Free Field Operator: Building Quantum Fields

Free Field Operator: Building Quantum Fields How Quantum Fields Evolve Without Interactions 馃幆 Our Goal We aim to construct the free scalar field operator \( A(x,t) \), which describes a quantum field with no interactions—just free particles moving across space-time. 馃 Starting Expression This is the mathematical formula for our field \( A(x,t) \): \[ A(x, t) = \frac{1}{(2\pi)^{3/2}} \int_{\mathbb{R}^3} \frac{1}{\sqrt{k_0}} \left[ e^{i(k \cdot x - k_0 t)} a(k) + e^{-i(k \cdot x - k_0 t)} a^\dagger(k) \right] \, dk \] x: Spatial position t: Time k: Momentum vector k₀ = √(k² + m²): Relativistic energy of the particle a(k): Operator that removes a particle (annihilation) a†(k): Operator that adds a particle (creation) 馃З What Does This Mean? The field is made up of wave patterns (Fourier modes) linked to momentum \( k \). It behaves like a system that decides when and where ...

Distributional Derivative of ( f(x) = x^\lambda ) for ( x > 0 ): Theory & SageMath Implementation

Distributional Derivative of ( f(x) = x^\lambda ) for ( x > 0 ): Theory & SageMath Implementation

Distributional Derivative of \( f(x)=x^位 \) for 饾懃>0: Theoretical Insights and SageMath Implementation

1. Introduction

In this post, we dive deeper into the world of generalized (distributional) derivatives and examine how singularities affect the process of differentiation.
We focus on the function: \[ f(x) = x^\lambda \], for 饾懃>0 , with \( \quad -1 < \lambda < 0 \)
This function is locally summable, but its classical derivative: \[ f'(x) = \lambda x^{\lambda - 1} \] is not integrable near 饾懃=0, and hence not a true function in the sense of distributions. To handle this, we need a regularization approach to define its derivative in a meaningful distributional sense.
Can differentiation be redefined at singular points? What happens when classical differentiation fails? Let's explore these ideas, both theoretically and computationally using SageMath.

2. Theoretical Foundation

2.1 Functional Derivative Definition

In the theory of distributions, we define the derivative of a function \( 饾憮(饾懃) \)via its action on a test function \( \varphi(x) \) \[ (f', \varphi) = -\int_{0}^{\infty} f(x) \varphi'(x) ,dx \] For \( f(x)= x^\lambda \), this become: \[ (f', \varphi) = -\int_{0}\lambda \varphi'(x) ,dx \] This integral diverges at 饾懃=0 if \( 饾渾 < 0 \) , so we apply a regularization technique by subtracting the singularity at the origin: \[ \varphi(x) \rightarrow \varphi(x) - \varphi(0) \] Now the integral becomes: \[ (f', \varphi) = -\int_{0}\lambda (\varphi'(x) - \varphi'(0)) ,dx\] This regularized form defines a distribution and justifies the generalized derivative as: \[ (x^\lambda)' = \lambda x^{\lambda - 1} \] ,valid only when paired with test functions vanishing at x=0

3. SageMath Implementation

We now use SageMath to verify and visualize the behavior of this distributional derivative.

3.1 Define the Functionn

      
from sympy import Heaviside
from sage.all import var, integrate, diff

# Declare variables with valid names
x, lam = var('x lam')  # Changed 'lambda' to 'lam'

# Define f(x) = x^lam * Heaviside(x)
f_x = x**lam * Heaviside(x)

print("Function f(x):", f_x)
	
    

3.2 Compute Generalized Derivative

      
# Symbolic derivative using Sage
f_prime = diff(f_x, x)

print("Symbolic derivative f'(x):", f_prime)
	
    

This result reveals the Dirac delta behavior at 饾懃=0, capturing the singular nature of the derivative. The term 饾浛(饾懃) ensures the correctness of the derivative in the distributional framework.

3.3 Functional Regularization (Integration by Parts)

We now apply integration by parts to compute the generalized derivative manually:

      
phi = var('phi')  # Test function placeholder

# Functional form of generalized derivative
regularized_f_prime = -integrate(x**lam * diff(phi, x), x, 0, +oo)

print("Regularized functional:", regularized_f_prime)
	
    

This expression represents the functional action of the derivative on a test function 饾湋(饾懃), and corresponds to the distributional interpretation.

4. Visualization

To visualize the function \( f(x) = x^\lambda \cdot \theta(x) \) for different values of 饾渾, try:

      
from sympy import Heaviside
from sage.all import plot, var

x = var('x')

# Define the function
f_x = x**0.5 * Heaviside(x)

# Restrict the domain to x ≥ 0
plot(f_x, (x, 0, 5), title="f(x) = x^0.5 * Heaviside(x)")
	
    

馃搳 Try different values:

  • 位=−0.5 → singular at origin
  • 位=1, 位=2 → smooth behavior

This helps understand how the function behaves near the singularity at 饾懃=0.

5. Conclusion

  • The function \( f(x) = x^\lambda \) is not classically differentiable at 饾懃=0 for 饾渾<0, but its distributional derivative is well-defined.
  • Regularization is essential to make sense of otherwise divergent expressions.
  • SageMath is a powerful tool for computing and visualizing such expressions, offering both symbolic and functional insights.

Next upcoming

"Beyond \(x^\lambda \): Exploring Regularization Methods for Singular Integrals in Generalized Functions"

  • Logarithmic singularities \( f(x)=ln∣x∣ \)
  • Principal value integrals
  • Distributions with non-integrable behavior

馃挕 Try It Yourself! Now You can copy and paste directly into here Run SageMath Code Here

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