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What is the probability that a right-circularly polarized photon will pass through a linear polarizer with its transmission axis along the \(x^{\prime}\) axis, which makes an angle \(\phi\) with the \(x\) axis?

Short Answer

Expert verified
The probability is \( \cos^2(\phi) \).

Step by step solution

01

Understanding the Setup

We have a right-circularly polarized photon and a linear polarizer whose transmission axis is at an angle \( \phi \) relative to the \( x \) axis. We need to determine the probability that the photon will pass through the polarizer.
02

Expression for Probability

The probability that a photon will pass through a polarizer is given by the squared modulus of the cosine of the angle between the photon’s polarization and the polarizer’s transmission axis. For a circularly polarized photon, the angle effectively becomes \( \phi \). Hence, the probability is \( \cos^2(\phi) \).
03

Calculating the Probability

We use the formula derived: \( P = \cos^2(\phi) \). This is computed directly based on the angle \( \phi \).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Photon Polarization
Photon polarization refers to the orientation of the oscillations of a photon's electric field. Photons can be polarized in several ways, with two primary types being linear and circular polarization.

Circular polarization, as in this exercise with a right-circularly polarized photon, means that the electric field of the photon rotates in a circle as the photon moves forward. This kind of polarization can be thought of as having components in two perpendicular directions that are out of phase by 90 degrees.

When photons are linearly polarized, their electric field oscillates in a single plane. The direction of this oscillation is known as the polarization direction or axis. Understanding photon polarization is crucial in many fields, including optical physics and quantum mechanics. It is the basis of technologies and phenomena ranging from liquid crystal displays (LCDs) to quantum cryptography.

Photon polarization plays a key role in determining how light interacts with polarizers and other optical devices, influencing outcomes in experiments and practical applications.
Linear Polarizer
A linear polarizer is an optical filter that allows light waves of a specific polarization to pass through while blocking others. In this exercise, the linear polarizer's transmission axis is set along an arbitrary angle, noted as the \( x' \) axis, which forms an angle \( \phi \) with the standard \( x \)-axis.

Linear polarizers are indispensable in controlling light in various applications. They work by only allowing light waves aligned with their transmission axis to pass, while absorbing or reflecting waves that are perpendicular to it.
  • This selective passage of light based on its polarization is why sunglasses with polarizing lenses can reduce glare, for example.
  • In physics experiments, they serve to analyze the polarization state of photons or beams of light, crucial in understanding wave optics behavior.
For circularly polarized light, the polarizer "sees" an oscillation of electric fields and determines how much of that light can pass through based on its alignment with the transmission axis. This concept was directly applied in calculating the probability in the given exercise.
Optical Physics
Optical physics is a branch of physics focused on the study of light and its interactions, including its propagation, emission, and absorption. It encompasses a vast array of phenomena and technologies.

One key area within optical physics is the study of polarization, which involves understanding how light waves can be described by their orientation and wavefront characteristics. Polarization techniques allow for exploration of various optical devices like polarizers, wave plates, and interferometers which manipulate these properties of light.

Key concepts of optical physics include:
  • Wave-Particle Duality: Light exhibits both wave-like and particle-like properties, fundamental to photon behavior.
  • Interference and Diffraction: When light waves overlap, they can constructively or destructively interfere, leading to patterns that can be measured and used in precision instruments.
The calculation in this exercise rests upon understanding how light polarized in different ways interacts with polarizers, an essential skill in optical physics, and showcases how different types of light can be quantitatively analyzed for various applications.

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Most popular questions from this chapter

A system of \(N\) ideal linear polarizers is arranged in sequence, as shown in Fig. 2.13. The transmission axis of the first polarizer makes an angle of \(\phi / N\) with the \(y\) axis. The transmission axis of every other polarizer makes an angle of \(\phi / N\) with respect to the axis of the preceding one. Thus, the transmission axis of the final polarizer makes an angle \(\phi\) with the \(y\) axis. A beam of \(y\)-polarized photons is incident on the first polarizer. (a) What is the probability that an incident photon is transmitted by the array? (b) Evaluate the probability of transmission in the limit of large \(N\). (c) Consider the special case with the angle \(\phi=90^{\circ}\). Explain why your result is not in conflict with the fact that \(\langle x \mid y\rangle=0 .^{16}\)

The Hermitian operator \(\hat{A}\) corresponding to the observable \(A\) has two eigenstates \(\left|a_{1}\right\rangle\) and \(\left|a_{2}\right\rangle\) with eigenvalues \(a_{1}\) and \(a_{2}\), respectively. Assume \(a_{1} \neq a_{2}\). Show that \(\hat{A}\) can be written in the form $$ \hat{A}=a_{1}\left|a_{1}\right\rangle\left\langle a_{1}\left|+a_{2}\right| a_{2}\right\rangle\left\langle a_{2}\right| $$ and that $$ \langle\psi|\hat{A}| \psi\rangle=\langle A\rangle $$

Use Dirac notation (the properties of kets, bras, and inner products) directly without explicitly using matrix representations to establish that the projection operator \(\hat{P}_{+}\)is Hermitian. Use the fact that \(\hat{P}_{+}^{2}=\hat{P}_{+}\)to establish that the eigenvalues of the projection operator are 1 and 0 .

A beam of linearly polarized light is incident on a quarter-wave plate with its direction of polarization oriented at \(30^{\circ}\) to the optic axis. Subsequently, the beam is absorbed by a black disk. Determine the rate at which angular momentum is transferred to the disk, assuming the beam carries \(N\) photons per second.

Construct projection operators out of bras and kets for \(x\)-polarized and \(y\) polarized photons. Give physical examples of devices that can serve as these projection operators. Use (a) the properties of bras and kets and (b) the properties of the physical devices to show that the projection operators satisfy \(\hat{P}_{x}^{2}=\hat{P}_{x}, \hat{P}_{y}^{2}=\hat{P}_{y}\), and \(\hat{P}_{x} \hat{P}_{y}=\hat{P}_{y} \hat{P}_{x}=0\).

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