{ "id": "1905.10557", "version": "v1", "published": "2019-05-25T08:48:53.000Z", "updated": "2019-05-25T08:48:53.000Z", "title": "Correlation function $g^{(k)}(0)$ and sub-$k$ photon emission", "authors": [ "Peter Grünwald" ], "categories": [ "quant-ph", "math-ph", "math.MP" ], "abstract": "We study the relation between the $k$th-order correlation function $g^{(k)}(0)$ at equal time for all operators and the projection of the underlying quantum state of light onto the subspace with less than $k$ photons. It was previously established that for $g^{(2)}(0)$ falling below 1/2, a non-zero projection on zero or single photons follows, as well as a lower bound on the ratio for single-to-multi-photon emission. Here we generalize these results to higher-orders $k$. When $g^{(k)}(0)$ falls below its value for the Fock state $|k\\rangle$ a nonzero projection on the subspace with less than $k$ photons can be concluded. In particular a nonzero lower bound is found, when vacuum is included in this space, whereas, when it is left out, the remaining space of $1$ to $k-1$ photons can have arbitrarily low projection. This is due to the influence of vacuum, artificially enhancing the value of $g^{(k)}(0)$. We derive an effective correlation function $\\tilde g^{(k)}(0)$, which takes the effect of vacuum into account and yields a nonzero lower bound on the ratio of sub-$k$-photon-to-$k$-or-more-photon emission. We examine these boundaries for different quantum states and derive a large-$k$ limit. Due to the monotone decrease of the boundaries with increasing $k$, this limit serves as a general lower bound for all correlation functions $g^{(k)}(0)$. Finally, we consider measurement of $\\tilde g^{(k)}(0)$.", "revisions": [ { "version": "v1", "updated": "2019-05-25T08:48:53.000Z" } ], "analyses": { "keywords": [ "photon emission", "nonzero lower bound", "quantum state", "th-order correlation function", "general lower bound" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }