y=exy = e^{-x}

Graph of the Exponential Decay y=exy = e^{-x}

y=exy = e^{-x} is a decaying exponential with base e2.718e \approx 2.718, and can be written ex=1ex=(1e)xe^{-x} = \dfrac{1}{e^x} = \left(\dfrac{1}{e}\right)^x. Its domain is all real numbers and its range is y>0y > 0; the value is never zero or negative.

The derivative y=exy' = -e^{-x} is always negative, so the function is monotonically decreasing everywhere. Each time xx increases by 11, the value is multiplied by 1e\dfrac{1}{e} (about 0.3680.368).

As x+x \to +\infty it approaches 00, so the xx-axis (y=0y = 0) is a horizontal asymptote; as xx \to -\infty it diverges to ++\infty. It always passes through (0,1)(0, 1). The second derivative y=ex>0y'' = e^{-x} > 0, so the graph is always convex (concave up).

Concretely, y=1y = 1 at x=0x = 0, y=1e0.368y = \dfrac{1}{e} \approx 0.368 at x=1x = 1, y=1e20.135y = \dfrac{1}{e^2} \approx 0.135 at x=2x = 2, and y=e2.718y = e \approx 2.718 at x=1x = -1.

It is the mirror image of y=exy = e^x across the yy-axis: where exe^x grows explosively, exe^{-x} decays just as fast. It is closely tied to lnx\ln x as well: setting ex=te^{-x} = t gives x=lntx = -\ln t.

Decaying exponentials appear throughout nature. Radioactive decay, Newton's law of cooling, the discharge of a capacitor, and the elimination of a drug from the body — any process that decreases in proportion to the amount currently present takes the form ekxe^{-kx}. It also underlies the exponential distribution in probability.