scholarly journals Unified Fano-like interference picture for charmoniumlike statesY(4008),Y(4260)andY(4360)

2016 ◽  
Vol 93 (1) ◽  
Author(s):  
Dian-Yong Chen ◽  
Xiang Liu ◽  
Xue-Qian Li ◽  
Hong-Wei Ke
Keyword(s):  
Interference Picture

RESULTS OF POLARIZED LIGHT USE FOR STUDY OF STRESS-STRAIN STATE OF CORNEA IN PATHOLOGY OF EXTRAOCULAR MUSCLES

2020 ◽  
pp. 65-69
Author(s):  
Nataliia Mykhailivna Kovtun ◽  
Ihor Volodymyrovych Kaplin
Keyword(s):  
Interference Pattern ◽  
Optical Anisotropy ◽  
Extraocular Muscle ◽  
Strain State ◽  
Polarized Light ◽  
Attachment Site ◽  
Rectus Muscle ◽  
Extraocular Muscles ◽  
Asymmetric Distortion ◽  
Interference Picture

The parameters of interference patterns observed on the cornea in a polarized light in pathology of extraocular muscles were quantitatively evaluated. A study of the shape of 147 interference patterns observed on the cornea in a polarized light showed that the horizontal deviation of an eye in 56 % of cases was caused by the displacement of the attachment of the upper rectus muscle towards the inner rectus muscle. During illumination of the cornea of a live eye with polarized light, a specific interference pattern in the form of a rhombus formed by rainbow stripes (isochromes) is observed. It is established that such an interference pattern is the result of the influence of extraocular muscles on the cornea. The findings showed that the weakening of the force of one of muscles leads to asymmetric distortion of the shape of the interference rhombus, which is manifested with a reduced length of the corresponding section of the diagonal. On the contrary, as the force of the muscle increases, the corresponding section of the diagonal enhances. The displacement of the attachment site of direct extraocular muscle along the line of action is equivalent to a change in effort on its part, indicated appropriately by the shape of the interference rhombus. As the muscle moves away from the line of action, the angle of the interference rhombus is shifted away from the corresponding meridian. Key words: polarized light, optical anisotropy, cornea, extra−ocular muscles, interference picture.

scholarly journals Connecting Fano interference and the Jaynes-Cummings model in cavity magnonics

2021 ◽  
Vol 7 (1) ◽  
Author(s):  
Jakob Gollwitzer ◽  
Lars Bocklage ◽  
Ralf Röhlsberger ◽  
Guido Meier
Keyword(s):  
Cross Section ◽  
Coupling Strength ◽  
Room Temperature ◽  
Optical Model ◽  
Microwave Cavity ◽  
Additional Contribution ◽  
Fano Interference ◽  
Quantum Optical ◽  
Interference Picture ◽  
Photon Coupling

AbstractWe show that Fano interference can be realized in a macroscopic microwave cavity coupled to a spin ensemble at room temperature. Via a formalism developed from the linearized Jaynes-Cummings model of cavity electromagnonics, we show that generalized Fano interference emerges from the photon–magnon interaction at low cooperativity. In this regime, the reflectivity approximates the scattering cross-section derived from the Fano-Anderson model. Although asymmetric lineshapes in this system are often associated with the Fano formalism, we show that whilst Fano interference is actually present, an exact Fano form cannot be achieved from the linear Jaynes-Cummings model. In the Fano model an additional contribution arises, which is attributed to decoherence in other systems, and in this case is due to the resonant nature of the photonic mode. The formalism is experimentally verified and accounts for the asymmetric lineshapes arising from the interaction between magnon and photon channels. As the magnon–photon coupling strength is increased, these channels merge into hybridized magnon–photon modes and the generalized Fano interference picture breaks down. Our results are universally applicable to systems underlying the linearized Jaynes-Cummings Hamiltonian at low cooperativity and connect the microscopic parameters of the quantum optical model to generalized Fano lineshapes.

scholarly journals Orientational characteristics of magnetization precession excitation on the interference grating formed by femtosecond laser.

