How do I evaluate [x, SinPx] commutator

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Homework Help Overview

The discussion revolves around evaluating the commutator [x, SinPx], given the known commutation relation [x, Px] = ih. The subject area pertains to quantum mechanics and operator algebra, particularly focusing on position and momentum operators.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore different methods to evaluate the commutator, including using Taylor series expansions for the sine function and considering the implications of position and momentum operators in different spaces. Some participants question the validity of certain approaches and suggest alternative methods.

Discussion Status

The discussion is active, with various participants sharing their attempts and reasoning. Some guidance has been offered regarding the use of Taylor series, and there are multiple interpretations of the problem being explored. However, there is no explicit consensus on the final evaluation of the commutator.

Contextual Notes

There are indications of typos and potential misunderstandings in the mathematical expressions used, which participants are addressing. The original poster's approach and subsequent responses reflect a mix of confidence and uncertainty regarding the methods employed.

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Homework Statement



Evaluate [x, SinPx] given [x, Px]=ih

Homework Equations



Px = h/I( d/dx)

The Attempt at a Solution


Let f (x) be a function of x.[ x, Sin Px ] f( x) ⇒ [ x sin{( h / i )d / dx} f ( x ) -Sin { (h/i) d / dx } x f(x)] . Does anybody concur .
 
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What you wrote is correct, but it does not answer the problem.
 
What is the answer?
 
sudipmaity said:
What is the answer?
I won't tell you that directly. You should start by looking at the Taylor series for the sine function.
 
after a strenous ordeal Of 48 hr and heated debate with my pals and two sleepless nights, here is what I have come up with.we know in position space momentum oprtr is given -ih d/dx.what would be the opposite.what if I had acess to a position operator in momentum space.lets say x = ih d/dPx.then what happens.
This is what happens :[x , sinPx]f (Px)= [ ih (d / dPx) , sin Px ]f (Px) = ih [ d /dx ( fSin Px )-sin Px d/dx( f )] =
ih [ cos Px f(Px) + sinPx f' (Px)-sin Pxf' (Px) ] = ih cos Px f(Px) . Thrfr [ x, sin Px ] = ih Cos Px
does Anybody agree ??
 
Last edited:
sudipmaity said:
after a strenous ordeal Of 48 hr and heated debate with my pals and two sleepless nights, here is what I have come up with.we know in position space momentum oprtr is given -ih d/dx.what would be the opposite.what if I had acess to a position operator in momentum space.lets say x = ih d/dPx.then what happens.
This is what happens :[x , sinPx]f (x)= [ ih (d / dPx) , sin Px ]f (x) = ih [ d /dx ( fSin Px )-sin Px d/dx( f )] =
ih [ cos Px f(x) + sinPx f' (x)-sin Pxf' (x) ] = ih cos Px f(x) . Thrfr [ x, sin Px ] = ih Cos Px
does Anybody agree ??
There are a few typos along the way (##d/dx## instead of ##d/dP_x##), but it seems ok. You should also try using the Taylor series for the sine. You should find that
$$
\sin \left(\frac{\hbar}{i} \frac{d}{dx} \right) x = x \sin \left(\frac{\hbar}{i} \frac{d}{dx} \right) + \frac{\hbar}{i} \cos \left(\frac{\hbar}{i} \frac{d}{dx} \right)
$$
which leads you to the same answer.
 
I know.I did it that way earlier infact. But this method is more compact and satisfying as it doesn't involves any approximation.You can google out POSITION OPERATOR IN MOMENTUM SPACE.there are very good articles out there upon this.as i am a beginner today I am very happy when I came to know about this concept.
 
sudipmaity said:
I know.I did it that way earlier infact. But this method is more compact and satisfying as it doesn't involves any approximation.
The method I used is not approximate. You never truncate the Taylor series, you let it go to infinity, although you do not need to calculate all the terms, as the pattern is easily identifiable. It is more general, as the momentum space approach only worked because the differential operator wasn't in a function anymore. What if you had to calculate ##[ \cos(x), \sin(P_x)]##? You will also encounter things such as the exponential of operators, and the only correct way to express them is through their Taylor series.
 
Thanks for the insight.
 
  • #10
You first need to prove [x , pn] = niħpn-1.
In order to do that take arbitrary values of n=1, 2, 3 and check.
You'll see for n=1 [x , p] = iħ result holds (as it is given and also we know)
for n=2 [x , p] = p[x , p] +[x , p]p = piħ +ipħ = 2ipħ = 2iħp2-1 again result holds
Similarly you can show for n=3 with the help of first two.
Now, assume for n=k this will hold i.e. [x , pk] = kiħpk-1
then show for n=k+1 and you will find [x , pk+1] = [x , pk]p + pk[x , p] = kihpk-1p + pkih
= kiħpk + kiħpk = (k+1)iħpk = (k+1)iħp(k+1)-1 again holds.
So, [x , pn] = niħpn-1 (PROVED)
Now, to evaluate [x , sin(p)], first expand sin(p) in taylor series.
You'll get sin(p) = p - (p3)/3! + (p5)/5! - ...
Put this in [x , sin(p)]
You'll get [x , sin(p)] = [x , p - (p3)/3! + (p5)/5! - ...]
= [x , p] - (1/3!)[x , p3] + (1/5!)[x , p5] - ...
= iħ - (1/3!)3iħp2 + (1/5!)5iħp4 - ...
= iħ [1 - p2/2! + p4/4! - ...]
= iħ cos(p)
∴ [x , sin(p)] = iħ cos(p)
And this is how you may do it.
 
  • #11
dipanshum said:
You first need to prove [x , pn] = niħpn-1.
In order to do that take arbitrary values of n=1, 2, 3 and check.
You'll see for n=1 [x , p] = iħ result holds (as it is given and also we know)
for n=2 [x , p] = p[x , p] +[x , p]p = piħ +ipħ = 2ipħ = 2iħp2-1 again result holds
Similarly you can show for n=3 with the help of first two.
Now, assume for n=k this will hold i.e. [x , pk] = kiħpk-1
then show for n=k+1 and you will find [x , pk+1] = [x , pk]p + pk[x , p] = kihpk-1p + pkih
= kiħpk + kiħpk = (k+1)iħpk = (k+1)iħp(k+1)-1 again holds.
So, [x , pn] = niħpn-1 (PROVED)
Now, to evaluate [x , sin(p)], first expand sin(p) in taylor series.
You'll get sin(p) = p - (p3)/3! + (p5)/5! - ...
Put this in [x , sin(p)]
You'll get [x , sin(p)] = [x , p - (p3)/3! + (p5)/5! - ...]
= [x , p] - (1/3!)[x , p3] + (1/5!)[x , p5] - ...
= iħ - (1/3!)3iħp2 + (1/5!)5iħp4 - ...
= iħ [1 - p2/2! + p4/4! - ...]
= iħ cos(p)
∴ [x , sin(p)] = iħ cos(p)
And this is how you may do it.

Note that the previous posts are 6 years old.
 

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