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1 About the instructor: Pengqian Wang, Associate Professor, Department of Physics, Western Illinois University Phone: 309-298-2541

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Presentation on theme: "1 About the instructor: Pengqian Wang, Associate Professor, Department of Physics, Western Illinois University Phone: 309-298-2541"— Presentation transcript:

1 1 About the instructor: Pengqian Wang, Associate Professor, Department of Physics, Western Illinois University Phone: 309-298-2541 E-mail: p-wang@wiu.edup-wang@wiu.edu http://faculty.wiu.edu/P-Wang Mathematics Science Partnership (MSP) 2011 Polarization of Light (Color online if you have a black and white printout) Pengqian Wang Contents: 1. Electromagnetic Waves 2. Polarization of Light 3. Polarizers 4. Polarization by Reflection 5. Birefringence 6. Optical Activity

2 2 1. Electromagnetic Waves Lights are electromagnetic waves. A light has an oscillating electric field and an oscillating magnetic field. The directions of the electric field (E), the magnetic field (B), and the propagation of the light (v) are perpendicular to each other. They are related by the right hand rule: E×B//v. Waves are categorized into transverse waves and longitudinal waves. Light is a transverse wave, because its oscillation directions (E and B) are perpendicular to its propagation direction (v). Assignment 1.

3 3 2. Polarization of Light 2.1 Definition of the polarization direction of light The polarization direction of light is defined as in the direction of its electric field. 1)Since F e = qE, the polarization determines the force direction. Most light phenomena are governed by the fact that the electrons in the molecules receive forces from the electric field of the light waves. 2)An electron usually receives a much stronger force from the electric field than from the magnetic field of the light. F e = qE, F m = qv×B. 2.2 Polarization states of light Suppose the light is propagating in the z-direction. Because light is a transverse wave, the electric field (E-field) direction, which has been defined as the polarization of the light, must be in the x-y plane. Its two components on the x and y axes are algebraically x y ExEx EyEy

4 4 x y ExEx EyEy E  = 0 x y ExEx EyEy E  = ±  1) Linear polarization The E-field is always oscillating in one direction. This corresponds to  phase lag  = 0 or  = ±  in the algebraic description. 2) Circular polarization The direction of the E-field rotates. The end point of the E vector traces out a circle. This corresponds to  E 0x =E 0y =E 0,  = ±  /2 in the algebraic description. x E0E0 E0E0 E  t y  = -  /2 x E0E0 E0E0 E tt y  =  /2

5 5 3) Elliptical polarization The E vector rotates and changes its magnitude as well. The end point of the E vector traces out an ellipse. Elliptical polarization is the most general form of the polarization state of light. E0xE0x E0yE0y E 4) Random polarization The direction of the E-field is not predictable. Also called unpolarized light. Nature light (sun light) is randomly polarized.

6 6 3. Polarizers A polarizer is an optical device whose output is a certain form of polarized light. A linear polarizer is the most common type of polarizer. It has a transmission axis and an extinction axis, which are perpendicular to each other. Light polarized in the direction of the transmission axis passes through the polarizer freely. Light polarized in the direction of the extinction axis is totally absorbed or deflected. Therefore the transmitted light is polarized in the direction of the transmission axis of the polarizer. Malus’s law The energy transmitivity of a linear polarizer is given by the Malus’s law. Suppose a linearly polarized light with intensity I 0 is impinging upon a linear polarizer, the intensity of the transmitted light is given by Here  is the angle between the polarization direction of the input light and the transmission axis of the polarizer. Assignment 2. For randomly polarized light, the transmission through a linear polarizer is always ½.  Input polarization Output polarization Transmission axis Light propagation direction Polarizer

7 7 Activities: 1. Preparing the polarizer. Tear off the protection film. Mark the two shorter sides with transparent tape. They are the transmission axes. Cut the polarizer into halves. You now have two linear polarizers. 2. Observation of light sources. 1)Ceiling lights. Please hold a polarizer and look through it at a ceiling light. Rotate the polarizer through 360º. What happens to the intensity of the transmitted light? What is the polarization state of the light emitted by the ceiling lights? 2)Two polarizers. Please hold one polarizer in each hand, one in front of the other, and look through them at a ceiling light. Now rotate one of the polarizers through 360º. What happens to the intensity of the light transmitted through the two polarizers? What is the angular relationship between the transmission axes of the two polarizers when the light is blocked? 3)Laser pointer. Please observe laser safety. 4)Flashlight. 5)LCD screens. E.g., a computer monitor, a cell phone, a camera, a calculator, etc. Assignment 3.