2021 ◽  
Author(s):  
V.S. Vlasov ◽  
Keyword(s):  
Magnetic Field ◽  
Femtosecond Laser ◽  
Magnetic Film ◽  
Theoretical Interpretation ◽  
Deformation Tensor ◽  
Constant Field ◽  
Polarization Rotation ◽  
Leaky Waves ◽  
Magnetization Precession ◽  
Interference Picture

The subject of investigation in this work is the excitation of magnetization precession in magnetic film on the surface of which is formed the temperature relief which is formed by interference picture formatted by preliminary divided ray from femtosecond laser. It is mentioned the discovered in experiment the dependence of excitation efficiency from the orientation of magnetic field applied in the plane of film. The main aim of this work is the theoretical interpretation of observed orientation dependence. The realized in experiment scheme “pump-probe” is described. The whole geometry of task is proposed. This geometry includes in oneself the magnetic film with formed in its surface interference picture and applied in the plane of film the constant field. It is shown that by the thermal expansion in the film the elastic waves two types are excited; the surface Rayleigh waves and leaky longitudinal waves. The projections of wave-vectors of propagating waves to plane of film are normal to the strips of interference picture. The orientation of field may change from to longitudinal to transverse from the same strips. The components of deformation tensor of Rayleigh and leaky waves are determined. The precession of magnetization in the coordinate system connected with field is investigated. By using the apparatus of crossing matrixes it is found the components of deformation tensor are determined. In the frame of linear approach in this system the task about excitation of magnetization precession by elastic deformations by Rayleigh and leaky waves is solved. The dynamical component of magnetization precession which ensures the light polarization rotation which passes along the normal to the plane of film is found. It is shown that the angle of rotation is straight proportional to the tensor deformation components with the summarization with the resonance character of precession magnetization dependence from the value of magnetic field. The dependence of polarization rotation from orientation of field which is applied in the plane of film is found. It is shown that by the orientation of field along and across the interference stripes the rotation of polarization plane is absent. Between these extreme orientations the dependence has appearance as two maxima divided by deep minimum. The received results are compared with data of experiment. It is found the quality and in some cases quantity correlation. The recommendations for further development of work are proposed.

NANOSCALE PERIODICAL STRUCTURES FABRICATED BY INTERFERENCE PHOTOLITHOGRAPHY

2004 ◽  
Vol 03 (01n02) ◽  
pp. 59-64 ◽  
Author(s):  
S. I. NESTEROV ◽  
D. V. MYAGKOV ◽  
E. L. PORTNOI
Keyword(s):  
Development Process ◽  
Light Wave ◽  
Exposure Dose ◽  
Minimum Size ◽  
Optimal Conditions ◽  
Minimal Size ◽  
Coherent Light ◽  
Standing Light Wave ◽  
Wide Line ◽  
Interference Picture

The possibility of periodical mask fabrication with elements of minimal size by means of interference photolithography is considered. The method is based on application of striped interference picture of coherent light for photoresist exposition. The investigation of inorganic photoresist based on chalcogenide glass As 2 S 3 reveals high resolution, sufficient contrast and vertical edge of the masks stripe. The influence of exposure dose and development parameters on photoresist profile are analyzed with the help of the method of computer simulation of the development process. The possibility of decreasing the effect of standing light wave by means of additional homogeneous light irradiation is demonstrated. The optimal conditions for minimum size elements fabrication are found, which enables fabrication of periodical grating with a 80-nm-wide line and two-dimensional periodical structures with pillars of 50 nm cross-section.

