Representations of the Lorentz group in an arbitrary number of space-time dimensions$.$ Let $\mathrm{SO}(1,d-1)^\uparrow$ be the connected Lorentz group in $d$ dimensions. I am looking for a book/article where its finite-dimensional projective representations are studied in detail. Rather surprisingly, I haven't been able to find anything online, so here I am.
Some topics that I'd like to see discussed in the references are:


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*Does any projective representation correspond to a regular representation of the spin group $\mathrm{Spin}(1,d-1)$?

*Is any projective representation decomposable (i.e., it can be written, up to similarity, as the direct sum of irreducible representations)?

*How can we classify all irreducible representations? in other words, how many labels do we need in order to specify a particular representation?  are they half-integers? (in $d=4$, we have two labels, cf. the $(m,n)$ representation, which is $(2m+1)(2n+1)$-dimensional)

*Can an arbitrary object transforming according to an irreducible representation be written as the tensor product of spinors? (in $d=4$, an element transforming according to the $(m,n)$ representation can be identified with an object carrying $m$ dotted and $n$ un-dotted spinor indices).

*How does a large transformation ($C,P,T$) act on an arbitrary object transforming under a particular projective representation? (in $d=4$, the general formulas can be found e.g. in Wightman's PCT).
Any reference that addresses at least one of these topics will be welcome and appreciated. Ideally, the best reference would discuss all of them.

I think I know the answer for the first and second sub-questions, but I've included them anyway for completeness (the lack of results in the typical google searches suggests me that this post might end up being the first result when one googles "representations of the Lorentz in higher dimensions").
 A: The lecture notes 


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*Bekaert, X. and Boulanger, N., The unitary representations of the Poincaré group in any spacetime dimension [arXiv:hep-th/0611263]


are rather nice. I would say it assumes standard (physics) knowledge of QFT. Here is the abstract:

An extensive group-theoretical treatment of linear relativistic wave equations on Minkowski spacetime of arbitrary dimension $D>3$ is presented in these lecture notes. To start with, the one-to-one correspondence between linear relativistic wave equations and unitary representations of the isometry group is reviewed. In turn, the method of induced representations reduces the problem of classifying the representations of the Poincaré group
  $ISO(D−1,1)^\uparrow$ to the classication of the representations of the stability subgroups only. Therefore, an exhaustive treatment of the two most important classes of unitary irreducible representations, corresponding to massive and massless particles (the latter class decomposing in turn into the “helicity” and the “infinite-spin” representations) may be performed via the well-known representation theory of the orthogonal groups $O(n)$ (with $D−3\leq n\leq D−1$). Finally, covariant wave equations are given for each unitary irreducible representation of the Poincaré group with non-negative mass-squared. Tachyonic representations are also examined. All these steps are covered in many details and with examples. The present notes also include a self-contained review of the representation theory of the general linear and (in)homogeneous orthogonal group s in terms of Young diagrams.

This reference at least provides the answer to the OP's subquestion (2) [see Section 1.3], and, I think, subquestion (3) [namely: Young diagrams, see Section 4.3 onwards].
See also Section 3 of 


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*Vasiliev, M. A., Introduction into higher-spin gauge theory, lecture notes for a course at Utrecht University taught in Spring 2014 (draft, 2015)



For the more mathematically inclined reader, the lecture notes


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*Van der Ban, E., Representation theory and applications in classical quantum mechanics, lectures for the MRI Spring School ‘Lie groups in Analysis, Geometry and Mechanics’ (2006)


certainly deserve to be mentioned. Assuming familiarity with analysis, differential geometry and functional analysis, this reference gives a nice and detailed mathematical treatment of the topic. It includes such things as the basics of representation theory, lifting projective reps to (anti)unitary reps of the universal cover [answering subquestion (1)], the spectral-theory prerequisites, induced representations and the reverse construction, and representations of semi-direct products.
[I would expect the detailed answer to question (2) to be here somewhere too, but haven't found it upon skimming the text.] 
The applications discussed towards the end, viz. Wigner's classification of unitary Poincaré irreps (see Section 12 onwards), focus on the case $d=4$, but the discussion is still instructive.
