Skip to main content
Book cover

Lasers pp 63–96Cite as

Einstein Coefficients and Light Amplification

  • Chapter
  • First Online:
  • 6328 Accesses

Part of the book series: Graduate Texts in Physics ((GTP))

Abstract

In this chapter we discuss interaction of radiation and atoms and obtain the relationship between absorption and emission processes. We show that for light amplification a state of population inversion should be created in the atomic system. We also obtain an expression for the gain coefficient of the system. This is followed by a discussion of two-level, three-level, and four-level systems using the rate equation approach. Finally a discussion of various mechanisms leading to broadening of spectral lines is discussed.

This is a preview of subscription content, log in via an institution.

Buying options

Chapter
USD   29.95
Price excludes VAT (USA)
  • Available as PDF
  • Read on any device
  • Instant download
  • Own it forever
eBook
USD   79.99
Price excludes VAT (USA)
  • Available as EPUB and PDF
  • Read on any device
  • Instant download
  • Own it forever
Softcover Book
USD   99.99
Price excludes VAT (USA)
  • Compact, lightweight edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info
Hardcover Book
USD   129.99
Price excludes VAT (USA)
  • Durable hardcover edition
  • Dispatched in 3 to 5 business days
  • Free shipping worldwide - see info

Tax calculation will be finalised at checkout

Purchases are for personal use only

Learn about institutional subscriptions

Notes

  1. 1.

    We will show in Section 4.5 that \(g(\omega_0)\Delta \omega \) equals \((2/\pi)\) and \((4\ln 2/\pi)^{1/2}\) for Lorentzian and Gaussian lineshape functions, respectively.

  2. 2.

    Ruby laser active medium consists of Cr+3-doped ion Al2O3 and is an example of a three level laser. More details regarding the ruby laser are given in Section 10.2.

  3. 3.

    We are considering here a single electron atom with r representing the position of the electron with respect to the nucleus. Thus the electric dipole moment of the atom is given by p = e r because the direction of the dipole moment is from negative to the positive charge. The interaction energy of a dipole placed in an electric field \({E}\ {\textrm{is}} \ -\vec{p}.{E} \) is which leads to Eq. (4.62).

  4. 4.

    It may be noted that Eq. (4.80) predicts an indefinite increase in the transition probability with time; however, the first-order perturbation theory itself breaks down when Γ21 is not appreciably less than unity. Thus Eq. (4.80) gives correct results as long as Γ21≪ 1.

  5. 5.

    It can be shown that \(\left|\int\psi_{1}^{\ast}{\textbf{r}}\psi_2{\textrm d}\tau\right|^2\) has the same value for transition from anyone of the states (n = 2, l = 1, m = 0) or (n = 2, l = 1, m = -1) or (n = 2, l = 1, m = -1) to ( n = 2, l = 0, m = 0) state. However, the matrix element for the transition from (n = 2, l = 0, m = 0) state to the (n = 1, l = 0, m = 0) state is zero. This implies that the corresponding dipole transition is forbidden.

References

  • Ghatak, A. K., and Lokanathan, S. (2004), Quantum Mechanics, Macmillan, New Delhi.

    MATH  Google Scholar 

  • Gopal, E. S. R. (1974), Statistical Mechanics and Properties of Matter, Wiley, New York.

    Google Scholar 

  • McFarlane, R. A., Bennet, W. R., and Lamb, W. E. (1963), Single mode tuning dip in the power output of an He–Ne Optical maser, Appl. Phys. Lett. 2, 189.

    Article  ADS  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Corresponding author

Correspondence to K. Thyagarajan .

Rights and permissions

Reprints and permissions

Copyright information

© 2011 Springer Science+Business Media, LLC

About this chapter

Cite this chapter

Thyagarajan, K., Ghatak, A. (2011). Einstein Coefficients and Light Amplification. In: Lasers. Graduate Texts in Physics. Springer, Boston, MA. https://doi.org/10.1007/978-1-4419-6442-7_4

Download citation

Publish with us

Policies and ethics