Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Discover Nano

Single tin-vacancy center in nanoscale diamond

Masanori Fujiwara, Masanao Ohori, Frederick T.-K. So, Yuto Makino, Naoya Morioka, Izuru Ohki, Ryuji Igarashi, Masahiro Nishikawa, Norikazu Mizuochi

Published May 14, 2025• 8 citations
Publisher

Abstract

Group-IV color centers in diamonds are promising not only as spin-photon interfaces for quantum networks but also as multicolor photoluminescence probes and all-optical temperature sensors for biological research. Therefore, generating group-IV color centers in detonation nanodiamonds (DNDs), the smallest class of diamond nanocrystals, has become a research focal point. This approach holds potential for the noninvasive introduction of diamond sensors into living cell organelles, enabling sensing of local structural and temperature changes with minimal disturbance. Following the successful generation of silicon- and germanium-vacancy centers in DNDs, the generation of tin-vacancy (SnV) centers was investigated. Similar to other group-IV color centers, the SnV centers exhibit strong photoluminescence. In addition, the SnV center offers a long spin coherence time compared with those of silicon- and germanium-vacancy centers. However, the strain induced by large Sn atoms poses substantial challenges for generating SnV centers in ultrasmall nanodiamonds. In this study, Sn-doped DNDs with a mean particle size of ~ 5 nm were subjected to a 3 days boiling acid treatment, which led to sharp zero-phonon lines of SnV centers at ~ 620 nm in the photoluminescence spectra. Photon autocorrelation measurements further revealed the presence of single SnV centers in these DNDs.

DOI
10.1186/s11671-025-04256-0

Related papers

Creation of Single Tin-Vacancy Color Centers in Small Nanodiamonds

Hideaki Takashima, Konosuke Shimazaki, Hiroshi Abe +2 more

Nanodiamonds containing single tin-vacancy (SnV) centers have the potential for integration into nanophotonic devices employed in quantum technologies such as quantum sensing, quantum information processing and quantum communication. The present study assessed single SnV centers in nanodiamonds less than 10 nm in size. Such centers were generated by implanting Sn ions into size-selected small nanodiamonds followed by high-temperature annealing. A sharp emission peak with a line width of 2.6 nm was observed at 618.7 nm, corresponding to the zero phonon line of SnV centers in bulk diamond. The Debye–Waller factor for this peak at room temperature was estimated to be 0.38 and so was slightly greater than the value for bulk diamond. A second-order correlation function yielded a g 2 (0) value of 0.04 ± 0.11, indicating single-photon emission. The successful creation of single SnV centers in nanodiamonds is a critical step toward integrating nanophotonic devices for photonic quantum technologies.

ACS Photonics•Aug 13, 2025•4 citations

Tin-Vacancy Centers in Diamond for Quantum Network

Takayuki Iwasaki

Quantum emitters in diamond are a promising candidate for quantum network applications. Here, we show basic properties of tin-vacancy (SnV) centers in diamond, which we recently discovered. The SnV center shows a sharp zero phonon line and a high fluorescence intensity. The SnV center has a possibility to have a long spin coherence time in the Kelvin temperature range, in contrast to other group-IV color centers, i.e. silicon-vacancy and germanium-vacancy centers. We discuss important experiments regarding spin and optical properties of the SnV quantum emitter for further development towards quantum network.

The Review of Laser Engineering•Jan 1, 2021•0 citations

Fabrication and Photoluminescence Studies of Tin-Vacancy Centers in Chemical Vapor Deposition Diamond

Rani Mary Joy, Miquel Cherta Garrido, Omar J. Y. Harb +8 more

Group IV color centers in diamond are promising single-photon emitters for quantum information processing and networking. Among them, the tin-vacancy (SnV) center stands out due to its long spin coherence times at cryogenic temperatures above 1 K. While SnV centers have been realized using various fabrication routes, their in situ formation via microwave plasma-enhanced chemical vapor deposition (MW PE CVD) remains relatively unexplored. In this study, SnV centers, identified by a zero-phonon line (ZPL) near 620 nm, were synthesized in nanocrystalline diamond and free-standing microcrystalline diamond using tin oxide (SnO 2 ) as a dopant source at substrate temperatures of 750°C and 850°C. Photoluminescence measurements reveal that lowering the substrate temperature enhances both the ZPL intensity and spatial uniformity of SnV centers. These results highlight substrate temperature as a key parameter for controlling SnV incorporation during MW PE CVD growth and provide insights into optimizing fabrication strategies for diamond-based quantum technologies.