Reciprocal Space X-Ray Mapping and Transmission Electron Microscopic Studies of Coincided δ-Inas and As-Cluster Superlattices in Gaas Films Grown by Molecular-Beam Epitaxy at Low Temperature

1999 ◽  
Vol 583 ◽  
Author(s):  
V. V. Chaldyshev ◽  
N. A. Bert ◽  
N. N. Faleev ◽  
Yu. G. Musikhin ◽  
A. E. Kunitsyn ◽  
...  
Keyword(s):  
Molecular Beam Epitaxy ◽  
Molecular Beam ◽  
Reciprocal Space ◽  
Growth Surface ◽  
Electron Microscopic ◽  
Extended Defect ◽  
X Ray ◽  
Transmission Electron ◽  
Transmission Electron Microscopic ◽  
Interference Picture

AbstractInAs/GaAs superlattices with thin (0.5–1 monolayer) δ-InAs insertions were grown by molecular beam epitaxy at low (150–200°C) temperature. The as-grown samples contained up to 1020 cm−3 arsenic antisite defects. Transmission electron microscopic study revealed no extended defect and showed that the real thickness of δ-InAs insertions is 3–4 monolayers. This thickness seems to be due to short-range roughness of the growth surface. Low diffuse scattering and extended interference picture were observed for such superlattices by x-ray diffraction study. Superlattices of two-dimensional cluster sheets were produced by annealing of the δ-InAs/GaAs superlattices at 500–600°C. Precipitation of excess arsenic at InAs δ-layers was found to be accompanied by enhanced In-Ga intermixing, roughening the InAs δ-layers, and smoothing the x-ray interference picture. No evidence for any self-ordering in the system of nanoscale As clusters was revealed using x-ray mapping in reciprocal space.

A Novel Method to Determine EHL Film Thickness with Optical Interference

2013 ◽  
Vol 456 ◽  
pp. 549-554 ◽  
Author(s):  
Qian Qian Yang ◽  
Ying Jun Chen ◽  
Huang Ping
Keyword(s):  
Film Thickness ◽  
Theoretical Result ◽  
Working Conditions ◽  
Contact Area ◽  
Second Grade ◽  
Optical Intensity ◽  
Sliding Speed ◽  
Glass Disc ◽  
Novel Method ◽  
Interference Picture

In this work, a new method to determine the interference grade of the central film is put forward. The interference figure is generated on a steel ball and a glass disc with a green monochromatic two-beam interferometry. With gradually increasing the rotational speed of the glass disc, the corresponding interference intensities of the central contact area are continually collected and sent to the computer. With these data, the periodical curve of the central interference grey value with the sliding speed has been drawn. Then, the curve is compared with the theoretical result so that the central interference grade of each figure can be determined. It has been found that while the sliding speed varies from 0.09 m/s to 0.21 m/s, the central interference grade of the interference figure is the first under the working conditions of the present paper. As the sliding speed increases between 0.21 m/s and 0.4 m/s, the second grade of the central interference figure is achieved. As the central interference grade has been known, the film thickness and the film shape can be easily determined by the interference picture of the EHL film and the relative optical intensity principle.

Contact Region of a Hard Ball Rolling on a Viscoelastic Plate

1968 ◽  
Vol 90 (1) ◽  
pp. 101-105 ◽  
Author(s):  
J. Halaunbrenner ◽  
A. Kubisz
Keyword(s):  
Contact Area ◽  
Contact Region ◽  
Superposition Principle ◽  
Viscoelastic Plate ◽  
Observation Data ◽  
Relaxation Functions ◽  
Ball Rolling ◽  
Mutually Independent ◽  
Interference Picture ◽  
Hard Ball

In the work presented, the contact region of a glass ball rolling without slip on a flat plate of viscoelastic material at various velocities was recorded. An interference microscope was used. Deformation of the base in the vicinity of the contact area was read from the interference picture obtained due to a narrow air gap between the ball and the base. The material of the base was characterized by creep and relaxation functions at constant temperature of (21 ± 0.5) deg C. The viscoelastic continuum of the base was replaced by the system of mutually independent vertical columns. By a subsequent twofold application of Boltzmann’s superposition principle, the diameter of the contact surface parallel to the velocity vector of the ball and depth of the concave track behind the ball were calculated. The results obtained were compared with observation data. Satisfactory agreement in cases where the shape of the contact area does not differ considerably from a circle (for small and great rolling velocities) was obtained.

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