In a recent reference $[1]$ the authors evocated a particular Hamiltonian,
$$H = c\chi(\tau)\mu(\tau)\otimes\Phi(x(\tau)), \tag{1}$$
calling it "interaction Hamiltonian". The physics in this situation is described in the following $[1]$:
An Unruh-Dewitt detector, moving along a trajectory $x(\tau)$ Minkowski spacetime $-$$\tau$ is the proper time$-$, where also, $c$ is a coupling constant, $\chi(\tau)$ is a smooth function $-$ compactly supported which satisfies how the interaction "is switched on and off, betwween the detector's monopole moment operator $\mu(\tau)$" and the field pulled back to the detector's worldline $\Phi(x(\tau))$ $-$
Well, my question lies beyond the particularity of that paper. Like, consider,
$$H = A \otimes B, \tag{2}$$
What is the meaning of usage of tensor products like $(1)$ or, in "general case", $(2)$? Is like the field components $A$ interacting with the $B$ components?
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