Coherent Ising machines are a type of optical accelerators that can solve different optimization tasks by encoding the problem in the connection matrix of the network. So far, experimental realizations have been limited to time multiplexed solutions, in which one nonlinear node is present in a feedback loop. In Hewlett Packard Labs, we investigate the implementation of a spatially multiplexed solution, with an array of nominally identical nonlinear nodes. As this avoids the need for a long delayline, this makes the system more suitable for integration and hence mass production. HPE investigated two material platforms with good bulk nonlinearity properties: a-Si and GaAs. For the CMOS compatible a-Si platform, HPE demonstrated a design approach that allows to fabricate 1000 component all-optical computational circuits in a scalable way. In addition, to be able to do layout of Ising machines with ~1000 components, HPE developed highly capable photonic layout that will help across interconnects, sensors, and computation. In the GaAs platform, we focused on reducing the energy per elementary operation down to 1 fJ. The optical gates are designed with a bus-waveguide connectivity using a multi-level layered architecture design that allows waveguide connectivity between optical gates. This allows to separate computation and communication into their own dedicated layers increasing overall performance. Finally, we will highlight how both drastic automation at the layout stage and a tight integration between the electronic control layer (used for tuning of resonances and phase-shifters) and the photonic layer are key to achieve actual scalability to larger circuits.
A key enabler of the IT revolution of the late 20th century was the development of electronic design automation (EDA) tools allowing engineers to manage the complexity of electronic circuits with transistor counts now reaching into the billions. Recently, we have been developing large-scale nonlinear photonic integrated logic circuits for next generation all-optical information processing. At this time a sufficiently powerful EDA-style software tool chain to design this type of complex circuits does not yet exist. Here we describe a hierarchical approach to automating the design and validation of photonic integrated circuits, which can scale to several orders of magnitude higher complexity than the state of the art.
Most photonic integrated circuits developed today consist of a small number of components, and only limited hierarchy.
For example, a simple photonic transceiver may contain on the order of 10 building-block components,
consisting of grating couplers for photonic I/O, modulators, and signal splitters/combiners. Because this is relatively
easy to lay out by hand (or simple script) existing photonic design tools have relatively little automation in
comparison to electronics tools. But demonstrating all-optical logic will require significantly more complex photonic
circuits containing up to 1,000 components, hence becoming infeasible to design manually.
Our design framework is based off Python-based software from Luceda Photonics which provides an environment to describe components, simulate their behavior, and export design files (GDS) to foundries for fabrication. At a fundamental level, a photonic component is described as a parametric cell (PCell) similarly to electronics design. PCells are described by geometric characteristics of their layout. A critical part of the design framework is the implementation of PCells as Python objects. PCell objects can then use inheritance to simplify design, and hierarchical designs can be made by creating composite PCells (modules) which consist of primitive building-block PCells (components). To automatically produce layouts, we built on a construct provided by Luceda called a PlaceAndAutoRoute cell: we create a module component by supplying a list of child cells, and a list of the desired connections between the cells (e.g. the out0 port of a microring is connected to a grating coupler). This functionality allowed us to write algorithms to automatically lay out the components: for instance, by laying out the first component and walking through the list of connections to check to see if the next component is already placed or not. The placement and orientation of the new component is determined by minimizing the length of a connecting waveguide. Our photonic circuits also utilize electrical signals to tune the photonic elements (setting propagation phases or microring resonant frequencies via thermo-optical tuning): the algorithm also routes the contacts for the metal heaters to contact pads at the edge of the circuit being designed where it can be contacted by electrical probes.
We are currently validating a test run fabricated over the summer, and will use detailed characterization results to prepare our final design cycle in which we aim to demonstrate complex operational logic circuits containing ~50-100 nonlinear resonators.
