7 research outputs found
Super-resolution Fluorescence Quenching Microscopy of Graphene
Lately, fluorescence quenching microscopy (FQM) has been introduced as a new tool to visualize graphene-based sheets. Even though quenching of the emission from a dye molecule by fluorescence resonance energy transfer (FRET) to graphene happens on the nanometer scale, the resolution of FQM so far is still limited to several hundreds of nanometers due to the Abbe limit restricting the resolution of conventional light microscopy. In this work, we demonstrate an advancement of FQM by using a super-resolution imaging technique for detecting fluorescence of color centers used in FQM. The technique is similar to stimulated emission depletion microscopy (STED). The combined āFRET+STEDā technique introduced here for the first time represents a substantial improvement to FQM since it exhibits in principle unlimited resolution while still using light in the visible spectral range. In the present case we demonstrate all-optical imaging of graphene with resolution below 30 nm. The performance of the technique in terms of imaging resolution and contrast is well described by a theoretical model taking into account the general distance dependence of the FRET process and the distance distribution of donor centers with respect to the flake. In addition, the change in lifetime for partially quenched emitters allows extracting the quenching distance from experimental data for the first time
Relaxometry and Dephasing Imaging of Superparamagnetic Magnetite Nanoparticles Using a Single Qubit
To study the magnetic dynamics of
superparamagnetic nanoparticles, we use scanning probe relaxometry
and dephasing of the nitrogen vacancy (NV) center in diamond, characterizing
the spin noise of a single 10 nm magnetite particle. Additionally,
we show the anisotropy of the NV sensitivityās dependence on
the applied decoherence measurement method. By comparing the change
in relaxation (<i>T</i><sub>1</sub>) and dephasing (<i>T</i><sub>2</sub>) time in the NV center when scanning a nanoparticle
over it, we are able to extract the nanoparticleās diameter
and distance from the NV center using an OrnsteināUhlenbeck
model for the nanoparticleās fluctuations. This scanning probe
technique can be used in the future to characterize different spin
label substitutes for both medical applications and basic magnetic
nanoparticle behavior
Nanoengineered Diamond Waveguide as a Robust Bright Platform for Nanomagnetometry Using Shallow Nitrogen Vacancy Centers
Photonic structures in diamond are
key to most of its application in quantum technology. Here, we demonstrate
tapered nanowaveguides structured directly onto the diamond substrate
hosting shallow-implanted nitrogen vacancy (NV) centers. By optimization
based on simulations and precise experimental control of the geometry
of these pillar-shaped nanowaveguides, we achieve a net photon flux
up to ā¼1.7 Ć 10<sup>6</sup> s<sup>ā1</sup>. This
presents the brightest monolithic bulk diamond structure based on
single NV centers so far. We observe no impact on excited state lifetime
and electronic spin dephasing time (<i>T</i><sub>2</sub>) due to the nanofabrication process. Possessing such high brightness
with low background in addition to preserved spin quality, this geometry
can improve the current nanomagnetometry sensitivity ā¼5 times.
In addition, it facilitates a wide range of diamond defects-based
magnetometry applications. As a demonstration, we measure the temperature
dependency of <i>T</i><sub>1</sub> relaxation time of a
single shallow NV center electronic spin. We observe the two-phonon
Raman process to be negligible in comparison to the dominant two-phonon
Orbach process
Toward Optimized Surface Ī“āProfiles of Nitrogen-Vacancy Centers Activated by Helium Irradiation in Diamond
The negatively charged nitrogen-vacancy
(NV) center in diamond has been shown recently as an excellent sensor
for external spins. Nevertheless, their optimum engineering in the
near-surface region still requires quantitative knowledge in regard
to their activation by vacancy capture during thermal annealing. To
this aim, we report on the depth profiles of near-surface helium-induced
NV centers (and related helium defects) by step-etching with nanometer
resolution. This provides insights into the efficiency of vacancy
diffusion and recombination paths concurrent to the formation of NV
centers. It was found that the range of efficient formation of NV
centers is limited only to approximately 10 to 15 nm (radius) around
the initial ion track of irradiating helium atoms. Using this information
we demonstrate the fabrication of nanometric-thin (Ī“) profiles
of NV centers for sensing external spins at the diamond surface based
on a three-step approach, which comprises (i) nitrogen-doped epitaxial
CVD diamond overgrowth, (ii) activation of NV centers by low-energy
helium irradiation and thermal annealing, and (iii) controlled layer
thinning by low-damage plasma etching. Spin coherence times (Hahn
echo) ranging up to 50 Ī¼s are demonstrated at depths of less
than 5 nm in material with 1.1% of <sup>13</sup>C (depth estimated
by spin relaxation (T<sub>1</sub>) measurements). At the end, the
limits of the helium irradiation technique at high ion fluences are
also experimentally investigated
Photoinduced Modification of Single-Photon Emitters in Hexagonal Boron Nitride
Fluorescent defects
recently observed under ambient conditions
in hexagonal boron nitride (h-BN) promise to open novel opportunities
for the implementation of on-chip photonic devices that rely on identical
photons from single emitters. Here we report on the room-temperature
photoluminescence dynamics of individual emitters in multilayer h-BN
flakes exposed to blue laser light. Comparison of optical spectra
recorded at successive times reveals considerable spectral diffusion,
possibly the result of slowly fluctuating, trapped-carrier-induced
Stark shifts. Large spectral jumpsīøreaching up to 100 nmīøfollowed
by bleaching are observed in most cases upon prolonged exposure to
blue light, an indication of one-directional photochemical changes
possibly taking place on the flake surface. Remarkably, only a fraction
of the observed emitters also fluoresce on green illumination, suggesting
a more complex optical excitation dynamics than previously anticipated
and raising questions on the physical nature of the crystal defect
at play
Addressing Single Nitrogen-Vacancy Centers in Diamond with Transparent in-Plane Gate Structures
For many applications of the nitrogen-vacancy
(NV) center in diamond,
the understanding and active control of its charge state is highly
desired. In this work, we demonstrate the reversible manipulation
of the charge state of a single NV center from NV<sup>ā</sup> across NV<sup>0</sup> to a nonfluorescent, dark state by using an
all-diamond in-plane gate nanostructure. Applying a voltage to the
in-plane gate structure can influence the energy band bending sufficiently
for charge state conversion of NV centers. These diamond in-plane
structures can function as transparent top gates, enabling the distant
control of the charge state of NV centers tens of micrometers away from the nanostructure
Protecting a Diamond Quantum Memory by Charge State Control
In
recent years, solid-state spin systems have emerged as promising
candidates for quantum information processing. Prominent examples
are the nitrogen-vacancy (NV) center in diamond, phosphorus dopants
in silicon (Si:P), rare-earth ions in solids, and V<sub>Si</sub>-centers
in silicon-carbide. The Si:P system has demonstrated that its nuclear
spins can yield exceedingly long spin coherence times by eliminating
the electron spin of the dopant. For NV centers, however, a proper
charge state for storage of nuclear spin qubit coherence has not been
identified yet. Here, we identify and characterize the positively
charged NV center as an electron-spin-less and optically inactive
state by utilizing the nuclear spin qubit as a probe. We control the
electronic charge and spin utilizing nanometer scale gate electrodes.
We achieve a lengthening of the nuclear spin coherence times by a
factor of 4. Surprisingly, the new charge state allows switching of
the optical response of single nodes facilitating full individual
addressability