pattern had an off-center helical wavefront, which is the result of the superposition of ℓ = 1 and ℓ = 0 modes. The results show strong evidence of single-photon ...
Review !x
... ! We can see that the intensity varies from 0 to 4Imax ! Covering one slit, we get a constant intensity of Imax ! If we illuminate both slits with light that has random phases, we would observe a constant intensity of 2Imax ! Only when we illuminate both slits with coherent light do we observe the o ...
... ! We can see that the intensity varies from 0 to 4Imax ! Covering one slit, we get a constant intensity of Imax ! If we illuminate both slits with light that has random phases, we would observe a constant intensity of 2Imax ! Only when we illuminate both slits with coherent light do we observe the o ...
Winter 2008 exam 1 - BYU Physics and Astronomy
... 1. T or F: The real part of the refractive index cannot be less than one. 2. T or F: s-polarized and p-polarized light experience different phase shifts upon reflection from a material with a complex index of refraction. 3. T or F: When light is incident upon a material interface at Brewster’s angle ...
... 1. T or F: The real part of the refractive index cannot be less than one. 2. T or F: s-polarized and p-polarized light experience different phase shifts upon reflection from a material with a complex index of refraction. 3. T or F: When light is incident upon a material interface at Brewster’s angle ...
Conference title, upper and lower case, bolded, 18 point
... ηi=0.39, internal loss <αi>=11 cm-1, bimolecular coefficient B=10-10 cm3/s, auger recombination coefficient C=3.5×10-30 cm6/s, empirical gain parameter g0=966 cm-1, carrier density at transparency Ntr=1.8×1018/cm3 together with estimated pitch of grating, coupling coefficient and mirror loss to calc ...
... ηi=0.39, internal loss <αi>=11 cm-1, bimolecular coefficient B=10-10 cm3/s, auger recombination coefficient C=3.5×10-30 cm6/s, empirical gain parameter g0=966 cm-1, carrier density at transparency Ntr=1.8×1018/cm3 together with estimated pitch of grating, coupling coefficient and mirror loss to calc ...
Diffraction grating
In optics, a diffraction grating is an optical component with a periodic structure, which splits and diffracts light into several beams travelling in different directions. The emerging coloration is a form of structural coloration. The directions of these beams depend on the spacing of the grating and the wavelength of the light so that the grating acts as the dispersive element. Because of this, gratings are commonly used in monochromators and spectrometers.For practical applications, gratings generally have ridges or rulings on their surface rather than dark lines. Such gratings can be either transmissive or reflective. Gratings which modulate the phase rather than the amplitude of the incident light are also produced, frequently using holography.The principles of diffraction gratings were discovered by James Gregory, about a year after Newton's prism experiments, initially with items such as bird feathers. The first man-made diffraction grating was made around 1785 by Philadelphia inventor David Rittenhouse, who strung hairs between two finely threaded screws. This was similar to notable German physicist Joseph von Fraunhofer's wire diffraction grating in 1821.Diffraction can create ""rainbow"" colors when illuminated by a wide spectrum (e.g., continuous) light source. The sparkling effects from the closely spaced narrow tracks on optical storage disks such as CD's or DVDs are an example, while the similar rainbow effects caused by thin layers of oil (or gasoline, etc.) on water are not caused by a grating, but rather by interference effects in reflections from the closely spaced transmissive layers (see Examples, below). A grating has parallel lines, while a CD has a spiral of finely-spaced data tracks. Diffraction colors also appear when one looks at a bright point source through a translucent fine-pitch umbrella-fabric covering. Decorative patterned plastic films based on reflective grating patches are very inexpensive, and are commonplace.