In Lesson 19 (Series Solutions near a Singular Point), Example 1 glosses over a subtle, difficult, and perhaps important point. For the equation 4xy''[x] + 2*y'[x] + y[x] == 0, one recursion relation is derived leading to the sequence of coefficients {a[0], -a[0]/2!, +a[0]/4!, -a[0]/6!, ...} and another relation is derived leading to {a[0], -a[0]/3!, +a[0]/5!, -a[0]/7!, ...}.
Both these sequences appear in my old CRC handbook table of trigonometric series. The first is for Cos[x] and the second is for Sin[x]. But Lesson 19 goes on to say that the sequences we've just derived are for Cos[Sqrt[x]] and for Sin[Sqrt[x]] . Where did the Sqrt[..] come from?
The answer is implicit when you show the result of Series[Cost[Sqrt[x]], {x, 0, 3}]. There, we discover that the powers of x in the Cos series are {1, x, x^2, x^3, ...}, while the powers in my trust old CRC handbook are {1, x^2, x^4, x^6, ...} (each term the square of CRC's list). For Sin, CRC shows {x, x^3, x^5, x^7, ...} instead of {x^(1/2), x^(3/2), x^(5/2), x^(7/2), ...} as shown by Mathematica for Sin[Sqrt[x]].
QUESTION: How are we to know the powers of x that go with each term in the series expansion? I could probably answer this question 55 years ago in Calc 210, but it eludes me now.