Nanophotonic parametric quantum information processor
A photonic integrated circuit comprising one or more waveguides comprising a second order non-linearity configured to operate on optical pulses each having a pulse length shorter than 1000 optical cycles, as measured at their full width at half maximum. The circuit is configured to generate one or more quantum states carried by one or more of the optical pulses, manipulate one or more of the quantum states, and/or measure one or more of the quantum states.
1 . A photonic integrated circuit, comprising:
one or more waveguides comprising a second order non-linearity configured to operate on classical and/or quantum optical pulses each having a pulse length shorter than 1000 optical cycles, as measured at their full width at half maximum of their classical field values or their quantum wave functions, so as to at least:
generate one or more quantum states carried by one or more of the optical pulses,
manipulate one or more of the quantum states, or
measure one or more of the quantum states; and
wherein the waveguides comprise at least an optical parametric amplifier (OPA) comprising a phase-matching and/or a dispersion engineering for a second order parametric amplification process involving a signal vacuum field and at least one of the optical pulses comprising a first pump pulse.
2 . The circuit of claim 1 , wherein the waveguides each have a width and height of less than 5 micrometers and/or the waveguides have the phase matching and/or the dispersion engineering for nonlinear interactions of the optical pulses having a bandwidth in a range of 0.1-100 Terahertz.
3 . The circuit of claim 2 , wherein:
the circuit comprises at least one an optical parametric oscillator (OPO) comprising one of the waveguides,
and the at least one OPAs and/or the at least one OPO generate the quantum states comprising signal and/or idler pulses in response to the first pump pulse using a second order parametric process, and
the waveguides each have dimensions including the height, the width, and the length minimizing group velocity mismatch (GVM) between the optical pulses comprising pump pulses, comprising the first pump pulse, and signal pulses and/or idler pulses so as to provide temporal overlap of the pump and signal pulses and/or idler pulses, and
the pump pulses, signal pulses, and/or idler pulses each comprise an electromagnetic wave confined in and waveguided by the waveguides.
4 . The circuit of claim 1 , wherein the quantum states comprise Gaussian states comprising one or more squeezed vacuum states having one or more modes.
5 . The circuit of claim 4 , wherein the second order parametric amplification process amplifies the signal vacuum field in a first quadrature and attenuates the signal vacuum field in a second quadrature orthogonal to the first quadrature, thereby generating one or more of the optical pulses comprising one or more signal pulses carrying a first one of the quantum states comprising the one or more a squeezed vacuum states.
6 . The circuit of claim 5 or claim 1 , wherein at least one of an intensity of the first pump pulse, the phase matching, the dispersion engineering, or a length of the optical parametric amplifier are tailored for the second order parametric amplification process comprising non-degenerate parametric amplification so that the signal pulses, carrying the one or more squeezed vacuum states, comprise at least two modes.
7 . The circuit of claim 5 , wherein the circuit further comprises a second OPA having at least one of a second phase matching, a second dispersion engineering, or a second length tailored for an additional second order nonlinear interaction involving the optical pulses comprising a second pump pulse and the signal pulses comprising the first one of the quantum states, wherein the second pump pulse can have a phase difference relative to the first pump pulse and an intensity so that the additional second order nonlinear interaction comprises the parametric amplification in a linear (non-saturated) regime amplifying one of the quadratures of the first one of the quantum states, so as to form a second quantum state in the macroscopic regime, in which the average number of photons for the second quantum state is larger than 10 but less than 10∧9, and thereby enabling a loss-tolerant (de-coherence tolerant) quantum measurement of the first one of the quantum states.
8 . The circuit of claim 1 , wherein the quantum states comprise non-Gaussian states comprising one or more cat states, one or more binomial code states, one or more Gottesnan-Kitaev-Preskill (GKP) states, or one or more photon pair states.
9 . The circuit of claim 1 , wherein the circuit comprises a modulator driven by a driving signal allowing control of a phase or an intensity of the optical pulses comprising one or more pump pulses comprising the first pump pulse or one or more quantum state pulses.
10 . The circuit of claim 1 , wherein:
the circuit comprises the optical parametric amplifier having the phase matching, the dispersion engineering, and length tailored for a second order parametric interaction involving the first pump pulse, having the pulse length, and the signal vacuum field, and
the second order nonlinear interaction comprises a parametric amplification in a saturated regime characterized by the pump energy of the first pump pulse being suppressed by more than 10% through the parametric amplification process, and
so as to form at least one of the optical pulses comprising a signal pulse carrying at least one of the quantum states comprising negativity in its Wigner function.
11 . The circuit of claim 1 , wherein the circuit comprises one or more components for manipulating the one or more quantum states, the one or more components comprising at least one of:
one or more modulators for manipulating an intensity or phase of the quantum states,
one or more couplers for combining a plurality of the quantum states, or
one or more spectral filters, one or more spectral-dependent splitters, one or more polarization rotators, one or more wavelength convertors, or one or more Mach-Zehnder interferometers.
