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for de Broglie waves

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* wave numbers nee<strong>de</strong>d to represent a wave group extend from<br />

k=0 to k=∞, but <strong>for</strong> a group which length Δx is finite<br />

<strong>waves</strong> which amplitu<strong>de</strong>s g(k) are appreciable have wave number<br />

that lie within a finite interval Δk<br />

the shorter the group,<br />

the broa<strong>de</strong>r the range of wave numbers nee<strong>de</strong>d.<br />

Figure3.15 A gaussian distribution. The probability of finding a value of x is given by the gaussian<br />

function f(x). The mean value of x is x 0 , and the total width of the curve at half its maximum value is<br />

2.35σ, whereσis the standard <strong>de</strong>viation of the distribution. The total probability of finding a value of x<br />

within a standard <strong>de</strong>viation of x 0 is equal to the sha<strong>de</strong>d area and is 68.3 percent.<br />

*Gaussian function: f(x)=<br />

1<br />

2<br />

x<br />

x <br />

1 o<br />

2<br />

2<br />

e<br />

2<br />

n<br />

2<br />

x i<br />

x o<br />

n i<br />

1<br />

Standard <strong>de</strong>viation (square-root-mean)<br />

Width of a gaussian curve at half its max is 2.35σ<br />

o<br />

<br />

x<br />

p f dx 0 . 683<br />

x <br />

o<br />

x <br />

x <br />

o<br />

• Min ΔxΔk occur <strong>for</strong> Gaussian function<br />

Take Δx,Δk as standard <strong>de</strong>viation ofφ(x)& g(x)<br />

ΔxΔk=1/2∴<br />

in general ΔxΔk 1/2<br />

∵ k=2π/λ = 2πP/h P=hk/2π ΔP =hΔk/2π<br />

19

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