The solution of the differential equation \[ \frac{d^{2} y}{d t^{2}}-y=0 \text {, } \] subject to the boundary conditions \( y(0)=1 \) and \( y(\infty)=0 \), is
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The given differential equation is a second-order linear homogeneous equation. The characteristic equation corresponding to it is \( r^2 - 1 = 0 \), which has solutions \( r = 1 \) and \( r = -1 \). Therefore, the general solution to the differential equation can be expressed as: \[ y(t) = A e^{t} + B e^{-t} \] Now, applying the first boundary condition \( y(0) = 1 \), we have: \[ A e^{0} + B e^{0} = A + B = 1 \] Next, to apply the second boundary condition \( y(\infty) = 0 \), it is important to analyze the behavior of the solution as \( t \) approaches infinity. The term \( A e^{t} \) will go to infinity unless \( A = 0 \). Therefore, we can conclude that \( A \) must be 0. Using \( A = 0 \) in the first condition: \[ 0 + B = 1 \implies B = 1 \] Thus, the solution simplifies to: \[ y(t) = e^{-t} \] This satisfies both boundary conditions \( y(0) = 1 \) and \( y(\infty) = 0 \). Hence, the final solution is: \[ \boxed{y(t) = e^{-t}} \]