Visualization of polarization state and its application in Optics classroom teaching

Similar documents
: Imaging Systems Laboratory II. Laboratory 6: The Polarization of Light April 16 & 18, 2002

Lab #13: Polarization

PROCEEDINGS OF SPIE. Modulation of visualized electrical field. Chin-Jung Chuang, Chi-Chung Wu, Yi-Ting Wang, Shiuan-Hau Huang

PROCEEDINGS OF SPIE. Optical circulator analysis and optimization: a mini-project for physical optics

16. More About Polarization

Polarization of Light and Birefringence of Materials

PROCEEDINGS OF SPIE. FDTD method and models in optical education. Xiaogang Lin, Nan Wan, Lingdong Weng, Hao Zhu, Jihe Du

PROCEEDINGS OF SPIE. Teaching the concept of convolution and correlation using Fourier transform

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

PROCEEDINGS OF SPIE. Optical phase measurement emphasized

Design of a Multi-Mode Interference Crossing Structure for Three Periodic Dielectric Waveguides

LECTURE 11 ELECTROMAGNETIC WAVES & POLARIZATION. Instructor: Kazumi Tolich

Experiment 8. Fresnel Coefficients. 8.1 Introduction. References

PROCEEDINGS OF SPIE. Student activity: verification on Malus's law of polarization at low cost. Shahrul Kadri, David Chong, Bor Wei, Rosly Jaafar

Fundamentals of Photoelasticity

POLARIZATION OF LIGHT

Chap. 5. Jones Calculus and Its Application to Birefringent Optical Systems

Polarization Puzzles for the Upper Elementary Grades

Lecture PowerPoints. Chapter 24 Physics: Principles with Applications, 7 th edition Giancoli

PROCEEDINGS OF SPIE. Photonic simulation software tools for education

Identifying the crystal orientation of the black phosphorus

Experiment 5 Polarization and Modulation of Light

Lab 2: Mach Zender Interferometer Overview

2. OPERATIONAL CONDITIONS

Physics I Keystone Institute Technology & Management Unit-II

ECEN 4606, UNDERGRADUATE OPTICS LAB

POLARISATION. We have not really discussed the direction of the Electric field other that that it is perpendicular to the direction of motion.

REFLECTION AND REFRACTION

Polarized Light. Nikki Truss. Abstract:

NAWAB SHAH ALAM KHAN COLLEGE OF ENGINEERING & TECHNOLOGY UNIT II-a POLARISATION

E The oscillating E-field defines the polarization of the wave. B

Physics 214 Course Overview

Lab 8 - POLARIZATION

Waves & Oscillations

polarisation of Light

PH 222-2C Fall Electromagnetic Waves Lectures Chapter 33 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition)

OPSE FINAL EXAM Fall 2015 YOU MUST SHOW YOUR WORK. ANSWERS THAT ARE NOT JUSTIFIED WILL BE GIVEN ZERO CREDIT.

1. In Young s double slit experiment, when the illumination is white light, the higherorder fringes are in color.

Atomic and nuclear physics

Chapter 34. Electromagnetic Waves

Topic 4: Waves 4.3 Wave characteristics

Model 556X User s Manual. Optical Isolator

Light Waves and Polarization

arxiv: v1 [physics.optics] 30 Mar 2010

Lecture 4: Polarisation of light, introduction

Physics 313: Laboratory 8 - Polarization of Light Electric Fields

Lab 11 - Polarization

Lecture 8 Notes, Electromagnetic Theory II Dr. Christopher S. Baird, faculty.uml.edu/cbaird University of Massachusetts Lowell

The Zeeman Effect refers to the splitting of spectral

Lab 11 - Polarization

Experiment and Simulation Study on A New Structure of Full Optical Fiber Current Sensor

ABSTRACT 1. INTRODUCTION

Lab 8 - Polarization

Polarization of Light

Polarization of light

PHY410 Optics Exam #3

Photonic Simulation Software Tools for Education

PROCEEDINGS OF SPIE. Quantum optics laboratories for undergraduates

More Optical Telescopes

Waveplate analyzer using binary magneto-optic rotators

Double-distance propagation of Gaussian beams passing through a tilted cat-eye optical lens in a turbulent atmosphere

Waves & Oscillations

ON MICROMETRIC PATTERN FORMATION IN MAGNETIC FLUIDS THIN FILMS

Measurement of the velocities of dielectric particles in ER fluids with laser speckle

TOP LATERAL REFRACTION AND REFLECTION OF POLARIZED LIGHT IN LENSES

Polarization properties of corner-cube retroreflectors: Theory and experiment

A NEW AUTOMATED MEASURING INSTRUMENT FOR MINUTE PHOTOELASTICITY

Quarter wave plates and Jones calculus for optical system

Electromagnetic Waves. Chapter 33 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition)

Deviations from Malus Law

Single-shot measurement of free-electron laser polarization at SDUV-FEL

A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth.