ACS Materials Letters•Dec 2, 2025•1 citation

Single Silicon Vacancy Centers in 10 nm Diamonds for Quantum Information Applications

Stepan V. Bolshedvorskii, Anton I. Zeleneev, Vadim V. Vorobyov +13 more

Ultrasmall (about 10 nm), low-strain, artificially produced diamonds with an internal, active color center have substantial potential for quantum information processing and biomedical applications. Thus, it is of great importance to be able to artificially produce such diamonds. Here, we report on the high-pressure, high-temperature synthesis of such nanodiamonds about 10 nm in size and containing an optically active, single silicon-vacancy color center. Using special sample preparation technique, we were able to prepare samples containing single nanodiamonds on the surface. By correlating atomic-force microscope images and confocal optical images, we verified the presence of optically active color centers in single nanocrystals, and using second-order correlation measurements, we proved the single-photon emission statistics of these nanodiamonds. These color centers have nonblinking, spectrally narrow emission with narrow distribution of spectral width and positions of zero-phonon line, thus proving the high quality of the nanodiamonds produced.

arXiv:1812.06534•ACS Applied Nano Materials•Jul 8, 2019•36 citations

Narrowband photoluminescence of Tin-Vacancy colour centres in Sn-doped chemical vapour deposition diamond microcrystals

Vadim Sedov, Мартьянов Артём Константинович, Arthur Yu. Neliubov +8 more

Tin-Vacancy (Sn-V) colour centres in diamond have a spin coherence time in the millisecond range at temperatures of 2 K, so they are promising to be used in diamond-based quantum optical devices. However, the incorporation of large Sn atoms into a dense diamond lattice is a non-trivial problem. The objective of our work is to use microwave plasma-assisted chemical vapour deposition (CVD) to grow Sn-doped diamond with submicron SnO 2 particles as a solid-state source of impurity. Well-faceted diamond microcrystals with sizes of a few micrometres were formed on AlN substrates. The photoluminescence (PL) signal with zero-phonon line (ZPL) peak for Sn-V centre at ≈620 nm was measured at room temperature (RT) and at 7 K. The peak width (full width at half-maximum) was measured to be 1.1–1.7 nm at RT and ≈0.05 nm at 7 K. The observed variations of ZPL shape and position, in particular, narrowing of PL peak at RT and formation of single-line fine structure at low- T , are attributed to strain in the crystallites. The diamond doping with Sn via CVD process offers a new route to from Sn-V colour centre in the bulk of the diamond crystallites. This article is part of the Theo Murphy meeting issue 'Diamond for quantum applications'.

Philosophical Transactions of the Royal Society A Mathematical Physical and Engineering Sciences•Dec 3, 2023•12 citations

Tin-Vacancy Quantum Emitters in Diamond

Takayuki Iwasaki, Yoshiyuki Miyamoto, Takashi Taniguchi +4 more

Tin-vacancy ($\mathrm{Sn}\text{\ensuremath{-}}V$) color centers were created in diamond via ion implantation and subsequent high-temperature annealing up to $2100\text{ }\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$ at 7.7 GPa. The first-principles calculation suggested that a large atom of tin can be incorporated into a diamond lattice with a split-vacancy configuration, in which a tin atom sits on an interstitial site with two neighboring vacancies. The $\mathrm{Sn}\text{\ensuremath{-}}V$ center showed a sharp zero phonon line at 619 nm at room temperature. This line split into four peaks at cryogenic temperatures, with a larger ground state splitting ($\ensuremath{\sim}850\text{ }\text{ }\mathrm{GHz}$) than that of color centers based on other group-IV elements, i.e., silicon-vacancy ($\mathrm{Si}\text{\ensuremath{-}}V$) and germanium-vacancy ($\mathrm{Ge}\text{\ensuremath{-}}V$) centers. The excited state lifetime was estimated, via Hanbury Brown--Twiss interferometry measurements on single $\mathrm{Sn}\text{\ensuremath{-}}V$ quantum emitters, to be $\ensuremath{\sim}5\text{ }\text{ }\mathrm{ns}$. The order of the experimentally obtained optical transition energies, compared with those of $\mathrm{Si}\text{\ensuremath{-}}V$ and $\mathrm{Ge}\text{\ensuremath{-}}V$ centers, was in good agreement with the theoretical calculations.

