A conceptual question about spin I read in Landau's quantum mechanics（section 62) that if the Hamiltonian does not involve spin, the total wave function can be written 
$$ \psi ( x_1, x_2, ...) \chi ( \sigma_1 , \sigma_2 ,...)$$ 
in which coordinate and spin dependence are separated.
Does this mean that for such Hamiltonian for a system of identical particles, there is always a complete set of wavefunctions of form
$$ \psi ( x_1, x_2, ...) \chi ( \sigma_1 , \sigma_2 ,...)$$ 
which are either symmetric or antisymmetric under interchange of labels?
If that is true, why exactly are the spin part and the coordinate part be neither symmetric nor antisymmetric in general, according to Landau（section 63)?
 A: This is actually a very insightful question. 
You are correct to say that a general wavefunction for a Hamiltonian without a spin interaction may be written as
$$\psi(x_1,x_2,\dots)\chi(\sigma_1,\sigma_2,\dots)$$
where $\psi$ is the spatial wavefunction and $\chi$ the spin wavefunction.
For a system of bosons, the overall wavefunction must be invariant under all permutations, in other words
$$P (\psi \chi) = \psi \chi$$
where $P$ is the parity operator. We call such overall wavefunctions symmetric.
For a system of fermions, the overall wavefunction must change sign under an odd permutation, in other words
$$ P (\psi \chi) = \textrm{sign}(P)\psi \chi$$
We call such overall wavefunctions antisymmetric.
We must now examine what restrictions these conditions place on the spatial and spin wavefunctions $\psi$ and $\chi$. 
Suppose we have a system of 2 identical bosons. Then we must have either


*

*both $\psi$ and $\chi$ are symmetric under interchange

*both $\psi$ and $\chi$ are antisymmetric under interchange 


In both cases this produces a symmetric overall wavefunction, since $(-1)^2 = 1$.
Now more generally, suppose we have $n$ identical bosons. Then there is more freedom in choosing $\psi$ and $\chi$ such that you get something overall symmetric. If I choose $\psi$ and $\chi$ carefully enough, they don't have to be completely symmetric or antisymmetric themselves!
This comes down to the fact that for several particles, there are more representations of the symmetric group than just the totally symmetric or totally antisymmetric ones. In fact you get one representation for each Young diagram you can draw.
$\psi$ and $\chi$ have definite linear transformations under particle permutation, so must lie in representations of the symmetric group. We just need to know which Young diagrams match up correctly to give the right overall symmetry behaviour.
For bosons, both $\psi$ and $\chi$ must be represented by the same Young diagram in order to get overall symmetry. For fermions, the Young diagrams for $\psi$ and $\chi$ must be related by swapping rows and columns in order to get overall antisymmetry.
Feel free to ask some more questions if you are still confused. I've tried to elucidate what Landau was talking about in section 63 - reread his excellent account and see whether you understand it better now!
A: Editted: total wave function of Fermion system = anti-symmetric --> either spatial or spin function is anti-symmetric 
total wave function of boson system = symmetric --> both symmetric