The negatively-charged nitrogen-vacancy centers in diamond has motivated many groups building scalable quantum information processors based on diamond photonics. This is owning to the long-lived electronic spin coherence and the capability for spin manipulation and readout of NV centers.1-4 The primitive operation is to create entanglement between two NV centers, based on schemes such as 'atom-photon entanglement' proposed by Cabrillo et al.5To scale this type of scheme beyond two qubits, one important component is an optical switch that allows light emitted from a particular device to be routed to multiple locations. With such a switch, one has choices of routing photons to specified paths and has the benefit of improving the entanglement speed by entangling multiple qubits at the same time. Yield of the existing diamond cavities coupled with NV centers are inevitably low, due to the nature of randomness for NV placement and orientation, variation of spectral stability, and variation of cavity resonance frequency and quality factor. An optical switch provides the capability to tolerate a large fraction of defective devices by routing only to the working devices. Many type of switching devices were built on conventional semiconductor materials with mechanisms from mechanical, thermal switching to carrier injection, photonics crystal, and polymer refractive index tuning .6-8 In this paper, we build an optical-thermal switch on diamond with micro-ring waveguides, mainly for the simplicity of the diamond fabrication. The the switching function was realized by locally tuning the temperature of the diamond waveguides. Switching efficiency of 31% at 'drop' port and 73% at 'through' port were obtained.
We demonstrate coupling between the zero phonon line (ZPL) of nitrogen-vacancy centers in diamond and the
modes of optical micro-resonators fabricated in single crystal diamond membranes sitting on a silicon dioxide
substrate. A more than ten-fold enhancement of the ZPL is estimated by measuring the modification of the
spontaneous emission lifetime. The cavity-coupled ZPL emission was further coupled into on-chip waveguides
thus demonstrating the potential to build optical quantum networks in this diamond on insulator platform.
Nitrogen-vacancy centers in diamond are widely studied both as a testbed for solid state quantum optics and for
their applications in quantum information processing and magnetometry. Here we demonstrate coupling of the
nitrogen-vacancy centers to gap plasmons in metal nano-slits. We use diamond samples where nitrogen-vacancy
centers are implanted tens of nanometers under the surface. Silver nano-slits are patterned on the sample such
that diamond ridges tens of nanometers wide fill the slit gap. We measure enhancement of the spontaneous
emission rate of the zero photon line by a factor of 3 at a temperature of 8K.
The combination of the long electron state spin coherence time and the optical coupling of the ground electronic
states to an excited state manifold makes the nitrogen-vacancy (NV) center in diamond an attractive candidate
for quantum information processing. To date the best spin and optical properties have been found in centers
deep within the diamond crystal. For useful devices it will be necessary to engineer NVs with similar properties
close to the diamond surface. We report on properties including charge state control and preferential orientation
for near surface NVs formed either in CVD growth or through implantation and annealing.
We present DWDM nanophotonics architectures based on microring resonator modulators and detectors. We
focus on two implementations: an on chip interconnect for multicore processor (Corona) and a high radix network
switch (HyperX). Based on the requirements of these applications we discuss the key constraints on the photonic
circuits' devices and fabrication techniques as well as strategies to improve their performance.
The understanding of the coherence properties of photons emitted from negatively charged nitrogen-vacancy (NV)
centers in diamond is essential for the success of quantum information applications based on indistinguishable
photons. Here we study both the polarization of photons emitted from and the linewidth of photons absorbed by
single NV centers as a function of temperature T. We find that for T < 100 K the main dephasing mechanism
contributing to the linewidth broadening is phonon-mediated population transfer between the two excited orbital
states. The observed T5 temperature dependence of the population transfer rate and linewidth is experimental
evidence of a dynamic Jahn-Teller effect in the excited states.
We describe research on new optical structures in diamond for quantum information and sensing applications
based on the nitrogen-vacancy (NV) center. Results include etching experiments that reveal the vertical distribution
of NV centers produced by ion implantation and annealing, and gallium phosphide waveguides fabricated
on diamond with evanescent coupling to NV centers close to the diamond surface.
Spatial and k-space properties of subwavelength cross-section GaP waveguides supported by a diamond substrate are
analyzed theoretically. These waveguides are suitable for optically coupling to nitrogen vacancy centers located near the
surface of a single crystal diamond sample.
We observe the coupling of nitrogen-vacancy centers in single-crystal diamond to GaP waveguides on the diamond
surface. We describe the fabrication procedure and characterize the waveguide performance. Our results
indicate that the GaP/diamond hybrid system is a promising system for coupling nitrogen-vacancies to optical
microstructures for quantum information processing and sensing applications.
