Dye laser and its construction

Dye lasers use liquid organic dyes. These organic dyes are dissolved in solvents like water, ethyl  alcohol, methanol. The most widely used dye is rhodamine-6G, also known as Xanthene dye. These lasers are discovered by Sorokin and his colleagues. Dye lasers operate without the intervening metastable state.


The dye laser consisted of a 1cm long quartz glass tube filled with solutions of organic  dyes such as rhodamine- 6G.
Active Medium. Rhodamine-6G dissolved in a suitable liquid like water, ethyl alcohol or methanol is used as the active medium. The dye solution used in the dye lasers typically has a concentration in the range of 10-2 to 10-4 M. Rhodamine-6G emits in yellow-red region.

Pumping source: Energy to excite the dye is supplied by a strong light source that may be a flash lamp or another laser like N2 laser or argon-ion laser. Thus, optical pumping is used to excite the dye and to achieve population inversion.

Optical resonator System. The most useful feature of dye lasers is their tunability.  The tunability means that the lasing wavelength for a dye may be varied over a wide range.  Due  to this   reason, dye lasers are also called tunable lasers. Tuning over 500 angstrom has been obtained.

One of the teachniques to obtain tuning is to replace one of the mirrors  of the resonant cavity with a diffraction  grating. Thus a dye cell is usually placed inside a cavity consisting of a partially  reflective  mirror  on
the  front and a diffraction grating on the rear. A source light is focused onto the  dye to excite it and stimulate laser action.

By rotating the diffraction grating , wavelength of laser output can be altered. Thus tuning is obtained. Therefore, this combination of partially reflective mirror and diffraction grating will act as optical resonator system. For radiation to be reflected back along the  laser cavity axis, the angle θ that the normal to the diffraction grating makes with the cavity must satisfy the condition.

2dsinθ =nλ  (n = 1, 2, 3, …)

Where  d is grating spacing

Λ is wavelength of radiation.

By rotating the grating, angle θ will be changed and thus the output wavelength will be changed that is tuning of output wavelength will be achieved.

Reference: This article is referred from my authored book “Optics and lasers” having ISBN 978-81-272-3833-9. In case of any doubt in this article or any article of Physics, kindly post in the comment section. Try to make the construction figure. I will explain the working in the next article.

Kindly Read This Also :

Note from winnerscience: If you want the e-notes of all the laser documents that will include the basics of lasers like stimulated absorption, difference between spontaneous and stimulated emission, Einstein  Coefficients, properties and applications of lasers, complete construction and working of lasers like Ruby laser, He-Ne laser, Carbon dioxide laser, Nd:YAG laser, dye laser, semiconductor laser, holography and additional articles of Q-switching and mode locking, then please contact [email protected]. You can post your queries also there.

Leave a Reply

This site uses Akismet to reduce spam. Learn how your comment data is processed.