QUANTUM PHYSICS FUNDAMENTALS - Chapter 7, Exercise 1 Solution ========================================================== Proton Tunneling Through the Same Barrier as an Electron PROBLEM ------- A proton (mass 1.673 x 10^-27 kg) approaches the same barrier as the chapter's worked example - 1 eV (1.602 x 10^-19 J) high, 1 nm wide. Calculate kappa and estimate the transmission probability. Compare it to the electron's own result. SOLUTION -------- Step 1: Calculate kappa. kappa = sqrt(2 m (V0 - E)) / hbar kappa = sqrt(2 x 1.673 x 10^-27 x 1.602 x 10^-19) / 1.0546 x 10^-34 kappa = sqrt(5.360 x 10^-46) / 1.0546 x 10^-34 kappa = 2.315 x 10^-23 / 1.0546 x 10^-34 kappa = 2.196 x 10^11 m^-1 Step 2: Calculate the transmission probability, with L = 1 x 10^-9 m. T = e^(-2 kappa L) T = e^(-2 x 2.196 x 10^11 x 1 x 10^-9) T = e^(-439.2) T = approximately 10^-191 ANSWER: The proton's transmission probability through the identical barrier is approximately 10^-191 - effectively zero, compared to the electron's own real, nonzero result of approximately 3.5 x 10^-5 (roughly a 1-in-30,000 chance). ---- WHY THIS WORKS AS AN ANSWER This is a direct, striking real illustration of the exponential mass dependence in the tunneling formula. The proton is only about 1,836 times more massive than the electron, but because kappa depends on the SQUARE ROOT of mass, and the transmission probability depends exponentially on kappa, that modest mass ratio (sqrt(1836) is only about 43) produces an almost incomprehensibly larger drop in tunneling probability once it's inside an exponential. This is exactly why quantum tunneling is a routinely observed, practically significant effect for electrons (in the scanning tunneling microscope and tunnel diodes covered in this chapter) but is utterly negligible for a proton crossing an identically-sized barrier under ordinary conditions - and it is also why, in the chapter's own real stellar- fusion example, the enormous NUMBER of protons colliding in the Sun's core, not a large individual tunneling probability, is what makes the overall fusion rate real and observable.