The differential equation \((1 + y^2) + (x - 2e^{\tan^{-1}y}) \frac{dy}{dx} = 0\) is rewritten as \(\frac{dy}{dx} = -\frac{1+y^2}{x-2e^{\tan^{-1}y}}\).
Given \(x = f(y)\), the equation can be expressed in terms of \(y\). Substituting \(\frac{dx}{dy} = -\frac{x-2e^{\tan^{-1}y}}{1+y^2}\) and simplifying yields:
\[\frac{dx}{dy} + \frac{x}{1+y^2} = \frac{2e^{\tan^{-1}y}}{1+y^2}.\]
This is a linear first-order differential equation in the form \(\frac{dx}{dy} + P(y)x = Q(y)\), with \(P(y) = \frac{1}{1+y^2}\) and \(Q(y) = \frac{2e^{\tan^{-1}y}}{1+y^2}\).
The integrating factor \(I(y)\) is calculated as:
\[I(y) = e^{\int P(y) \, dy} = e^{\int \frac{1}{1+y^2} \, dy} = e^{\tan^{-1}y}.\]
Multiplying the equation by \(I(y)\) results in:
\[e^{\tan^{-1}y}\frac{dx}{dy} + \frac{e^{\tan^{-1}y}x}{1+y^2} = \frac{2e^{2\tan^{-1}y}}{1+y^2}.\]
The left side is the derivative of \(xe^{\tan^{-1}y}\). Integrating both sides gives:
\[\frac{d}{dy}\left(xe^{\tan^{-1}y}\right) = \frac{2e^{2\tan^{-1}y}}{1+y^2}.\]
The integral of the right side is:
\[xe^{\tan^{-1}y} = \int \frac{2e^{2\tan^{-1}y}}{1+y^2} \, dy = e^{2\tan^{-1}y} + C.\]
The general solution is therefore:
\[x = e^{\tan^{-1}y} + Ce^{-\tan^{-1}y}.\]
Using the initial condition \(f(0) = 1\), we get \(1 = e^0 + Ce^0\), which implies \(C = 0\).
The specific solution is \(x = e^{\tan^{-1}y}\).
Evaluating \(f\left(\frac{1}{\sqrt{3}}\right)\) yields:
\[f\left(\frac{1}{\sqrt{3}}\right) = e^{\tan^{-1}\left(\frac{1}{\sqrt{3}}\right)}.\]
Since \(\tan^{-1}\left(\frac{1}{\sqrt{3}}\right) = \frac{\pi}{6}\), the final result is:
\[f\left(\frac{1}{\sqrt{3}}\right) = e^{\frac{\pi}{6}}.\]