Optimal quantum metrology for two-photon absorption
- URL: http://arxiv.org/abs/2311.12555v1
- Date: Tue, 21 Nov 2023 12:07:41 GMT
- Title: Optimal quantum metrology for two-photon absorption
- Authors: Athena Karsa, Ranjith Nair, Andy Chia, Kwang-Geol Lee and Changhyoup
Lee
- Abstract summary: Two-photon absorption (TPA) is a nonlinear optical process with wide-ranging applications from spectroscopy to super-resolution imaging.
We study the potential of single-mode quantum light to enhance TPA parameter estimation through the quantum Fisher information (QFI)
For fixed average energy $barn in 2mathbbN$, the Fock state is shown to be optimal for large TPA parameters, while a superposition of vacuum and a particular Fock state is optimal for small absorption for all $barn$.
- Score: 0.0
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Two-photon absorption (TPA) is a nonlinear optical process with wide-ranging
applications from spectroscopy to super-resolution imaging. Despite this, the
precise measurement and characterisation of TPA parameters are challenging due
to their inherently weak nature. We study the potential of single-mode quantum
light to enhance TPA parameter estimation through the quantum Fisher
information (QFI). Discrete variable (DV) quantum states (defined to be a
finite superposition of Fock states) are optimised to maximise the QFI for
given absorption, revealing a quantum advantage compared to both the coherent
state (classical) benchmark and the single-mode squeezed vacuum state. For
fixed average energy $\bar{n} \in 2\mathbb{N}$, the Fock state is shown to be
optimal for large TPA parameters, while a superposition of vacuum and a
particular Fock state is optimal for small absorption for all $\bar{n}$. This
differs from single-photon absorption where the Fock state is always optimal.
Notably, photon counting is demonstrated to offer optimal or nearly optimal
performance compared to the QFI bound for all levels of TPA parameters for the
optimised quantum probes. Our findings provide insight into known limiting
behaviours of Gaussian probes and their different Fisher information (FI)
scalings under photon counting ($\propto \bar{n}^2$ for squeezed vacuum states
versus $\bar{n}^3$ for coherent states). The squeezed state outperforms
coherent states for small TPA parameters but underperforms in the intermediate
regime, becoming comparable in the large absorption limit. This can be
explained through fundamental differences between behaviours of even and odd
number Fock states: the former's QFI diverges in both large and small
absorption limits, while the latter diverges only in the small absorption
limit, dominating at intermediate scales.
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