Exploring Solutions to $\phi$ and $\ket{\overrightarrow{P}}$

In summary, the conversation discusses the analysis of a quantity that diverges. The integral of the given expression is shown to diverge as the variable k approaches infinity due to the behavior of the integrand. This is demonstrated by considering the limit of the integrand as k approaches infinity.
  • #1
Diracobama2181
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TL;DR Summary
Currently needing insight on re normalization for $$\bra{ \overrightarrow{P'}}\phi^4\ket{ \overrightarrow{P}}$$.
I already know this quantity diverges, however I was wondering where to go from there. Any resource would be appreciated. Thank you.
Useful Information:
$$\phi=\int\frac{d^3k}{2\omega_k (2\pi)^3}(\hat{a}(\overrightarrow{k})e^{-ikx}+\hat{a}(\overrightarrow{k})^{\dagger}e^{ikx}))$$
$$\ket{\overrightarrow{P}}=\hat{a}(\overrightarrow{k})^{\dagger}\ket{0}$$
 
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  • #2
$$\bra{\overrightarrow{P}}\phi\ket{0}=\frac{1}{2\omega_k (2\pi)^3}(\hat{a}(\overrightarrow{k})e^{-ikx}+\hat{a}(\overrightarrow{k})^{\dagger}e^{ikx})$$To show that this quantity diverges, you will need to analyze the behavior of the integrand as $k \rightarrow \infty$. To do this, consider the limit of the integrand as $k \rightarrow \infty$:$$\lim_{k\rightarrow\infty}\frac{1}{2\omega_k (2\pi)^3}(\hat{a}(\overrightarrow{k})e^{-ikx}+\hat{a}(\overrightarrow{k})^{\dagger}e^{ikx})$$Since $\omega_k \propto k$, the denominator goes to infinity faster than the numerator as $k \rightarrow \infty$, so the integrand goes to 0. Therefore, the integral diverges as $k \rightarrow \infty$.
 

1. What is the significance of exploring solutions to $\phi$ and $\ket{\overrightarrow{P}}$?

The exploration of solutions to $\phi$ and $\ket{\overrightarrow{P}}$ is crucial in the field of quantum mechanics. These solutions represent the wave function and momentum of a quantum system, respectively, and understanding them is essential in predicting the behavior of particles at the quantum level.

2. How do you determine the solutions to $\phi$ and $\ket{\overrightarrow{P}}$?

The solutions to $\phi$ and $\ket{\overrightarrow{P}}$ are determined through mathematical equations and calculations, such as the Schrödinger equation. These solutions are often represented as complex numbers and can be visualized as wave-like patterns.

3. Can the solutions to $\phi$ and $\ket{\overrightarrow{P}}$ change over time?

Yes, the solutions to $\phi$ and $\ket{\overrightarrow{P}}$ can change over time. This is known as wave function collapse, where the wave function of a particle collapses into a single state when it is measured or observed.

4. How do the solutions to $\phi$ and $\ket{\overrightarrow{P}}$ relate to each other?

The solutions to $\phi$ and $\ket{\overrightarrow{P}}$ are related through the uncertainty principle, which states that the more precisely we know the momentum of a particle, the less we know about its position, and vice versa. This means that the solutions to $\phi$ and $\ket{\overrightarrow{P}}$ cannot be known simultaneously with complete accuracy.

5. What are some real-world applications of exploring solutions to $\phi$ and $\ket{\overrightarrow{P}}$?

The exploration of solutions to $\phi$ and $\ket{\overrightarrow{P}}$ has led to significant advancements in technology, such as quantum computing and cryptography. It also has implications in fields such as medicine and materials science, where understanding the behavior of particles at the quantum level is crucial.

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