Phy5645/AngularMomentumProblem: Difference between revisions
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:Now we will calculate the uncertainties <math>\Delta L_x</math> and <math>\Delta L_y</math> and the product <math>\Delta L_x \Delta L_y</math> | :Now we will calculate the uncertainties <math>\Delta L_x</math> and <math>\Delta L_y</math> and the product <math>\Delta L_x \Delta L_y</math> | ||
:After measuring <math>l_z=-\hbar</math> the system will be in the eigenstate <math>|lm>=|1,-1></math>, that is <math>\psi(\theta,\phi)=Y_1,_-1(\theta,|phi)</math>. We will first calculate the expectation values of <math>L_x, L_y, L^2_x, L^2_y</math> using <math>|1,-1></math>. Symmetry requires <math><1,-1|L_x|1,-1>=<1,-1|L_y|1,-1>=0</math>. Using the relation <math>l-1</math> and <math>m=-1</math>; | :After measuring <math>l_z=-\hbar</math> the system will be in the eigenstate <math>|lm>=|1,-1></math>, that is <math>\psi(\theta,\phi)=Y_1,_-1(\theta,|\phi)</math>. We will first calculate the expectation values of <math>L_x, L_y, L^2_x, L^2_y</math> using <math>|1,-1></math>. Symmetry requires <math><1,-1|L_x|1,-1>=<1,-1|L_y|1,-1>=0</math>. Using the relation <math>l-1</math> and <math>m=-1</math>; | ||
:<math><L^2_x>=<L^2_y>=1/2[<L^2>-<L^2_z>]=\hbar^2/2[l(l+1)-m^2]=\hbar^2/2</math> | :<math><L^2_x>=<L^2_y>=1/2[<L^2>-<L^2_z>]=\hbar^2/2[l(l+1)-m^2]=\hbar^2/2</math> |
Revision as of 13:16, 2 December 2009
Posted by Group 6:
- A system is initally in the state:
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi(\theta,\phi)=1/\sqrt{5}Y_1,-_1(\theta,\phi)+\sqrt{3/5}Y_1,_0(\theta,\phi)+1/\sqrt{5}Y_1,_1(\theta,\phi)}
- Let us now find the value of the opperator acting on the system as well as the probability of finding each value.
- We may first rewright the notation for the system as follows;
- acting on the system produces three values for ;
- The probablity for finding the value is;
- This can easially be verified since;
- and
- The probablites of measuring are give as follows;
- Now we will calculate the uncertainties and and the product
- After measuring Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle l_z=-\hbar} the system will be in the eigenstate , that is Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \psi(\theta,\phi)=Y_1,_-1(\theta,|\phi)} . We will first calculate the expectation values of using Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle |1,-1>} . Symmetry requires Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle <1,-1|L_x|1,-1>=<1,-1|L_y|1,-1>=0} . Using the relation and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle m=-1} ;
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle <L^2_x>=<L^2_y>=1/2[<L^2>-<L^2_z>]=\hbar^2/2[l(l+1)-m^2]=\hbar^2/2}
- Therefore;
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Delta L_x \Delta L_y=\sqrt{<L^2_x><L^2_y>}=\hbar^2/2}