The Fourier series $$f(t) = d + \sum_{n=-1}^\infty a_n \cos(nt) + b_n \sin(nt),$$
can be written in the form
$$\sum_{n=-\infty}^\infty c_n e^{int},$$
where
$c_n = \begin{cases} d \quad \text{for} \ n = 0 \\ (a - ib_n)/2, \quad \text{for} \ n \ \text{positive} \\ (a_{-n} + ib_{-n})/2, \quad \text{for} \ n \ \text{negative}. \\ \end{cases} $
Now if I expand this I get
\begin{align} f(t) \sum_{n=-\infty}^\infty c_n e^{int} & = \sum_{n=-\infty}^\infty c_n \bigg(\cos(nt) + i \sin(nt)\bigg) \\ & = c_0 + \sum_{n=1}^\infty c_n \bigg(\cos(nt) + i \sin(nt) + \cos(-nt) + i \sin(-nt)\bigg) \\ & = c_0 + \sum_{n=1}^\infty c_n \bigg(\cos(nt) + i \sin(nt) + \cos(nt) - i \sin(nt)\bigg) \\ & = c_0 + \sum_{n=1}^\infty c_n 2\cos(nt). \end{align}
But now the Fourier series has lost its dependence on sin functions! Am I incorrect or is this telling me that we only need $\cos$ functions to represent any periodic function using a Fourier series?
I rewrite your solution: \begin{align} f(t)& = \sum_{n=-\infty}^\infty c_n e^{int}\\ & = \sum_{n=-\infty}^\infty c_n \bigg(\cos(nt) + i \sin(nt)\bigg) \\ & = c_0 + \sum_{n=1}^\infty c_n \bigg(\cos(nt) + i \sin(nt) \bigg)+\sum_{n=1}^\infty c_{-n} \bigg(\cos(-nt) + i \sin(-nt)\bigg) \\ & = c_0 + \sum_{n=1}^\infty \color{blue}{c_n \bigg(\cos(nt) + i \sin(nt) + \cos(nt) - i \sin(nt)\bigg)} \\ & = c_0 + \sum_{n=1}^\infty c_n 2\cos(nt). \end{align} the blue line is true if $c_n=c_{-n}$ or by definition $(a - ib_n)/2=(a_{-n} + ib_{-n})/2$ or $b_n=0$ that means $c_n$'s are real, with other notation $$f(t)=\sum_{n=-\infty}^\infty c_n e^{int}=d+\sum_{n>0}^\infty c_n e^{int}+\sum_{n<0}^\infty c_n e^{int}=d+\sum_{n>0}^\infty( c_n e^{int}+ c_{-n} )e^{-int}=d+\sum_{n>0}^\infty (a_n e^{int}+ a_n e^{-int})=d+\sum_{n>0}^\infty a_n 2\cos nt$$