Shankar CH1 Derivative of Dirac delta

In summary, The conversation is discussing the delta function and its derivative. The speaker is trying to understand how the second equality in Shankar's Principles of QM can be derived. They suggest that a product rule may be used, but the response explains that the sifting property of the delta function allows for the second term to be simplified.
  • #1
LAHLH
409
1
Hi,

On p67 of shankar Principles of QM, he considers the delta functions derivative. He says:

[tex] \int \delta'(x-x')f(x')dx'= \int \frac{d\delta(x-x')}{dx}f(x')dx'= \frac{d}{dx}\int \delta(x-x') f(x')dx'=\frac{df(x)}{dx} [/tex]

I don't understand how the second equality follows, how can the derivative just be pulled out like that here? I'm not sure if differentiating under the integral vs externally changes things from what I may have expected. But I thought some kind of product rule of the form:

[tex] \frac{d}{dx}\int \delta(x-x') f(x')dx'=\int \left[ \frac{d\delta(x-x')}{dx} f(x')+\frac{d f(x')}{dx} \delta(x-x') \right] dx' [/tex]

would be in operation.
 
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  • #2
[tex]\frac{d f(x')}{dx} = 0[/tex]

Because x and x' are independent variables.
 
  • #3
But isn't the second term:

[tex]
\int \frac{d f(x')}{dx} \delta(x-x') \right] dx'=\frac{d f(x)}{dx}
[/tex]

by using the sifting property of the delta function?
 

Related to Shankar CH1 Derivative of Dirac delta

1. What is the Shankar CH1 Derivative of Dirac delta?

The Shankar CH1 Derivative of Dirac delta is a mathematical concept used in quantum mechanics to represent the derivative of the Dirac delta function. It is commonly used in the study of wavefunctions and probability in quantum mechanics.

2. How is the Shankar CH1 Derivative of Dirac delta calculated?

The Shankar CH1 Derivative of Dirac delta is calculated by taking the derivative of the Dirac delta function, which is a mathematical representation of an infinitely narrow peak. This derivative is then used in various equations and calculations in quantum mechanics.

3. What is the significance of the Shankar CH1 Derivative of Dirac delta in quantum mechanics?

The Shankar CH1 Derivative of Dirac delta is significant in quantum mechanics because it allows for the calculation of probabilities and wavefunctions in a mathematical framework. It is also used in the study of quantum systems and their behavior.

4. Can the Shankar CH1 Derivative of Dirac delta be applied to other fields of science?

The Shankar CH1 Derivative of Dirac delta is primarily used in the field of quantum mechanics. However, it can also be applied in other fields such as signal processing and engineering, where it is used to analyze signals and systems.

5. Are there any limitations or drawbacks to using the Shankar CH1 Derivative of Dirac delta?

One limitation of using the Shankar CH1 Derivative of Dirac delta is that it is only applicable to certain types of functions and may not accurately represent all systems in quantum mechanics. Additionally, it can be difficult to interpret and understand, making it challenging to use in practical applications.

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