12 . The circuit of claim 1 , wherein the circuit further comprises one or more single-photon detectors, one or more photon number resolving detectors, and/or one or more homodyne detectors configured to at least:
engineer or detect the quantum states, or
enable quantum computing tasks using the quantum states.
13 . The circuit of claim 1 , further comprising:
one or more inputs connected to the waveguides, and
one or more outputs connected to the waveguides, wherein the optical pulses comprise one or more input pulses and one or more output pulses outputted at the outputs in response to the input pulses received at the inputs, and
the waveguides are configured to at least generate, manipulate, or measure one or more of the optical pulses carrying a different one of the quantum states representing a different bit of information according to a time division multiplexing scheme wherein:
the optical pulses are distributed among different equally spaced time bins,
the different equally spaced time bins can be routed to different ones of the waveguides using one or more first modulators and one or more first couplers connected to each other via one or more first delay lines, the one or more first modulators configured to modulate the optical pulses, and
the different equally spaced time bins can be combined using one or more second couplers and one or more second delay lines so that the quantum states in the different time bins can be combined.
14 . The circuit of claim 13 , wherein the pulse lengths are in a range of 1-1000 femtoseconds so that the optical pulses can be routed into the different equally spaced time bins of longer than 1-1000 femtosecond duration and containing the different bits.
15 . The circuit of claim 1 , configured:
as a processor for performing one or more quantum computations on the one or more quantum states, or
as a quantum sensor for performing quantum sensing by a measurement of the one or more quantum states, or
to perform quantum state tomography of the quantum states that is robust against detection losses, or
to perform all-optical continuous-variable quantum error correction with Binomial and squeezed Cat codes using the quantum states, or
to perform quantum teleportation using the quantum states, or
perform boson sampling in time/frequency domain using the quantum states, or
to protect the quantum coherence of the quantum states.
16 . The circuit of claim 1 , wherein the waveguides comprise the optical parametric amplifier having the phase matching and the dispersion engineering such that parametric gain is in a non-linear saturated regime, thereby allowing at least:
all—optical linear or nonlinear quantum measurement of the quantum states, or Gaussian or non-Gaussian operations on the quantum states.
17 . The circuit of claim 1 , further comprising a wavelength converter converting a wavelength of the optical pulses, carrying the quantum states, into a different frequency range.
18 . A method of processing one or more quantum states, comprising:
inputting one or more input optical pulses to one or more waveguides; and
generating, manipulating, or measuring one or more quantum states using one or more of the waveguides comprising a second order non-linearity configured to operate on optical pulses including the input optical pulses, wherein the waveguides each have a width and height of less than 5 micrometers and/or the waveguides have a phase matching and dispersion engineering for the optical pulses having a bandwidth in a range of 0.1-100 Terahertz,
wherein the waveguides comprise at least one optical parametric amplifier (OPA) comprising a phase-matching and/or a dispersion engineering for a second order parametric amplification process involving a signal vacuum field and the optical pulses comprising a first pump pulse.
19 . The method of claim 18 , wherein the generating, manipulating, or measuring is implemented using a time division multiplexing scheme, comprising:
distributing the optical pulses among equally spaced time bins;
routing each of the time bins to different ones of the waveguides using one or more modulators and one or more first couplers connected to each other via one or more first delay lines; and
combining the different time bins using one or more second couplers and one or more second delay lines so that the quantum states in the different time bins are combined; and
wherein the waveguides comprise one or more of the optical parametric amplifiers and/or the waveguides are disposed in one or more optical parametric oscillators comprising one or more of the optical parametric amplifiers.
20 . The method of claim 18 , wherein the generating, manipulating, and/or measuring comprises at least one of:
performing one or more quantum computations on the one or more quantum states, or
quantum sensing by a measurement of the one or more quantum states, or
performing quantum state tomography of the quantum states that is robust against detection losses, or
performing all-optical continuous-variable quantum error correction with Binomial and squeezed Cat codes using the quantum states, or
performing quantum teleportation using the quantum states, or
performing boson sampling in time/frequency domain using the quantum states,
or
protecting a quantum coherence of the quantum states.
21 . The method of claim 18 , wherein at least one of an intensity of the first pump pulse, the phase matching, the dispersion engineering, or a length of the optical parametric amplifier are tailored for the second order parametric amplification process comprising non-degenerate parametric amplification.
22 . The circuit of claim 1 , wherein at least one of an intensity of the first pump pulse, the phase matching, the dispersion engineering, or a length of the optical parametric amplifier are tailored for the second order parametric amplification process comprising non-degenerate parametric amplification.