I got motivation from twisted Cohomology where we twisted the derivative $d_\psi=d+\psi\wedge$ and find cohomology class $H_{\psi}^k(M)$ where $\psi$ is closed one form.
I try to define twisted connection similarly, which lead me to define $\nabla_{X,\psi}e_j=\omega^i_j(X)e_i+\psi(X)e_j.\tag1$ which satisfy:
- $\nabla_{X,\psi}(fs)=X_{\psi}(f)s+f\nabla_{X,\psi}(s)$ where we define $X_\psi(f)=X(f)+\psi(X)\cdot f\tag2$
Here if $\psi=0$ then this exactly matches with our classical notion of connection satisfying the ordinary Leibniz rule. Does this really define a connection? Is there any existing work related with this? It will be a great help if anyone provide some information or guidance.
I tried to compute associate curvature form using $(1)$ and $(2)$, $\nabla_{X,\psi}\nabla_{Y,\psi}e_j=[X(\omega^i_j(Y))+\psi(X)\cdot\omega^i_j(Y)]e_i+\omega^k_j(Y)\omega^i_k(X)e_i+[X(\psi(Y))+\psi(X)\cdot\psi(Y)]e_j+\psi(Y)[\omega^k_j(X)e_k+\psi(X)e_j]$ and Interchanging $X$ and $Y$ will give $\nabla_{Y,\psi}\nabla_{X,\psi}e_j$. And $$\nabla_{[X,Y],\psi}e_j\stackrel{1}{=}\omega^i_j([X,Y])e_i+\psi([X,Y])e_j.$$ Combining all we get, \begin{align} &\nabla_{X,\psi}\nabla_{Y,\psi}e_j-\nabla_{Y,\psi}\nabla_{X,\psi}e_j-\nabla_{[X,Y],\psi}e_j\\ &=d\omega^i_j(X,Y)e_i+\omega^k_j\wedge\omega^i_k(X,Y)e_i\\&+[X(\psi(Y))-Y(\psi(X))-\psi([X,Y])]e_j+\psi\wedge\omega^k_j(Y,X)e_k\\ &=d\omega^i_j(X,Y)e_i+\psi\wedge\omega^i_j(Y,X)e_i+\omega^k_j\wedge\omega^i_k(X,Y)e_i\\&+[X(\psi(Y))-Y(\psi(X))-\psi([X,Y])]e_j \end{align} I see some inconsistency, Like I was guessing to have $$d_\psi\omega^i_j(X,Y)e_j=d\omega^i_j(X,Y)e_i+\psi\wedge\omega^{i}_j(X,Y)e_i$$ but from the calculation I got something like $$\cdots=[\psi(Y)\omega^k_j(X)-\psi(X)\omega^k_j(Y)]e_k=\psi\wedge\omega^k_j(Y,X)e_k=\psi\wedge\omega^i_j(Y,X)e_i.$$ Another problem is, I couldn't interpret what $[X(\psi(Y))-Y(\psi(X))-\psi([X,Y])]e_j$ represent here?