Chapter 5. Past and Proposed Experiments Detecting Absolute Motion

1. Consider the biconvex thick lens shown in the figure below, made from transparent material with index n and thickness L.

Design of Integrated Error Compensating System for the Portable Flexible CMMs

Chapter 33. Electromagnetic Waves

C. Incorrect! The velocity of electromagnetic waves in a vacuum is the same, 3.14 x 10 8 m/s.

Zeeman Effect. Alex Povilus Physics 441- Fall 2003 December 20, 2003

Testing stress birefringence of an optical window. Chiayu Ai and. James C. Wyant. WYKO Corp., 2650 E. Elvira Road, Tucson, AZ ABSTRACT

Simple and Low Cost Polarimeter System

Phase Sensitive Faraday Rotation in. and various Diamagnetic liquid Samples

PROCEEDINGS OF SPIE. Shedding the light on spectrophotometry: the SpecUP educational spectrophotometer

Gravitational field around blackhole induces photonic spin-orbit interaction that twists. light

A COMPACT POLARIZATION BEAM SPLITTER BASED ON A MULTIMODE PHOTONIC CRYSTAL WAVEGUIDE WITH AN INTERNAL PHOTONIC CRYSTAL SECTION

Computer Modelling and Numerical Simulation of the Solid State Diode Pumped Nd 3+ :YAG Laser with Intracavity Saturable Absorber

Optics of Liquid Crystal Displays

Polarizers and Retarders

Probing the orbital angular momentum of light with a multipoint interferometer

Study of Steady and Transient Thermal Behavior of High Power Semiconductor Lasers

Physics Test Pack WALCH PUBLISHING

Atomic and nuclear physics

Jones calculus for optical system

Electromagnetic Waves

Experiment O-2. The Michelson Interferometer

Optics Polarization. Lana Sheridan. June 20, De Anza College

Light for which the orientation of the electric field is constant although its magnitude and sign vary in time.

90 degree polarization rotator using a bilayered chiral metamaterial with giant optical activity

JRE Group of Institutions ASSIGNMENT # 1 Special Theory of Relativity

Experiment 2-7. Planck constant measurement. using photoelectric effect

Transcription:

Visualization of polarization state and its application in Optics classroom teaching Bing Lei 1, *, Wei Liu 1, Jianhua Shi 1, Wei Wang 1, Tianfu Yao 1 and Shugang Liu 2 1 College of Optoelectronic Science and Engineering, National University of Defense Technology, Changsha, Hunan 410073, China 2 Heilongjiang University, Harbin, Heilongjiang 150080, China ABSTRACT Polarization of light and the related knowledge are key and difficult points in optical teaching, and they are difficult to be understood since they are very abstract concepts. To help students understand the polarization properties of light, some classroom demonstration experiments have been constructed by employing the optical source, polarizers, wave plates optical cage system and polarization axis finder (PAF). The PAF is a polarization indicating device with many linear polarizing components concentric circles, which can visualize the polarization axis s direction of linearly polarized light intuitively. With the help of these demonstration experiment systems, the conversion and difference between the linear polarized light and circularly polarized light have been observed directly by inserting or removing a quarter-wave plate. The rotation phenomenon of linearly polarized light s polarization axis when it propagates through an optical active medium has been observed and studied in experiment, and the strain distribution of some mounted and unmounted lenses have also been demonstrated and observed in experiment conveniently. Furthermore, some typical polarization targets, such as liquid crystal display (LCD), polarized dark glass and skylight, have been observed based on PAF, which is quite suitable to help students understand these targets polarization properties and the related physical laws. Finally, these demonstration experimental systems have been employed in classroom teaching of our university in physical optics, optoelectronics and photoelectric detection courses, and they are very popular with teachers and students. Keywords: Visualization of polarization state, classroom demonstration experiment, polarization axis finder, lens strain detection, optics classroom teaching 1. INTRODUCTION As we all known, light waves traveling in free space or another homogeneous isotropic non-attenuating medium, are properly described as transverse waves, and polarization is the basic performance of electromagnetic wave. However, polarization of light is important and difficult points in optical classroom teaching, and the related knowledge, such as linearly polarized light, circularly polarized light, elliptically polarized light, degree of polarization, polarization angle and direction, are all difficult to be understood since they are non-intuitive concept and really difficult to be observed in experiment [1]. To help students understand the polarization properties of light, a number of classroom demonstration experiments have been constructed by utilizing the optical source, polarizers, wave plates, polarization axis finder (PAF) and optical cage system. The PAF is an unique tool that provides instant indication of the laser beam s polarization axis, and not only no twisting or turning is required, but also measuring minimum and maximum power levels with a power meter is also not needed. The actual direction of the electric vector (i.e. axis of polarization) is indicated directly by an hourglass or bowtie pattern in the beam [2]. In this paper, some polarization related classroom teaching demonstration experimental systems have been constructed to help students understand the key and difficult knowledge points of polarization based on PAF. The working principle and main features of PAF has been introduced firstly. Two different types of polarization axis visualization systems have been made to observe the polarization direction of a light beam, and the optical activity and strain detection experiments have been demonstrated based on the experimental configuration. Finally, the polarization properties of LCD, polarized dark glass and skylight have also been studied by PAF. *leibing_2000@126.com; phone 086 0731-84574749 14th Conference on Education and Training in Optics and Photonics: ETOP 2017, edited by Xu Liu, Xi-Cheng Zhang, Proc. of SPIE Vol. 10452, 1045212 2017 ICO, IEEE, OSA, SPIE CCC code: 0277-786X/17/$18 doi: 10.1117/12.2269496 Proc. of SPIE Vol. 10452 1045212-1

