How to Tune a Helium-Neon Laser's Frequency Over Its Gain Bandwidth?

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Homework Help Overview

The discussion revolves around tuning the frequency of a helium-neon (He-Ne) laser within its gain bandwidth, specifically focusing on the relationship between the laser's resonator length and the wavelength of emitted light. The problem involves understanding the gain bandwidth of the laser and how it relates to the standing wave condition in the resonator.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the relationship between the resonator length and the wavelength of the laser, questioning how to determine the longest and shortest wavelengths within the specified gain bandwidth. There is also discussion about the conversion between wavelength and frequency and how it affects calculations.

Discussion Status

The conversation is ongoing, with participants providing insights and asking clarifying questions. Some guidance has been offered regarding the calculation of wavelengths corresponding to the gain bandwidth, but confusion remains about the correct approach to determine acceptable wavelengths within the bandwidth.

Contextual Notes

Participants are grappling with the implications of a gain bandwidth of 1 GHz around a central wavelength of 632.8 nm, and the conversion between frequency and wavelength is a focal point of the discussion. There is uncertainty regarding the interpretation of bandwidth limits and their impact on wavelength calculations.

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Homework Statement


A helium-neon (He-Ne) laser has a gain bandwidth (denoted here as the frequency interval
over which the laser gain equals or exceeds the minimum threshold gain) given by ΔG= 1.0 GHz, centred on the λ = 632.8 nm emission wavelength.

Show that in order to tune the frequency of this He-Ne laser over its entire gain
bandwidth, the length of the resonator should be changed by ΔL = -1/2λ.

Homework Equations


L=mλ/2


The Attempt at a Solution


The length and frequency changes are both small compared to the length and fre-
quency, respectively so differentiation of the condition for standing waves in a
resonator must be applied.

The condition for standing waves is :L=mλ/2

but dL/dλ= m/2 , how can i get ΔL = -1/2λ ?
 
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helpcometk said:
The condition for standing waves is :L=mλ/2

You want the fundamental mode, so m=1. The calculation is pretty straightforward. Calculate the longest and shortest wavelength still within the gain bandwidth and calculate the corrsponding resonator lengths needed to get a standing wave for these two wavelengths.
 
thanks for the reply but i can't understand what it means:
longest and shortest wavelength still within the gain bandwidth ,how can you see if wavelength is within the bandwidth?
 
helpcometk said:
how can you see if wavelength is within the bandwidth?

The problem statement says you have a bandwidth of 1 GHz around the central wavelength of 632.8 nm, so your bandwidth goes from 632.8nm-0.5 GHz to 632.8nm+0.5 GHz. The conversion between wavelength and frequency is pretty much the only math involved here. You should be able to do that yourself.
 
this doesn't make sense because 0.5 Ghz corresponds to 0.6 m wavelength, so 632.8*10^-9 -0.6 gives negative wavelength which cannot be acceptable
 
Ok...let me start at the very beginning.

Just do me the favour and calculate the wavelengths corresponding to 0nm +0.5 Ghz (as you did), 100nm+0.5 GHz, 632nm+0.5 GHz and 2000 nm+0.5 GHz by converting wavelength to frequency FIRST and then adding the 0.5 GHz.

And while you are at it please just plot a graph of wavelength vs. corresponding frequency and have a look at whether it is linear or not. Does that help you understand why one cannot just convert 0.5 GHz into a wavelength and subtract it, but have to convert the desired wavelength into a frequency before and then add or subtract the bandwidth from that converted value?
 
Last edited:

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