Cauchy defined infinitesimal as a variable or a function tending to zero, or as a null sequence.
While I found the definition is not so popular and nearly discarded in math according to the following statement.
(1). Infinitesimal entry in Wikipedia:
Some older textbooks use the term "infinitesimal" to refer to a variable or a function tending to zero
Why textbooks involved with the definition is said to be old ?
(2). Robert Goldblatt, Lectures on the Hyperreals: An Introduction to Nonstandard Analysis, P15
(His = Cauchy's)
Why says 'Even'?
(3). Abraham Robinson, Non-standard analysis, P276
why Cauchy's definition of infinitesimal, along with his 'basic approach' was superseded?
Besides, I found most of the Real analysis or Calculus textbooks, such as Principles of mathematical analysis(Rudin) and Introduction to Calculus and Analysis(Richard Courant , Fritz John), don't introduce Cauchy's definition of infinitesimal, Why ? Why Cauchy's definition of infinitesimal was unpopular and not widely used, and nearly discarded?
P.S. I refered some papers still cannot find the answer.
Because Cauchy's formulation doesn't quite correspond to what we want it to be. For example, suppose $y$ is a function of $x$. Per Cauchy, we take $dx$ to be some decreasing value. What does that mean mathematically? Decreasing with respect to what? Evidently, $dx$ is to be a function of some other variable, which I'll call $t$. $dx = dx(t)$. Calling it a sequence as one of your quotes does just restricts the domain of $t$ to the natural numbers. The requirement on the function is that some appropriate limit with respect to $t$ of $dx(t)$ is $0$.
Now $dy$ is also some function of $t$, determined by the relationship between $y$ and $x$. In particular, $dy(t) = y(x + dx(t)) - y(x)$. Well and good, but by this definition, $\frac{dy}{dx}$ is a function of both $x$ and $t$. That is not what we want. We want $\frac{dy}{dx}$ to be the derivative, which is a function of $x$ alone. By the Cauchy definition, $$y'(x) = \lim_t \frac{dy}{dx} \ne \frac{dy}{dx}$$ Since the latter depends on $t$.
So Cauchy's idea came closer to putting the idea on a solid foundation, but it still needed refining. Once suitable refinments were established, it has fallen out of favor.