Scalable quantum information processing using nitrogen-vacancy (NV) centers in diamond will be difficult without
the ability to couple the centers to optical microcavities and waveguides. Here we present our preliminary
result of coupling a single NV center in a nanoparticle to a silica microdisk at cryogenic temperatures. The
cavity-coupled NV photoluminescence is coupled out of the cavity through a tapered fiber. Although the current
system is limited by the spectral properties of the NV center and the Q of the cavity, efficient particle-cavity
and cavity-waveguide coupling should lead to the realization of a "one-dimensional atom" as needed for CQED,
enable single-shot electron-spin readout, and increase the probability of success in entanglement schemes based
on single-photon detection.
General requirements for single-photon devices in various applications are presented and compared with experimental
progress to date. The quantum information applications that currently appear the most promising require
a matter qubit-enabled single-photon source, where the emitted photon state is linked to the state of a long-lived
quantum system such as an electron spin. The nitrogen-vacancy center in diamond is a promising solid-state
system for realizing such a device due to its long-lived electron spin coherence, optical addressability, and ability
to couple to a manageable number of nuclear spins. This system is discussed in detail, and experimental results
from our laboratory are shown. A critical component of such a device is an optical microcavity to enhance the
coupling between the nitrogen-vacancy center and a single photon, and we discuss theoretically the requirements
for achieving this enhancement.
Nitrogen-vacancy centers in diamond typically have spin-conserving optical transitions, a feature which allows
for optical detection of the long-lived electronic spin states through fluorescence detection. However, by applying
stress to a sample it is possible to obtain spin-nonconserving transitions in which a single excited state couples to
multiple ground states. Here we describe two-frequency optical spectroscopy on single nitrogen-vacancy centers
in a high-purity diamond sample at low temperature. When stress is applied to the sample it is possible to
observe coherent population trapping with a single center. By adjusting the stress it is possible to obtain a
situation in which all of the transitions from the three ground sublevels to a common excited state are strongly
allowed. These results show that all-optical spin manipulation is possible for this system, and we propose that
that by coupling single centers to optical microcavities, a scalable quantum network could be realized for photonic
quantum information processing.
A new route to grow single crystal semiconductor nanostructures was proposed and demonstrated on non-single crystal substrates. Hydrogenated silicon surfaces, amorphous silicon and microcrystalline silicon, were used to provide atomic short-range order required for epitaxial growth of nanostructures. Indium phosphide was chosen as a platform for semiconductor nanostructures. Indium phosphide was deposited on the hydrogenated silicon surfaces by low-pressure metalorganic chemical vapor deposition with a presence of colloidal gold nanoparticles. Under specific metal organic chemical vapor deposition growth conditions, the indium phosphide was found to grow into nanoneedles. Structural analysis reveals that the nanoneedles are single crystal and have either face-centered-cubic or hexagonal-closed-pack lattice when grown onto the hydrogenated microcrystalline silicon surfaces. Micro-photoluminescence measurements shows that the emission peak wavelength of an ensemble of the InP nanoneedles both on the hydrogenated amorphous silicon and hydrogenated microcrystalline silicon surfaces have a substantial blue-shift with respect to that of bulk indium phosphide. The unique shape of the emission spectra is attributed to different types of nanoneedles co-existing on the samples. The proposed route to grow semiconductor nanostructures on non-single crystal substrates would open new applications including photovoltaic, photo-detection, photo-emission and thermal energy-conversion, for which the usage of costly single crystal substrates is not preferred.
Moore's Law has set great expectations that the performance/price ratio of commercially available semiconductor
devices will continue to improve exponentially at least until the end of the next decade. Although the physics
of nanoscale silicon transistors alone would allow these expectations to be met, the physics of the metal wires
that connect these transistors will soon place stringent limits on the performance of integrated circuits. We
will describe a Si-compatible global interconnect architecture - based on chip-scale optical wavelength division
multiplexing - that could precipitate an "optical Moore's Law" and allow exponential performance gains until
the transistors themselves become the bottleneck. Based on similar fabrication techniques and technologies, we
will also present an approach to an optically-coupled quantum information processor for computation beyond
Moore's Law, encouraging the development of practical applications of quantum information technology for
commercial utilization. We present recent results demonstrating coherent population trapping in single N-V
diamond color centers as an important first step in this direction.
