Can anyone help? in quantum mechanics commutator prove [L^x,L^y] = ihL^z

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Homework Help Overview

The discussion revolves around proving the commutation relation [L^x, L^y] = ihL^z in the context of quantum mechanics, specifically focusing on angular momentum operators.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster expresses difficulty in rearranging terms to prove the relation and seeks assistance in understanding the mathematical breakdown. Some participants suggest using the form of the commutation relation and applying known commutation rules. Others mention a geometric proof from a textbook as a reference point.

Discussion Status

Participants are actively discussing various approaches to tackle the proof, with some providing specific mathematical manipulations and suggesting the use of commutation relations. There is an exchange of ideas on how to apply these relations to simplify the problem, indicating a collaborative effort to understand the proof without reaching a consensus on a single method.

Contextual Notes

Some participants note confusion regarding the mathematical steps required to manipulate the operators correctly, highlighting potential gaps in foundational knowledge or assumptions about the operators involved.

foranlogan2
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can anyone help?? in quantum mechanics commutator prove [L^x,L^y] = ihL^z

given

:L^x =(y^(pz)^-z^(py)^)
:L^y =(z^(px)^-x^(pz)^)
:L^z =(x^(py)^-y^(px)^) where ^ is just showing its operator


prove comutator [L^x,L^y] = ihL^z

I am swamped at every hurdle and can't seem to get my head around this question to find the answe of ihL^z . any help would be very much appreciated
 
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You're aware of the form of the commutation relation, correct?

[\hat{L}_x,\hat{L}_y]\psi = \hat{L}_x (\hat{L}_y\psi) - \hat{L}_y (\hat{L}_x\psi)

Solve this for the angular momentum operators \hat{L}_x and \hat{L}_y - which you know. The result should cancel down to the form of the angular momentum operator \hat{L}_z.
 
I like the nice, geometric proof of the commutation relations for angular momentum that Sakurai, for example, gives in his delightful book. Unfortunately not mathematically rigorous, but very well looking.
 
yeah I am aware commutator rules but i just can't prove the relation ,i am confused about how to rearange and put in that form. i.e my maths might not be up to scratch but if u can help me with this little proof i might be able to crack the rest... here it goes ...
z(py)x(pz) - x(pz)z(py) ,how do i break this down mathematically without breaking any rules to get ih{x(py)} if [z,pz] = ih..
 
foranlogan2 said:
yeah I am aware commutator rules but i just can't prove the relation ,i am confused about how to rearange and put in that form. i.e my maths might not be up to scratch but if u can help me with this little proof i might be able to crack the rest... here it goes ...
z(py)x(pz) - x(pz)z(py) ,how do i break this down mathematically without breaking any rules to get ih{x(py)} if [z,pz] = ih..

Write

[ L_x, L_y] = [Y P_z - Z P_y, Z P_x - X P_z ]

and then use the fact that the commutator of sums is equal to the sum of commutators

= [Y P_z, Z P_x] - [Z P_y, Z P_x] - [Y P_z , X P_z] + [ Z P_y , X P_z]

Now do each of those commutators.

(My favorite trick is to use directly [AB,CD] = A[B,C]D + B[A,D]C + AC[B,D] +[A,C] DB which can be proven by simply expanding or starting from the simpler and obvious [AB,C] = A[B,C] + [A,C] B )

Patrick
 
Lx=yPz-zPy
Ly=zPx-XPz
Pk=ih d/dk use these relations, careful derivatives and then eliminate.
and result is [Lx,Ly]=ihLz .
 
thanks patrick , do i use [AB,CD] relation for each 4 commutators?,like [YPz,ZPx] and also [ZPy,ZPx] etc
 
foranlogan2 said:
thanks patrick , do i use [AB,CD] relation for each 4 commutators?,like [YPz,ZPx] and also [ZPy,ZPx] etc

Yes. And you use [X_i, X_j]= [P_i,P_j] =0 and [X_i,P_j] = i \hbar \delta_{ij}. you'll see, you will get i \hbar L_z.

You are welcome

Patrick
 

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