Laser Theory: Calculating Power Gain/Loss with Inverted Medium

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The discussion focuses on calculating the power gain or loss of a light wave passing through an inverted medium with specific parameters. The medium has a gain coefficient of 0.1 cm^-1 and a loss coefficient of 0.05 cm^-1, leading to a net gain when the light wave is amplified. The power gain is calculated using the formula P = P0 * e^(g-L)*L, resulting in an approximate gain of 5.13%. This gain indicates that the light wave experiences an increase in power as it traverses the medium, assuming no gain saturation effects. Overall, the analysis highlights the relationship between gain, loss, and the characteristics of the medium in laser theory.
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Hi, I have no clue on how to attempt this problem. I could really use some assistance. Thanks in advance.

The transisition between two energy levels exhibits a Lorentzian lineshape of central frequency Vo=5*10^14 Hz with a linewidth deltaV=10^12 Hz. The population is inverted so that the small-signal gain coefficient has a peak value of 0.1 cm^-1. The medium has an additional loss coefficient alpha1=0.05 cm^-1. The inverted medium is used to amplify an incident light wave that has a uniform power spectral density centered about Vo and with a bandwidth 2deltaV. How much loss or gain in power cm is experienced by the light wave as it passes through the amplifying medium? Ignore gain saturation effects.
 
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The power gain or loss experienced by the light wave as it passes through the amplifying medium is equal to the small-signal gain coefficient multiplied by the additional loss coefficient, alpha1, and the incident power spectral density. In this case, the power gain or loss is equal to 0.1 cm^-1 * 0.05 cm^-1 * 2deltaV = 1 cm^-1.
 



To calculate the power gain or loss in this scenario, we can use the equation for gain/loss in a medium, which is given by P = P0 * e^(g-L)*L, where P0 is the initial power, g is the gain coefficient, L is the length of the medium, and L is the loss coefficient.

In this case, we have an inverted medium with a gain coefficient of 0.1 cm^-1 and a loss coefficient of 0.05 cm^-1. The length of the medium is not given, but we can assume it is long enough for the light wave to pass through completely.

We also know that the incident light wave has a central frequency of 5*10^14 Hz and a bandwidth of 2*10^12 Hz. This means that the power spectral density of the incident light wave is uniform and centered around the central frequency.

Now, we can plug in the values into the equation to calculate the power gain/loss. Since we are ignoring gain saturation effects, we can assume that the initial power (P0) is equal to the power of the incident light wave.

P = P0 * e^(g-L)*L

= P0 * e^(0.1-0.05)*L

= P0 * e^0.05*L

= P0 * 1.0513*L

Since the length of the medium is not given, we cannot calculate the exact power gain/loss. However, we can see that the power will increase by a factor of 1.0513. This means that the light wave will experience a power gain of approximately 5.13%. This makes sense since we have an inverted medium with a gain coefficient that is higher than the loss coefficient.

In conclusion, the light wave will experience a power gain of approximately 5.13% as it passes through the inverted medium. It is important to note that this calculation is only valid if we ignore gain saturation effects. If gain saturation effects are taken into account, the power gain/loss will be different.
 
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