Diffractive lens for controlling the focal length and depth of focus by using binary structure of grating and diffractive condenser lens for laser processing application

2018 ◽  
Author(s):  
Atsushi Motoagito ◽  
Yosuke Iguchi ◽  
Shuji Kato
Author(s):  
A. V. Crewe

A 100 kv transmission scanning microscope is now being constructed which should have a point resolution of 2.5 to 3 Å. The design of this microscope is similar to the design of our existing 30 kv 5 Å microscope, but there are several significant changes which are based upon some difficulties and sources of inflexibility of that microscope.A field emission electron gun of our usual design will be used as the source of electrons, the only difference being that the spacing between the anodes has been increased from 2 to 3 cm. The electron beam will then pass through a condenser lens which will produce a parallel beam of electrons. This parallel beam will then be focused onto the specimen by means of a short focal length lens (approximately 1 mm focal length). The reason for using a condenser lens to produce the parallel beam of electrons is that in the future a quadrupole-octupole correction system will be installed in this section of the microscope in order to attempt to correct the spherical aberrations of the objective lens and thereby improve its resolution.


2020 ◽  
Vol 10 (15) ◽  
pp. 5237
Author(s):  
Simo Wang ◽  
Siyang Yu ◽  
Fanxing Li ◽  
Fuping Peng ◽  
Jialin Du ◽  
...  

The movable super-diffraction optical needle (MSON) is a tightly focused beam like a “needle”, which can realize vector scanning on the focusing plane. Not only does it have a long focal depth, but its resolution also exceeds the diffraction limit. The modulation and control technology required for generating MSON by oblique incidence is explored in this manuscript for the purpose of processing high-aspect-ratio, sub-wavelength structures. As the optical needle generated by traditional methods is static and sensitive to variation of the angle information of the incident beam, here we introduce a confocal scanning system by using a two-dimensional galvanometer system, a scan lens, and a tube lens to control the oblique incidence angle. The effects of the oblique incidence angle on the resolution, depth of focus, uniformity, and side lobes of the MSON were analyzed. Further, the voltage-controlled liquid crystal located between the scan lens and the 2D galvanometer system can be used to compensate for the additional phase difference caused by oblique incidence. The aspect ratio is defined as the ratio of depth of focus to resolution. By modulating and controlling the light field, the MSON with high aspect ratio (7.36), sub-diffractive beam size (0.42λ), and long depth of focus (3.09λ) has been obtained with homogeneous intensity, and suppressed side lobes. High speed, high axial positioning tolerance, and high-resolution laser processing can also be achieved, which removes the restrictions presented by traditional laser processing technology, for which high resolution and long depth of focus cannot be achieved simultaneously.


2013 ◽  
Vol 552 ◽  
pp. 38-43
Author(s):  
Jun Yan Zhao ◽  
Guang Hu Du ◽  
Zhi Peng Qin

The effects of temperature changes on the focus of IR optical system are described in this paper, and the general methods used for compensation of thermal effects are analyzed. On this basis, the feasibility of athermalization of long focal length IR optical systems by using of hydraulics is studied, and an athermalization design of an uncooled IR optical system with focal length 200mm and F-number 1 is presented. The result shows that within the temperature range from -30 to 50 °C, the defocus of this system is less than the depth of focus.


Mathematics ◽  
2020 ◽  
Vol 8 (4) ◽  
pp. 581 ◽  
Author(s):  
Kang Min Kim ◽  
Sun-Ho Choe ◽  
Jae-Myung Ryu ◽  
Hojong Choi

When the number of lens groups is large, the zoom locus becomes complicated and thus cannot be determined by analytical means. By the conventional calculation method, it is possible to calculate the zoom locus only when a specific lens group is fixed or the number of lens groups is small. To solve this problem, we employed the Padé approximation to find the locus of each group of zoom lenses as an analytic form of a rational function consisting of the ratio of polynomials, programmed in MATLAB. The Padé approximation is obtained from the initial data of the locus of each lens group. Subsequently, we verify that the obtained locus of lens groups satisfies the effective focal length (EFL) and the back focal length (BFL). Afterwards, the Padé approximation was applied again to confirm that the error of BFL is within the depth of focus for all zoom positions. In this way, the zoom locus for each lens group of the optical system with many moving lens groups was obtained as an analytical rational function. The practicality of this method was verified by application to a complicated zoom lens system with five or more lens groups using preset patents.


2004 ◽  
Vol 43 (30) ◽  
pp. 5618 ◽  
Author(s):  
Angel Flores ◽  
Michael R. Wang ◽  
Jame J. Yang

2020 ◽  
Vol 28 (20) ◽  
pp. 30150
Author(s):  
N. Bregenzer ◽  
T. Öttl ◽  
M. Zobernig ◽  
M. Bawart ◽  
S. Bernet ◽  
...  

Author(s):  
T. Someya ◽  
M. Watanabe

Our electron mirror microscope has been improved by adopting magnetic lenses, which enable a wide range of magnification to be obtained. This improved version, known as the JEM-M1 (35kV acceleration) uses the straight design and shadow projection method.The construction of the newly designed instrument is illustrated in Fig. 1 and Fig. 2 shows a sectional view of its electron optical column. The electron gun assembly is located under the console table. Incident beam alignment is carried out by means of the deflection coil knob, the electron gun horizontal movement knob and the condenser lens knob located on the table. The zircaloy crystal located above the screen and on the optical axis enables the alignment procedure to be carried out easily and simply because it radiates light when impinged by the electron beam. The projector lens, having a short focal length, combined with the condenser lens, forms a small source for the shadow projection image on its back focal plane. The intermediate lens, acting on the reflected beam, produces image magnification by changing the excitation current. Magnification in the range x200 – x1500 is possible without any appreciable distortion.


Sign in / Sign up

Export Citation Format

Share Document