Phy5645/Double pinhole experiment: Difference between revisions
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[[Image:Double_pinhole_1.JPG]] | [[Image:Double_pinhole_1.JPG]] | ||
Suppose you send in an electron along the z axis on a screen at <math>z = 0</math> with two pinholes at <math>x = 0, y = \pm d/2</math>. On a point <math>(x,y)</math> on another screen at <math>z = L>>d, \lambda,</math> the distance from each pinhole is given by <math> r_{\pm}=\sqrt{x^{2}+(y\mp d/2)^{2}+L^{2}}</math>. The spherical wave from each pinhole is added on the screen and hence the | Suppose you send in an electron along the z axis on a screen at <math>z = 0</math> with two pinholes at <math>x = 0, y = \pm d/2</math>. On a point <math>(x,y)</math> on another screen at <math>z = L>>d, \lambda,</math> the distance from each pinhole is given by <math> r_{\pm}=\sqrt{x^{2}+(y\mp d/2)^{2}+L^{2}}</math>. The spherical wave from each pinhole is added on the screen and hence the wave function is | ||
:<math>\psi(x,y)=\frac{e^{ikr_{+}}}{r_{+}}+\frac{e^{ikr_{-}}}{r_{-}}</math>, | :<math>\psi(x,y)=\frac{e^{ikr_{+}}}{r_{+}}+\frac{e^{ikr_{-}}}{r_{-}}</math>, | ||
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where <math> r=\sqrt{x^{2}+y^{2}+L^{2}}</math>. | where <math> r=\sqrt{x^{2}+y^{2}+L^{2}}</math>. | ||
(b) Make a plot of the intensity <math>|\psi(0,y)|^{2}\!</math> as a function of <math>y\!</math>, by choosing <math>k=1, d =20\!</math>, and <math> L=1000 \!</math> | (b) Make a plot of the intensity <math>|\psi(0,y)|^{2}\!</math> as a function of <math>y\!</math>, by choosing <math>k=1, d =20\!</math>, and <math> L=1000 \!</math>. The intensity <math>|\psi(0,y)|^{2}\!</math> is interpreted as the probability distribution for the electron to be detected on the screen, after repeating the same experiment many many times. | ||
(c) Make a contour plot of the intensity <math>|\psi(x,y)|^{2}\!</math> as afunction of x and y, for the same parameters. | |||
(d) If you place a counter at both pinholes to see if the electron has passed one of them, all of a sudden the wave function "collapses". If the electron is observed to pass through the pinhole at <math>y=+d/2\!</math>, the wave function becomes | |||
:<math>\psi_{+}(x,y)=\frac{e^{ikr_{+}}}{r_{+}}</math>. | |||
If it is observed to pass through that at <math>y=-d/2\!</math>, the wave function becomes | |||
:<math>\psi_{-}(x,y)=\frac{e^{ikr_{-}}}{r_{-}}</math>. | |||
After repeating this experiment many times with 50:50 probability for each the pinholes, the probability on the screen will be given by | |||
:<math>|\psi_{+}(x,y)|^{2}+|\psi_{-}(x,y)|^{2}</math> |
Revision as of 22:08, 5 December 2009
Submitted by team 1
Question: Double Pinhole Experiment
Besides Stern-Gerlach experiment, double slit experiment is another one that demonstrates how different quantum mechanics is from the classic counterpart. To avoid mathematical complications with Bessel function, we discuss two pinholes rather than slits.
Suppose you send in an electron along the z axis on a screen at with two pinholes at . On a point on another screen at the distance from each pinhole is given by . The spherical wave from each pinhole is added on the screen and hence the wave function is
- ,
where . Answer the following questions.
(a) Considering just the exponential factors, show that the constructive interference appears approximately at
where .
(b) Make a plot of the intensity as a function of , by choosing , and . The intensity is interpreted as the probability distribution for the electron to be detected on the screen, after repeating the same experiment many many times.
(c) Make a contour plot of the intensity as afunction of x and y, for the same parameters.
(d) If you place a counter at both pinholes to see if the electron has passed one of them, all of a sudden the wave function "collapses". If the electron is observed to pass through the pinhole at , the wave function becomes
- .
If it is observed to pass through that at , the wave function becomes
- .
After repeating this experiment many times with 50:50 probability for each the pinholes, the probability on the screen will be given by