2. VISUALIZATION OF POLARIZATION STATE The polarization axis finder (PAF) is a unique tool with many linear polarizing components concentric circles [3], and real object and schematic diagram are shown in Fig. 1(a) and (b). PAF can be used conveniently, which can indicate the polarization axis direction of linearly polarized light intuitively and instantly, and the changes of polarization state and its stability can also be monitored directly. Moreover, no twisting or rotating is required, and no power meter or photo detector is needed since there is no need to measure minimum and maximum power levels. Transmission axis Transmission axis Radial direction Radial direction (a) Fig. 1 (a) the real object and (b) schematic diagram polarization axis finder (PAF). The working principle of a polarization axis finder indicating the light beam s polarization direction is shown in Fig. 2. An optical source emits unpolarized light without specific polarization axis, and a polarizer is utilized to transfer the unpolarized light into linearly polarized light, then the linearly polarized light s polarization axis, i.e. the actual direction of the electric vector is indicated directly by an hourglass or bowtie pattern in the beam by PAF. Since the PAF is consist of many linear polarizing components concentric circles, and the direction of these tiny linearly polarizers are perpendicular to the radial direction, therefore it is also called angular polarizer. If the small component linearly polarizer is parallel to the direction of input linearly polarized light s axis, in other words, the radial direction is perpendicular to the input beam s polarized axis, the light beam can pass PAF completely and form the bright part of the above bowtie pattern according to the Malus law. Oppositely, when the small component linearly polarizer is perpendicular to the direction of input linearly polarized light s axis, the light beam will be completely blocked by the PAF, and the dark area will be formed in the pattern. The rest polarizers with polarization axis in other directions will partially transmit the input light beam, and form the gradual gray level part of the above bowtie pattern. (b) Fig. 2 The PAF s working principle of indicating the polarization axis of linearly polarized light. Proc. of SPIE Vol. 10452 1045212-2

The experimental configuration of the polarization demonstration system is shown in Fig. 3, and the real object and its effect on polarization indication are shown in Fig. 4(a) and (b) respectively. The demonstration experimental setup is portable and easy to use, and it is quite suitable for classroom teaching and demonstration experiments. Based on the demonstration experimental setup, a series of polarization related phenomena have been observed conveniently. Firstly, the polarization axis s direction of linear polarized light has been observed intuitively. Secondly, the linear polarized light has been conversed to circularly polarized light by inserting a quarter-wave plate, and well-distributed pattern in the beam has been obtained in experiment, which means that no fixed polarization axis exist in circularly polarized light. It is helpful for students to understand the difference between linearly polarized light and circularly polarized light. Thirdly, the strain distribution of a lens has also been demonstrated and observed in experiment conveniently. Fig. 3 Experimental configuration of the polarization demonstration system. (a) (b) Fig. 4 (a) the real object of experimental configuration and (b) its effect of polarization indication. Fig. 5 Two unmounted lens with different strain distribution. The examining configuration of lens strain distribution has been obtained by simply improving the above system. Two polarizers with orthogonal polarization axis have been placed in a certain distance, and the lens needed to be checked is Proc. of SPIE Vol. 10452 1045212-3

