Linear differential equation of first order in EXP(C)

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Discussion Overview

The discussion revolves around the existence of solutions to a linear differential equation of first order within the ring of exponential sums $\text{EXP}(\mathbb{C})$. Participants explore various cases based on the coefficients of the equation and the nature of the functions involved.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant presents a general form of the linear differential equation and derives conditions for the existence of solutions based on the parameters involved.
  • Another participant breaks down the problem into four distinct cases based on the values of coefficients $a$ and $b$, analyzing the implications for the existence of solutions in each case.
  • Concerns are raised about the assumption of linear independence of the functions $\{ e^{\mu_i z} \}$, with examples provided to illustrate potential dependencies among them.
  • Some participants suggest that the reasoning presented is correct but emphasize the need to clarify the basis formed by the functions involved.
  • A later reply indicates that the original reasoning may be valid but suggests that certain conditions under which solutions exist should be explicitly stated.

Areas of Agreement / Disagreement

Participants express differing views on the independence of the exponential functions and the conditions under which solutions exist. While some agree with the reasoning presented, others challenge the assumptions made, leading to an unresolved discussion regarding the implications of these assumptions.

Contextual Notes

Participants highlight specific cases where solutions may not exist, depending on the values of the coefficients and the nature of the functions involved. However, the discussion does not resolve the implications of these cases fully.

mathmari
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Hey! :o

I want to check if there is a solution of a linear differential equation of first order in the ring of exponential sums $\text{EXP}(\mathbb{C})$. I have done the following: The general linear differential equation of first order is $$ax'(z)+bx(z)=y(z) \tag{*}$$
where $x,y \in \text{EXP}(\mathbb{C})$.

We have that $$y(z)=\sum_{i=1}^N \alpha_i e^{\mu_i z}, \ \ x(z)=\sum_{i=1}^N \beta_i e^{k_i z} \ \ \text{ so } \ \ x'(z)=\sum_{i=1}^N \beta_i k_i e^{k_i z}$$

$$(*) \Rightarrow a\sum_{i=1}^N \beta_i k_i e^{k_i z}+b\sum_{i=1}^N \beta_i e^{k_i z}= \sum_{i=1}^N \alpha_i e^{\mu_i z} \Rightarrow \sum_{i=1}^N \left [a\beta_i k_i +b\beta_i \right ]e^{k_i z}=\sum_{i=1}^N \alpha_i e^{\mu_i z}$$ For $k_i=\mu_i$ we have the following:

$$\sum_{i=1}^N \left [\beta_i (a\mu_i +b) \right ]e^{\mu_i z}=\sum_{i=1}^N \alpha_i e^{\mu_i z} \Rightarrow \sum_{i=1}^N \left [(a \mu_i +b)\beta_i -\alpha_i\right ]e^{\mu_i z}=0$$ 1. If for at least one $i$ with $\alpha_i\ne0$ we have $a\mu_i+b=0$, there is no solution.

2. If for at least one $i$ with $\alpha_i = 0$ we have $a\mu_i+b \neq 0$, we have that $\beta_i=0$.

3. If for all $i$ it holds that $\alpha_i = 0 \land a\mu_i+b = 0$, then thee are infinitely many solutions.

4. If for all $i$ it holds that $\alpha_i\ne0 \land a\mu_i+b\ne0$, then there is exactly one solution, with $\beta_i=\frac{\alpha_i}{a\mu_i+b}$.
Is everything correct? Have I forgotten a case? (Wondering)
 
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I did it also as follows by taking cases:
  • $\textbf{Case 1.}$
    $a=0, b \neq 0$

    Then we have $bx(z)=y(z)$.
    So, the solution is $$x(z)=\frac{1}{b}y(z) \in \text{EXP}(\mathbb{C})$$
  • $\textbf{Case 2.}$
    $a\neq 0, b=0$

    Then we have $ax'(z)=y(z)$.

    We have that $\displaystyle{x'(z)=\frac{1}{a}y(z)}$, where $\displaystyle{y(z)=\sum_{i=1}^N \alpha_i e^{\mu_i z}}$, so $\displaystyle{x'(z)=\frac{1}{a}\sum_{i=1}^N \alpha_i e^{\mu_i z}}$.
    • If $\exists j$ such that $\mu_j =0 \land \alpha_j \neq 0$ then $\displaystyle{x'(z)=\frac{1}{a}\sum_{i=1}^{j-1} \alpha_i e^{\mu_i z}+\frac{\alpha_j}{a}+\frac{1}{a}\sum_{i=j+1}^N \alpha_i e^{\mu_i z}}$ then $\displaystyle{x(z)=\frac{1}{a}\sum_{i=1}^{j-1} \frac{\alpha_i}{\mu_i} e^{\mu_i z}+\frac{\alpha_j}{a}z+\frac{1}{a}\sum_{i=j+1}^N \frac{\alpha_i}{\mu_i} e^{\mu_i z}} \notin \textbf{EXP}{(\mathbb{C})}$. So, there is no solution.
    • If $\mu_i \neq 0$ for $i$ for which $\alpha_i \neq 0$ then the solution is $\displaystyle{x(z)=\frac{1}{a}\sum_{i=1}^N \frac{\alpha_i}{\mu_i} e^{\mu_i z}}\in \text{EXP}(\mathbb{C})$.
  • $\textbf{Case 3.}$
    $a=0, b=0$