We report on two experiments implementing quantum communications primitives in linear optics systems: a
secure Quantum Random Bit Generator (QRBG) and a multi-qubit gate based on Two-Photon Multiple-Qubit
(TPMQ) quantum logic. In the first we use photons to generate random numbers and introduce and implement
a physics-based estimation of the sequence randomness as opposed to the commonly used statistical tests. This
scheme allows one to detect and neutralize attempts to eavesdrop or influence the random number sequence. We
also demonstrate a C-SWAP gate that can be used to implement quantum signature and fingerprinting protocols.
A source of momentum-entangled photons, remote state preparation, and a C-SWAP gate are the ingredients
used for this proof-of-principle experiment. While this implementation cannot be used in field applications due to the limitations of TPMQ logic, it provides useful insights into this protocol.
We describe how a quantum non-demolition device based on electromagnetically-induced transparency in solidstate atom-like systems could be realized. Such a resource, requiring only weak optical nonlinearities, could potentially enable photonic quantum information processing (QIP) that is much more efficient than QIP based on linear optics alone. As an example, we show how a parity gate could be constructed. A particularly interesting physical system for constructing devices is the nitrogen-vacancy defect in diamond, but the excited-state structure for this system is unclear in the existing literature. We include some of our latest spectroscopic results that indicate that the optical transitions are generally not spin-preserving, even at zero magnetic field, which allows the realization of a Λ-type system.
Single-photon sources rarely emit two or more photons in the same
pulse, compared to a Poisson-distributed source of the same
intensity, and have numerous applications in quantum information
science. The quality of such a source is evaluated based on three
criteria: high efficiency, small multi-photon probability, and
quantum indistinguishability. We have demonstrated a single-photon
source based on a quantum dot in a micropost microcavity that
exhibits a large Purcell factor together with a small multi-photon
probability. For a quantum dot on resonance with the cavity, the
spontaneous emission rate has been increased by a factor of five,
while the probability to emit two or more photons in the same
pulse has been reduced to 2% compared to a Poisson-distributed
source of the same intensity. The indistinguishability of emitted
single photons from one of our devices has been tested through a
Hong-Ou-Mandel-type two-photon interference experiment;
consecutive photons emitted from such a source have been largely
indistinguishable, with a mean wave-packet overlap as large as
0.81. We have also designed and demonstrated two-dimensional
photonic crystal GaAs cavities containing InAs quantum dots that
exhibit much higher quality factors together with much smaller
mode volumes than microposts, and therefore present an ideal
platform for construction of single photon sources of even higher
quality.
Quantum cryptography is a method to exchange secret messages with unconditional security over a potentially hostile environment using single photons. Previous implementations of quantum cryptography have relied on highly attenuated laser light to approximate single photo states. Such sources are vulnerable to eavesdropping attacks based on photon splitting. Here we present an experimental demonstration of quantum cryptography using a single photon source based on Indium Arsenide quantum dots. We achieve a communication rate of 25kbits/s. This source allows secure communication over a quantum channel with up to 28dB of channel loss, as opposed to only 23dB for an attenuated laser.
A high efficiency, triggered single photon source with applications to quantum communications is discussed. The sources is formed from an InAs-based quantum dot located in the center of a micropost cavity formed from GaAs, with top and bottom GaAs/AlAs distributive Bragg reflector pairs, and lateral processing. When pumped above band into the semiconductor host, correlation measurements show a reduction in the two-photon probability to 0.14, compared to unity for a Poisson source. The external efficiency of this structure is 0.24.
A single-photon device based on a semiconductor quantum dot
embedded in an optical microcavity is described. The spontaneous
emission lifetime, multi-photon suppression, and spectral linewidth
are measured. It is then shown that consecutively emitted photons possess a large degree of quantum-mechanical indistinguishability, with a mean wave-packet overlap as large as 0.8. This demonstration is accomplished through a Hong-Ou-Mandel-type two-photon interference experiment.
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