fermions - Supersymmetry transformations as coordinate transformations

Usually, a supersymmetry transformation is carried out on bosonic and fermionic fields which are functions of the coordinates (or on a superfield which is a function of real and fermionic coordinates). But, is it possible to interpret supersymmetry transformations as coordinate transformations on the set of coordinates $(x^0,\ldots,x^N,\theta_1,\ldots,\theta_M)$?

The problem I see is that the coordinates would transform something like $x^\mu\rightarrow x^\mu+\theta\sigma\bar{\theta}$ which is no longer a real (or complex) number, but a commuting Grassmann number. Can one make sens of a coordinate position no longer being a real number?

Edit: To clarify, this is NOT about confusion in what happens when adding real numbers with commuting grassmann numbers in general. That the lagrangian in QFT for example is not a real number, but a commuting grassmann number, is fine. What I am confused about is really how to make sense of coordinates that are grassmannian. Coordinates are supposed to describe a position in spacetime/on a manifold, and it seems to me that it is essential that a position is a standard real number.

Answer

Comments to the question (v3):

1. 
   
   

   Recall that a supernumber $z=z_B+z_S$ consists of a body $z_B$ (which always belongs to $\mathbb{C}$) and a soul $z_S$ (which only belongs to $\mathbb{C}$ if it is zero), cf. e.g. this Phys.SE post.

   
   


2. 
   

   An observable/measurable quantity can only consist of ordinary numbers (belonging to $\mathbb{C}$). It does not make sense to measure a soul-valued output in an actual experiment.

   
   


3. 
   

   Souls are indeterminates that appear in intermediate formulars, but are integrated (or differentiated) out in the final result.

   
   


4. 
   

   In a superspace formulation of a field theory, a Grasmann-even spacetime coordinates $x^{\mu}$ in superspace is promoted to a supernumber, and is not necessarily an ordinary number.

   
   
   


5. 
   

   A supersymmetry-translation of a Grasmann-even spacetime coordinate $x^{\mu}$ only changes the soul (but not the body) of $x^{\mu}$.

   
   


6. 
   

   Note that in the mathematical definition of a supermanifold, the focus of the theory is not on spacetime coordinates per se, but (very loosely speaking) rather on certain algebras of functions of spacetime. See also e.g. Refs. 1-3 for details.

   
   

References:

1. 
   

   Pierre Deligne and John W. Morgan, Notes on Supersymmetry (following Joseph Bernstein). In Quantum Fields and Strings: A Course for Mathematicians, Vol. 1, American Mathematical Society (1999) 41–97.

   
   


2. 
   

   V.S. Varadarajan, Supersymmetry for Mathematicians: An Introduction, Courant Lecture Notes 11, 2004.

   
   


3. 
   

   C. Sachse, A Categorical Formulation of Superalgebra and Supergeometry, arXiv:0802.4067.