integration with FABRIC testbeds and demonstrations
GS&PD (K)
state vector and tableax convertors/simulators
GS (K)
Gaussian QIS backend
GS (K)
tensor networks backend
GS&PD (K)
noise processes zoo
GS&PD (K)
base discrete event simulator
GS&PD (K)
noise zoo online portal
(K)
protocols zoo
PD (K&T)
stochastic AD for network sim
PD (K&T)
protocols online portal
(K)
interactive docs, embedded web sims
(K)
continuous surrogates for network dynamics
PD (T)
surrogates for quantum hardware
PD (K)
protocol and hardware optimization studies
GS&PD (K&T)
F_purcell
Purcell factor, i.e., the increase in decay to the ZPL thanks to the resonant cavity.
It should be easy to achieve
ξ_debye_waller
Debye-Waller factor, i.e., the fraction of radiative decays that fall in the zero phonon line without a cavity. In other words, how many of the emitted photons leave without interference from phonons.
It should be easy to achieve
ξ_quantum_efficiency
Also called "internal quantum efficiency". The ratio of radiative to total decay (including non-radiative decay, e.g., due to "shelf states").
It should be easy to achieve
ξ_optical_branching
There might be a number of close-together optical transitions for the given emitter. This gives us the fraction we care about.
It should be easy to achieve
η_blinking
Drop in efficiency due to the emitter blinking out of existence.
It should be easy to achieve
Dark Counts
It should be easy to achieve
η_binning
Drop in efficiency due to the finite time-binning while waiting for light to come from the emitter.
It should be easy to achieve
fdc_pump_leak
Frequency of dark counts due to leaks from the pump.
It should be easy to achieve
fdc_freespace_detector
Frequency of dark counts inherent to an off-chip detector.
It should be easy to achieve
fdc_snspd_detector
Frequency of dark counts inherent to an on-chip SNSPD.
It should be easy to achieve
Photonic switch
It should be easy to achieve
η_switch_per_depth
It should be easy to achieve
Diamond to photonic switch
It should be easy to achieve
η_free_space_e2s
The losses in the imagin system and coupling to free space.
It should be easy to achieve
η_chiplet_e2s
It should be easy to achieve
Photonic switch to detectors
It should be easy to achieve
η_free_space_s2d
It should be easy to achieve
η_fiber_s2d
It should be easy to achieve
η_onchip_SNSPD
The inefficiences in the nanowire detectors.
It should be easy to achieve
On chip emitter coupling OLD
It should be easy to achieve
η_1x4_switch
The losses due to routing in the chip.
It should be easy to achieve
η_chiplet
The losses due to couplings between the diamond chiplet and the mainboard.
It should be easy to achieve
η_SNSPDs
The inefficiences in the nanowire detectors.
It should be easy to achieve
Free space emitter coupling OLD
It should be easy to achieve
η_1x8_MZI_Tree
The losses due to routing in the chip.
It should be easy to achieve
η_imaging
The losses in the imagin system and coupling to free space.
It should be easy to achieve
η_detectors
The inefficiencies in the detector.
It should be easy to achieve
Indistinguishability of photons
It should be easy to achieve
Δλ_rel_sys
The expected systematic error in the optical resonance tuning (e.g., when strain tuning).
It should be easy to achieve
Δλ_rel_rand
The spectral diffusion of the emitters, i.e., the uncontrollable movements of the resonance due to the environment.
It should be easy to achieve
Γ_emitter
Intrinsic linewidth of a single emitter.
It should be easy to achieve
Excitation Control
It should be easy to achieve
f_reconfig
Speed at which spots can be turned on or off.
It should be easy to achieve
r_extinction
How dark are spots that are supposed to be dark. If not perfect, it can lead to spurious excitations.
It should be easy to achieve
MW Control of Emitters
It should be easy to achieve
T1e
T1 time of the electron spin achieved after cooling (and dynamical decoupling).
It should be easy to achieve
T2e
T2 time of the electron spin achieved after dynamical decoupling.
It should be easy to achieve
T1n
T1 time of the nuclear spin achieved.
It should be easy to achieve
T2n
T2 time of the nuclear spin achieved after dynamical decoupling.
It should be easy to achieve
Tcphase
Time for a CPHASE gate between e and n spins.
It should be easy to achieve
Tegate
Time for a single qubit gate on the electron spin.
It should be easy to achieve
Tngate
Time for a single qubit gate on the nuclear spin.
It should be easy to achieve
ε_init_e
Electron spin initialization error.
It should be easy to achieve
ε_init_n
Nuclear spin initialization error.
It should be easy to achieve
Scalability
It should be easy to achieve
N_strain_control
The number of color centers we can reliably strain tune.
It should be easy to achieve
N_em_control
The number of color centers we can reliably address with RF EM fields.
It should be easy to achieve
N_excitation_control
Number of different target spots that can be controlled at the same time.
It should be easy to achieve
To be derived
It should be easy to achieve
Tmeas
Time to measure the electron spin, depends on the optical lifetime.
It should be easy to achieve
p_cphase
Fidelity of gate, depends on ground manifold lifetime and gate duration.
It should be easy to achieve
p_egate
Fidelity of gate, depends on ground manifold lifetime and gate duration.
It should be easy to achieve
p_ngate
Fidelity of gate, depends on ground manifold lifetime and gate duration.
It should be easy to achieve
p_meas
Infidelity of measurement results, mostly due to dark counts.
It should be easy to achieve
Tbk
Time for one BK attempt (exciting both spins, waiting for their decay, looking for the photon leak)
It should be easy to achieve
Neglected
It should be easy to achieve
RF crosstalk
It should be easy to achieve
RF heating
It should be easy to achieve
Log of expected and attained performance parameters