# A question about the Bosonization of the Thirring model

Is there a way or sense in which one can Bosonize this kind of a Lagrangian,

$L = \bar{\psi}\gamma^\mu \partial _\mu \psi + f(x) \bar{\psi}\psi$

for $f(x)$ being some function on space-time.

• What is the most pedagogic reference which explains the Thirring Model/Sine-Gordon bosonization from scratch?
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Sorry, I should have said that my answer refers to your second question (i.e. the Thirring / sine-Gordon bosonization). As for your first question, one must have in mind that bosonization of fermion fields only works in 1+1 dimensions (this is missing from your question). That being said, it doesn't look much different from bosonization of free fermion fields, although your model may get messy depending on the form of $f$. Do you have a specific $f$ in mind? –  Pedro Lauridsen Ribeiro Feb 20 '14 at 6:49
Can you explain as to how do you think the 1+1 bosonization will work with that $f$? It seems you think it will! (...also it seems that Bosonization of these theories makes sense for higher-dimensions also - arxiv.org/pdf/hep-th/9509173v2.pdf ) –  user6818 Feb 21 '14 at 2:24
Your model is still free in the sense that the field equations are linear, but you no longer have a translation invariant vacuum state if $f$ is not constant. Nevertheless, you still have quasi-free reference states (i.e. such that all truncated $n$-point functions vanish for $n>2$) whose 2-point function have a short distance behavior similar to that of a vacuum state (the so-called Hadamard states). If one works with one of these states, the bosonization procedure shouldn't be that different from the standard one applied to Dirac fields in 1+1 dimensions. –  Pedro Lauridsen Ribeiro Feb 21 '14 at 21:27