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2 article(s) from Wrachtrup, Jörg

Active and fast charge-state switching of single NV centres in diamond by in-plane Al-Schottky junctions

Christoph Schreyvogel,
Vladimir Polyakov,
Sina Burk,
Helmut Fedder,
Andrej Denisenko,
Felipe Fávaro de Oliveira,
Ralf Wunderlich,
Jan Meijer,
Verena Zuerbig,
Jörg Wrachtrup and
Christoph E. Nebel

Beilstein J. Nanotechnol. 2016, 7, 1727–1735, doi:10.3762/bjnano.7.165

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Figure 1: Formation and quenching of NV centres. (a) PL-intensity mapping performed on the diamond surface wh...

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Figure 2: In-plane Schottky diode from diamond. (a) Schematic figure of an in-plane Al Schottky diode on an H...

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Figure 3: Active charge state control of a single NV centre. At zero bias there is only a PL-background of th...

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Figure 4: Schematic setup for time-resolved measurement of NV-intensity. To record the time evolution of the ...

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Figure 5: Fast charge state switching. The result of the time-resolved NV-intensity measurement shows that sw...

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Figure 6: Time constant for charge state switching. Time constants deduced from fitting an exponential functi...

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Figure 7: Degradation effect. After several 1000 switching cycles, the measured time constants for dischargin...

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Figure 8: Simultaneous measurement of NV⁻ and NV⁰ intensity. A time-resolved measurement of NV⁻ (red curve) a...

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Letter

Published 16 Nov 2016

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Diamond nanophotonics

Katja Beha,
Helmut Fedder,
Marco Wolfer,
Merle C. Becker,
Petr Siyushev,
Mohammad Jamali,
Anton Batalov,
Christopher Hinz,
Jakob Hees,
Lutz Kirste,
Harald Obloh,
Etienne Gheeraert,
Boris Naydenov,
Ingmar Jakobi,
Florian Dolde,
Sébastien Pezzagna,
Daniel Twittchen,
Matthew Markham,
Daniel Dregely,
Harald Giessen,
Jan Meijer,
Fedor Jelezko,
Christoph E. Nebel,
Rudolf Bratschitsch,
Alfred Leitenstorfer and
Jörg Wrachtrup

Beilstein J. Nanotechnol. 2012, 3, 895–908, doi:10.3762/bjnano.3.100

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Figure 1: (a) Scanning electron micrograph of a mica mask. High aspect ratio channels were created by bombard...

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Figure 2: Nonlinear optical microscopy of implanted color centers by using ground-state-depletion microscopy ...

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Figure 3: Fluorescence spectra of the nitrogen–vacancy defect in diamond. The upper curve shows the spectrum ...

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Figure 4: Plasmonic resonator geometries, field I and current q for (a) half-wave antenna, (b) bow tie and cr...

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Figure 5: Enhancement of the collection efficiency with a hemispherical solid immersion lens (SIL). (a) Reduc...

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Figure 6: Macroscopic solid immersion lens [10]. (a) Photograph of a single crystalline diamond hemisphere. (b) C...

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Figure 7: Fabrication of a microscopic diamond hemisphere by focused ion beam milling. (a) Grid of FIB marker...

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Figure 8: (a) Scanning electron microscopy (SEM) image of a micropillar resonator with embedded diamond nanoc...

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Figure 9: (a) Normalized intensity autocorrelation function g⁽²⁾(τ) from a micropillar cavity of 1.6 µm diame...

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Figure 10: View into the MWPECVD reactor during growth of a single-crystalline diamond layer.

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Figure 11: (a) Optical emission spectroscopy: observed nickel emission in the MWPECVD plasma during diamond gr...

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Figure 12: (a) SIMS depth profile of nickel-doped single-crystal diamond layer. The intensity of the two “mark...

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Figure 13: Cathodoluminescence spectra measured at a temperature of 5 K on a nickel-doped single-crystal diamo...

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Figure 14: (a–c) Room-temperature PL mapping excited at a wavelength of 660 nm on (111) diamond layers grown b...

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Figure 15: (a) As-grown nanodiamond particles on a silicon substrate. (b) Confocal photoluminescence mapping (...

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Video

Full Research Paper

Published 21 Dec 2012

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