set between the two polarizers. If there is uneven strain distribution in the lens, the extra phase difference between two orthogonal polarized modes will be introduced, and uneven intensity distribution will be observed. Two unmounted lens have been examined with the configuration, and the experimental results are shown in Fig. 5. A mounted lens and glasses have also been checked by this setup, and the results are shown in Fig. 6. The red circle shown in Fig. 6 includes a fixed screw, which induces great strain in the lens, and the strain can be indicated obviously in our experimental setup. Based on the experiments, we have clearly found that obvious and large strain exists in the mounted lens due to the mounting pressure, and it provides a simple and effective method to check the mounting quality of a lens. Fig. 6 A mounted lens and glasses with obvious and large strain distribution. Another version of the experimental configuration which can be utilized to investigate the medium s optical activity and indicate the beam s polarization direction has been constructed based on the optical cage system. As we all known, the glucose solution is a typical optical active medium, which is employed as samples to study the optical activity law by using our experimental system, and the experimental setup and results are shown in Fig. 7. According the demonstration experiment, we can reveal the relationship between optical active degree and optical length of glucose solution clearly, and it is quite convenient for students to understand the optical activity law. On the other hand, the solubility of glucose solution can be obtained by measuring the rotation angle of polarization axis precisely, and the measurement of rotation angle can be done by various digital image processing methods. Fig. 7 A mounted lens and glasses with obvious and large strain distribution. Proc. of SPIE Vol. 10452 1045212-4

3. THREE INTERESTING EXAMPLES ABOUT POLARIZATION Based on the polarization axis finder (PAF), three intuitive and interesting examples about polarization detection and its applications have been introduced and discussed, which are easy to implement and are welcome by teachers and students, and they are very suitable for exciting the students study interest and understanding the physical law of polarization. The first example is the polarized dark glass. The polarized dark glass can be regarded as a polarizer, and thus whether the dark glass is real polarized or not can be checked by the PAF. Based on the example, the Brewster s law and the polarization state of reflection light can be instructed easily, and some thinking questions can be proposed for further discussion, such as the polarized dark glass s axis should be set in horizontal direction or in vertical direction, why the polarized dark glass can make the user feel comfortable and which conditions is quite necessary to wear the polarized dark glass. Fig. 8 is the checking result of the polarized dark glass with PAF. Fig. 8 The checking results of the polarized dark glass with PAF. The second example is the liquid crystal display (LCD). Some students may not know the emitting light of LCD is linearly polarized light, but the truth can be examined by PAF conveniently. This example can not only help students understand the structure and working principle of LCD, but also make them confirm the LCD s polarization properties. Fig. 9(a) and (b) are the observed results of two different LCDs with PAF. (a) (b) Fig. 9 The observed results of two different LCD displays with PAF. The third example is the sky polarization mode. The natural light of sky shows partial degree of polarization due to the Rayleigh scattering, especially in a sunny day, which can also be observed by the PAF, and the experimental results is shown in Fig.10. According to the observed results, we can clearly find that the sky scatting light owns regular law in polarization direction, and investigating the sky polarizing law helps engender some important application fields, such as the polarized skylight navigation [4-5]. Proc. of SPIE Vol. 10452 1045212-5

Fig. 10 The sky polarization mode observed by PAF. 4. CONCLUSION The classroom demonstration experiment is not only an effective way to grasp students attention and excite their study interest, but also a good method to help students understand the difficult and key knowledge points correctly. Some polarization related classroom teaching demonstration experimental systems have been constructed based on a unique and useful tool PAF which can provide instant indication of the laser beam s polarization axis. Two different types of polarization axis visualization systems have been made to observe the polarization direction of a light beam. The optical activity of glucose solution has been studied based on the demonstration experimental system, and the strain distribution of some mounted and unmounted lenses have also been demonstrated and observed in experiment. Finally, three intuitive and interesting examples, LCD, polarized dark glass and skylight, have been observed and discussed based on PAF, which is quite suitable to help students understand these targets polarization properties and the related physical laws. Acknowledgments This work is supported by the education and teaching research undergraduate project of National University of Defense Technology (Grant No. U2016007) and the education and teaching reform research project of College of Optoelectronic Science and Engineering, National University of Defense Technology (Grant No. 2015XY03). REFERENCES [1] Q. D. Yuan, C. Y. Li, A portable demonstrator of polarized light in class, Journal of Hangzhou Normal University (Natural Science Edition) 14(4), 446-448 (2015). [2] http://www.tsi.com/products/_product-accessories/polarization-axis-finder-10901a.aspx. [3] Y. Huang, H. A. Ye, L. X. Gao, M. Zhang, S. G. Liu, New method of generating vectorial polarized beams, Chinese Journal of Lasers 39(4), 17-20 (2012). [4] W. J. Zhang, Y. Cao, X. Z. Zhang, Z. J. Liu, Sky light polarization detection with linear polarizer triplet in light field camera inspired by insect vision, Applied Optics, 54(30), 8962-8970(2015). [5] Y. J. Wang, X. P. Hu, J. X. Lian, L. L. Zhang, X. F. He, Mechanisms of bionic positioning and orientation based on polarization vision and corresponding experiments, Optics and Precision Engineering, 24(9), 2109-2116(2016). Proc. of SPIE Vol. 10452 1045212-6