E = 6 ⋅ 1 0 3 E=6\cdot10^3 E = 6 ⋅ 1 0 3 e V eV e V
λ = h 2 m E \lambda=\frac{h}{\sqrt{2mE}} λ = 2 m E h
For electron
λ e = h 2 m E = 6.62 ⋅ 1 0 − 34 2 ⋅ 9.1 ⋅ 1 0 − 31 ⋅ 1.6 ⋅ 1 0 − 19 ⋅ 6000 = 1.58 ⋅ 1 0 − 11 m = 15.8 \lambda_e=\frac{h}{\sqrt{2mE}}=\frac{6.62\cdot10^{-34}}{\sqrt{2\cdot 9.1\cdot10^{-31}\cdot 1.6\cdot10^{-19}\cdot 6000}}=1.58\cdot10^{-11} m=15.8 λ e = 2 m E h = 2 ⋅ 9.1 ⋅ 1 0 − 31 ⋅ 1.6 ⋅ 1 0 − 19 ⋅ 6000 6.62 ⋅ 1 0 − 34 = 1.58 ⋅ 1 0 − 11 m = 15.8 p m pm p m
For proton
λ p = h 2 m E = 6.62 ⋅ 1 0 − 34 2 ⋅ 1.67 ⋅ 1 0 − 27 ⋅ 1.6 ⋅ 1 0 − 19 ⋅ 6000 = 1.17 ⋅ 1 0 − 12 m = 1.17 \lambda_p=\frac{h}{\sqrt{2mE}}=\frac{6.62\cdot10^{-34}}{\sqrt{2\cdot 1.67\cdot10^{-27}\cdot 1.6\cdot10^{-19}\cdot 6000}}=1.17\cdot10^{-12} m=1.17 λ p = 2 m E h = 2 ⋅ 1.67 ⋅ 1 0 − 27 ⋅ 1.6 ⋅ 1 0 − 19 ⋅ 6000 6.62 ⋅ 1 0 − 34 = 1.17 ⋅ 1 0 − 12 m = 1.17 p m pm p m
I would use electrons to probe atomic structures.
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