8 8 4. Polarization by Reflection 4.1 s-polarization and p-polarization Plane-of-incidence is the plane formed by the incident light beam and the normal of the interface between the two media. The s-polarization is defined for those light whose E-field is perpendicular to the plane- of-incidence. The p-polarization is defined for those light whose E-field is parallel to the plane-of-incidence. EiEi ii rr tt nini ErEr EtEt ntnt s-polarization EiEi ii rr tt nini ErEr EtEt ntnt p-polarization

9 9 4.2 Reflectance The energy reflectance of a light beam incident on an optical medium depends on the polarization of the incident light, i.e., whether it is s-polarized or p-polarized.

10 10 s E R p = 0 Brewster angle BB p Polarizer When is called the Brewster angle. At the Brewster angle, the reflectance of the p-polarization is zero, therefore the reflected nature light is totally s-polarized, i.e., it is linearly polarized in the direction perpendicular to the plane-of-incidence. We can then reduce the reflected light using a polarizer. This is how a sunglass work. It is especially helpful when you are fishing. For a glass with n=1.5, the Brewster angle is Assignment 4. 4.3 Brewster angle

11 11 Activities: Glare from the floor: Please find a place on the floor in the classroom or hallway where you can see “glare” (reflection) from a ceiling light (carpet won’t work). You may need to turn off other lights. Look at the glare through a single polarizer and rotate the polarizer through 360º. At the minimum transmission, please further reduce the transmitted light by adjusting the angle of reflection. This is done by moving yourself a little forward or backward. What is the orientation of the transmission axis of the polarizer when the glare is minimized? What is the polarization direction of the light being reflected from the floor?

12 12 5. Birefringence 5.1 Birefringence Birefringence refers to the phenomenon that when light is propagating inside an optically anisotropic crystal, mostly a uniaxial crystal, the refractive index of the light depends on its polarization direction. The crystal has an optic axis. Light whose polarization is perpendicular to the optic axis feels a refractive index of n o and propagates with a speed of v o =c/ n o. Light whose polarization is parallel to the optic axis feels a refractive index of n e and propagates with a speed of v e =c/ n e. Inside the crystal, a light beam is in general split into an ordinary light and an extraordinary light, each with different speed and somehow different propagation direction. An anisotropic crystal can be used to separate light into two perpendicularly polarized light beams. Extraordinary-light Ordinary-light Optic axis

13 13 5.2 Wave plates Wave plates (retardation plates, or retarders) are optical elements used to transform the polarization states of light. They are made from one or more pieces of birefringent crystals. Each wave plate has a fast axis and a slow axis. Inside the crystal, the incident light is separated into two lights, each has refractive indices n o and n e, and is polarized parallel to the fast or slow axes. The two light have different speed, therefore at the output surface there is a phase lag between the two lights. The phase lag determines the polarization state of the output light. 1) A half-wave plate introduces a phase lag of . It converts a linearly polarized light into another linearly polarized light, mirrored by the fast or slow axis. 2) A quarter-wave plate introduces a phase lag of  /2. It converts a linearly polarized light into a circularly polarized light, when the input polarization is 45° to the fast and slow axes. Assignment 5. f s s f Half-wave plate s f Quarter-wave plate s f

14 14 Activities: 1. Calcite crystal 1)Please put the crystal on a page of paper and see the transmission of some letters without polarizers. Rotate the crystals a little so that the two images of the letters are well separated. Then look at the letters with one polarizer. Rotate the polarizer and explain what you observe. Please notice the relation between the polarization directions of the two images of the letters. Assignment 6. 2)Please put the crystal on a picture of a bird, and see the transmission of the picture when you are rotating the polarizer back and forth. I hope you have fun. 2. Crossed polarizers. Please fix the flashlight on your table with light shooting up, using a double-sided tape. Adjust the two polarizers until they are exactly crossed and the light coming from the flashlight is extinguished. Place each of the following objects between the polarizers and rotate them. You will see that light is transmitted in very interesting ways. 1) A plastic protractor. 2) A U-shape plastic ― squeeze it and see the stress-induced bands. 3) A small plastic box. 4) Pieces of cellophane tape on glass. 5) A sheet of mica.

15 15 6. Optical Activity 8.10 Optical activity Optical activity refer to the phenomena that when a linearly polarized light is passing through a medium, the polarization plane is rotated. It is thus also called optical rotation. When this happens, the medium is said to be optically active. The rotation of the polarization plane is proportional to the path length of the light, and can be measured by degree/centimeter. Common optically active media include quartz, sugar and syrup. It can be used to measure blood sugar concentration in diabetic people. Activities: Corn syrup Please fill a beaker with corn syrup to about 1.5 inch high. Put the beaker between the crossed polarizers above our flashlight station. Please rotate the upper polarizer in very fine step and observe the color changes of the syrup. Please take photos of your favorite colored liquid when possible.


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