Quantum absorption spectroscopy system
A quantum absorption spectroscopy system ( 1 ) includes a pump light source ( 11 ), a quantum interferometer ( 21 ), and a spectroscope ( 31 ). The pump light source ( 11 ) emits pump light. The quantum interferometer ( 21 ) causes quantum interference between a plurality of physical processes in which a quantum entanglement photon pair of a signal photon and an idler photon is generated through spontaneous parametric down-conversion of the pump light, a sample being arranged on a propagation path of the idler photon. The spectroscope ( 31 ) detects a signal photon from the quantum interferometer ( 21 ). The quantum interferometer ( 21 ) includes a single mode fiber (SMF) portion optically coupled to at least part of a propagation path of the signal photon and the propagation path of the idler photon.
1 . A quantum absorption spectroscopy system comprising:
a pump light source that emits pump light;
a quantum interferometer that includes a photon pair source that generates a quantum entanglement photon pair of a signal photon and an idler photon and causes quantum interference between a plurality of physical processes in which the quantum entanglement photon pair is generated through spontaneous parametric down-conversion of the pump light, a sample being arranged on a propagation path of the idler photon; and
a photodetector that detects the signal photon from the quantum interferometer, wherein the quantum interferometer includes:
a wavelength separation element that separates the quantum entanglement photon pair into the signal photon and the idler photon in accordance with a wavelength; and
a single mode fiber portion configured to measure the sample using propagation of the idler photon, the single mode fiber portion having a tapered fiber which is (i) optically coupled between the wavelength separation element and at least part of the propagation path of the idler photon and (ii) arranged external to the photon pair source.
2 . The quantum absorption spectroscopy system according to claim 1 , wherein the tapered fiber comprises:
a non-tapered portion, and
a taper waist portion thinner than the non-tapered portion,
the taper waist portion having a diameter included in a wavelength range from a visible range to a far-infrared range.
3 . The quantum absorption spectroscopy system according to claim 1 , wherein the tapered fiber is replaceable.
4 . The quantum absorption spectroscopy system according to claim 1 , wherein the quantum interferometer further includes:
a first mirror that reflects the idler photon, and
a second mirror that reflects the signal photon,
the first single mode fiber is optically coupled between the wavelength separation element and the first mirror,
the single mode fiber portion further includes a second single mode fiber that is optically coupled between the wavelength separation element and the second mirror and propagates light in a wavelength range of the signal photon, and
at least one of the first and second single mode fibers is a polarization maintaining fiber.
5 . The quantum absorption spectroscopy system according to claim 1 , wherein
the single mode fiber portion further includes a wideband single mode fiber that is optically coupled between the photon pair source and the wavelength separation element and propagates light in all wavelength ranges of the pump light, the signal photon, and the idler photon.
6 . The quantum absorption spectroscopy system according to claim 5 , wherein the wideband single mode fiber is a photonic crystal fiber.
7 . The quantum absorption spectroscopy system according to claim 1 , wherein
the single mode fiber portion includes a wideband single mode fiber that is optically coupled between the photon pair source and the wavelength separation element and propagates light in all wavelength ranges of the pump light, the signal photon, and the idler photon.
8 . A quantum absorption spectroscopy system comprising:
a pump light source that emits pump light;
a quantum interferometer that causes quantum interference between a plurality of physical processes in which a quantum entanglement photon pair of a signal photon and an idler photon is generated through spontaneous parametric down-conversion of the pump light, a sample being arranged on a propagation path of the idler photon; and
a photodetector that detects the signal photon from the quantum interferometer, wherein
the quantum interferometer includes a single mode fiber portion optically coupled to at least part of a propagation path of the signal photon and the propagation path of the idler photon, wherein
the pump light source is a pulsed light source,
the photodetector is a single-pixel photodetector, and
the single mode fiber portion includes a wavelength dispersion single mode fiber optically coupled to the single-pixel photodetector.
9 . The quantum absorption spectroscopy system according to claim 8 , wherein
the quantum interferometer is used in a high gain region in which a signal intensity of the single-pixel photodetector increases non-linearly as transmittance of the idler photon for the sample rises, and
the single mode fiber portion further includes an absorber that absorbs the idler photon.
10 . The quantum absorption spectroscopy system according to claim 1 , further comprising a processor that executes arithmetic processing for analyzing an absorption spectroscopy characteristic of the sample, wherein
the quantum interferometer further includes a phase converter that changes a phase of one of the signal photon and the idler photon,
the photodetector outputs a quantum interference signal in accordance with the number of the signal photons detected in a case where the phase of the one of the signal photon and the idler photon is changed by the phase converter, and
the processor calculates the absorption spectroscopy characteristic of the sample by Fourier transform on the quantum interference signal.
11 . The quantum absorption spectroscopy system according to claim 10 , wherein the processor
calculates a Fourier spectrum by Fourier transform on the quantum interference signal in a state where the sample is arranged on the propagation path of the idler photon, and further calculates a reference Fourier spectrum by Fourier transform on the quantum interference signal in a state where the sample is not arranged on the propagation path of the idler photon, and
calculates a complex transmittance spectrum of the sample based on a ratio between the Fourier spectrum and the reference Fourier spectrum.
12 . The quantum absorption spectroscopy system according to claim 11 , wherein the processor calculates an absorption spectrum of the sample by squaring an absolute value of the complex transmittance spectrum of the sample.
13 . The quantum absorption spectroscopy system according to claim 1 , wherein
the quantum interferometer generates a visible photon as the signal photon, and
the photodetector is a silicon-based photodetector.
14 . A quantum absorption spectroscopy system comprising:
a pump light source that emits pump light;
a pump light source that emits pump light;
a quantum interferometer that includes a photon pair source that generates a quantum entanglement photon pair of a signal photon and an idler photon and causes quantum interference between a plurality of physical processes in which the quantum entanglement photon pair is generated through spontaneous parametric down-conversion of the pump light, a sample being arranged on a propagation path of the idler photon; and
a photodetector that detects the signal photon from the quantum interferometer, wherein
the quantum interferometer includes:
a wavelength separation element that separates the quantum entanglement photon pair into the signal photon and the idler photon in accordance with a wavelength, and
a single mode fiber portion configured to measure the sample, the single mode fiber portion having a tapered fiber which is (i) optically coupled between the wavelength separation element and at least part of the propagation path of the idler photon and (ii) arranged external to the photon pair source, so as to measure the sample, and
the tapered fiber has a non-tapered portion and a taper waist portion thinner than the non-tapered portion and configured to be arranged in a vicinity of the sample so that an evanescent field of the propagation path of the idler photon and the sample interacts with each other.