    Then we have $0=y(z)$.
    • If $y(z)=0$ then we have infinitely many solutions.
    • If $y(z) \neq 0$ then we have no solution.
  • $\textbf{Case 4.}$
    $a \neq 0, b \neq 0$

    Then we have $$ax'(z)+bx(z)=y(z) \Rightarrow x'(z)+\frac{b}{a} x(z)=\frac{1}{a}y(z) \ \ \ \ \ (*)$$

    We have that $$y(z)=\sum_{i=0}^N \alpha_i e^{\mu_i z}, x(z)=\sum_{i=0}^N \beta_i e^{k_i z}=\beta_0 +\sum_{i=1}^N \beta_i e^{k_i z}, also x'(z)=\sum_{i=1}^N \beta_i k_i e^{k_i z} $$

    $$(*) \Rightarrow \sum_{i=1}^N \beta_i k_i e^{k_i z}+\frac{b}{a} \left [\beta_0 +\sum_{i=1}^N \beta_i e^{k_i z}\right ]=\frac{1}{a} \left [\sum_{i=0}^N \alpha_i e^{\mu_i z}\right ] \\
    \Rightarrow \frac{b}{a}\beta_0 +\sum_{i=1}^N \left [\beta_i k_i +\frac{b}{a}\beta_i \right ]e^{k_i z}=\frac{1}{a}\alpha_0+\sum_{i=1}^N \alpha_i e^{\mu_i z} $$

    So, the following must hold:

    $$\left\{\begin{matrix}
    \frac{b}{a}\beta_0=\frac{1}{a}\alpha_0\\
    \beta_i k_i+\frac{b}{a}\beta_i=\alpha_i, \ \ i=1, \dots , N\\
    k_i=\mu_i, \ \ i=1, \dots , N
    \end{matrix}\right. \Rightarrow \left\{\begin{matrix}
    \beta_0=\frac{\alpha_0}{b}\\
    \beta_i \mu_i+\frac{b}{a}\beta_i=\alpha_i, \ \ i=1, \dots , N\\
    k_i=\mu_i, \ \ i=1, \dots , N
    \end{matrix}\right. \Rightarrow \left\{\begin{matrix}
    \beta_0=\frac{\alpha_0}{b}\\
    \beta_i \left (\mu_i+\frac{b}{a}\right )=\alpha_i, \ \ i=1, \dots , N\\
    k_i=\mu_i, \ \ i=1, \dots , N
    \end{matrix}\right. $$
    • If $\displaystyle{\mu_i \neq -\frac{b}{a}}$, then the solution is $\displaystyle{x(z)=\frac{\alpha_0}{b}+\sum_{i=1}^N \frac{\alpha_i}{\mu_i+\frac{b}{a}}e^{\mu_i z}}$.
    • If $\displaystyle{\mu_i=-\frac{b}{a}}$ then if $\alpha_i=0$ then there are infinitely many solutions, but if $\alpha_i \neq 0$ then there is no solution.
Is this correct? Have I taken into consideration all the possible cases? (Wondering)
 
Hey mathmari! (Wave)

It seems you assume that $\{ e^{\mu_i z} \}$ forms an independent basis as long as the $\mu_i$ are distinct.
However, that is not the case.
For instance $1\cdot e^{i\pi/2 z} = -1 \cdot e^{-i\pi/2 z}$.
(Worried)
 
Last edited:
I like Serena said:
It seems you assume that $\{ e^{\mu_i z} \}$ forms an independent basis as long as the $\mu_i$ are distinct.
However, that is not the case.
For instance $1\cdot e^{i\pi/2} = -1 \cdot e^{-i\pi/2}$.
And $2e^{1+i} + 3e^{2+i} = (2e+3e^2)e^i$.
(Worried)

Ahaa... Ok... (Thinking)
And what could I change? (Wondering)
 
I like Serena said:
Hey mathmari! (Wave)

It seems you assume that $\{ e^{\mu_i z} \}$ forms an independent basis as long as the $\mu_i$ are distinct.
However, that is not the case.
For instance $1\cdot e^{i\pi/2 z} = -1 \cdot e^{-i\pi/2 z}$.
(Worried)

mathmari said:
Ahaa... Ok... (Thinking)
And what could I change? (Wondering)

Nevermind, I think $\{ e^{\mu_i z} :i=0..N, \text{ distinct } \mu_i\in \mathbb C \}$ does form a basis.
So I think your reasoning is correct, although you should probably mention that. (Thinking)
 
I like Serena said:
Nevermind, I think $\{ e^{\mu_i z} :i=0..N, \text{ distinct } \mu_i\in \mathbb C \}$ does form a basis.
So I think your reasoning is correct, although you should probably mention that. (Thinking)

Do you mean that I should mention that $\{ e^{\mu_i z} :i=0..N, \text{ distinct } \mu_i\in \mathbb C \}$ forms a basis? So, in the ring $\text{EXP}(\mathbb{C})$ the linear differential equation of first order has always a solution except at the following cases:
  • $a \neq 0 \land b =0 \land \mu_j =0 \land \alpha_j \neq 0$
  • $a=0 \land b=0 \land y \neq 0$
  • $a \neq 0 \land b \neq 0 \land \mu_i =-\frac{b}{a} \land \alpha_i \neq 0$

Is this correct? (Wondering)
 

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