arXiv:1708.03576•Physical Review Letters•Dec 22, 2017•324 citations
Group-IV color centers in diamonds are promising not only as spin-photon interfaces for quantum networks but also as multicolor photoluminescence probes and all-optical temperature sensors for biological research. Therefore, generating group-IV color centers in detonation nanodiamonds (DNDs), the smallest class of diamond nanocrystals, has become a research focal point. This approach holds potential for the noninvasive introduction of diamond sensors into living cell organelles, enabling sensing of local structural and temperature changes with minimal disturbance. Following the successful generation of silicon- and germanium-vacancy centers in DNDs, the generation of tin-vacancy (SnV) centers was investigated. Similar to other group-IV color centers, the SnV centers exhibit strong photoluminescence. In addition, the SnV center offers a long spin coherence time compared with those of silicon- and germanium-vacancy centers. However, the strain induced by large Sn atoms poses substantial challenges for generating SnV centers in ultrasmall nanodiamonds. In this study, Sn-doped DNDs with a mean particle size of ~ 5 nm were subjected to a 3 days boiling acid treatment, which led to sharp zero-phonon lines of SnV centers at ~ 620 nm in the photoluminescence spectra. Photon autocorrelation measurements further revealed the presence of single SnV centers in these DNDs.
Nanodiamonds containing single tin-vacancy (SnV) centers have the potential for integration into nanophotonic devices employed in quantum technologies such as quantum sensing, quantum information processing and quantum communication. The present study assessed single SnV centers in nanodiamonds less than 10 nm in size. Such centers were generated by implanting Sn ions into size-selected small nanodiamonds followed by high-temperature annealing. A sharp emission peak with a line width of 2.6 nm was observed at 618.7 nm, corresponding to the zero phonon line of SnV centers in bulk diamond. The Debye–Waller factor for this peak at room temperature was estimated to be 0.38 and so was slightly greater than the value for bulk diamond. A second-order correlation function yielded a g 2 (0) value of 0.04 ± 0.11, indicating single-photon emission. The successful creation of single SnV centers in nanodiamonds is a critical step toward integrating nanophotonic devices for photonic quantum technologies.
Quantum emitters in diamond are a promising candidate for quantum network applications. Here, we show basic properties of tin-vacancy (SnV) centers in diamond, which we recently discovered. The SnV center shows a sharp zero phonon line and a high fluorescence intensity. The SnV center has a possibility to have a long spin coherence time in the Kelvin temperature range, in contrast to other group-IV color centers, i.e. silicon-vacancy and germanium-vacancy centers. We discuss important experiments regarding spin and optical properties of the SnV quantum emitter for further development towards quantum network.
Group IV color centers in diamond are promising single-photon emitters for quantum information processing and networking. Among them, the tin-vacancy (SnV) center stands out due to its long spin coherence times at cryogenic temperatures above 1 K. While SnV centers have been realized using various fabrication routes, their in situ formation via microwave plasma-enhanced chemical vapor deposition (MW PE CVD) remains relatively unexplored. In this study, SnV centers, identified by a zero-phonon line (ZPL) near 620 nm, were synthesized in nanocrystalline diamond and free-standing microcrystalline diamond using tin oxide (SnO 2 ) as a dopant source at substrate temperatures of 750°C and 850°C. Photoluminescence measurements reveal that lowering the substrate temperature enhances both the ZPL intensity and spatial uniformity of SnV centers. These results highlight substrate temperature as a key parameter for controlling SnV incorporation during MW PE CVD growth and provide insights into optimizing fabrication strategies for diamond-based quantum technologies.
Ultrasmall (about 10 nm), low-strain, artificially produced diamonds with an internal, active color center have substantial potential for quantum information processing and biomedical applications. Thus, it is of great importance to be able to artificially produce such diamonds. Here, we report on the high-pressure, high-temperature synthesis of such nanodiamonds about 10 nm in size and containing an optically active, single silicon-vacancy color center. Using special sample preparation technique, we were able to prepare samples containing single nanodiamonds on the surface. By correlating atomic-force microscope images and confocal optical images, we verified the presence of optically active color centers in single nanocrystals, and using second-order correlation measurements, we proved the single-photon emission statistics of these nanodiamonds. These color centers have nonblinking, spectrally narrow emission with narrow distribution of spectral width and positions of zero-phonon line, thus proving the high quality of the nanodiamonds produced.
Tin-Vacancy (Sn-V) colour centres in diamond have a spin coherence time in the millisecond range at temperatures of 2 K, so they are promising to be used in diamond-based quantum optical devices. However, the incorporation of large Sn atoms into a dense diamond lattice is a non-trivial problem. The objective of our work is to use microwave plasma-assisted chemical vapour deposition (CVD) to grow Sn-doped diamond with submicron SnO 2 particles as a solid-state source of impurity. Well-faceted diamond microcrystals with sizes of a few micrometres were formed on AlN substrates. The photoluminescence (PL) signal with zero-phonon line (ZPL) peak for Sn-V centre at ≈620 nm was measured at room temperature (RT) and at 7 K. The peak width (full width at half-maximum) was measured to be 1.1–1.7 nm at RT and ≈0.05 nm at 7 K. The observed variations of ZPL shape and position, in particular, narrowing of PL peak at RT and formation of single-line fine structure at low- T , are attributed to strain in the crystallites. The diamond doping with Sn via CVD process offers a new route to from Sn-V colour centre in the bulk of the diamond crystallites. This article is part of the Theo Murphy meeting issue 'Diamond for quantum applications'.
Tin-vacancy ($\mathrm{Sn}\text{\ensuremath{-}}V$) color centers were created in diamond via ion implantation and subsequent high-temperature annealing up to $2100\text{ }\ifmmode^\circ\else\textdegree\fi{}\mathrm{C}$ at 7.7 GPa. The first-principles calculation suggested that a large atom of tin can be incorporated into a diamond lattice with a split-vacancy configuration, in which a tin atom sits on an interstitial site with two neighboring vacancies. The $\mathrm{Sn}\text{\ensuremath{-}}V$ center showed a sharp zero phonon line at 619 nm at room temperature. This line split into four peaks at cryogenic temperatures, with a larger ground state splitting ($\ensuremath{\sim}850\text{ }\text{ }\mathrm{GHz}$) than that of color centers based on other group-IV elements, i.e., silicon-vacancy ($\mathrm{Si}\text{\ensuremath{-}}V$) and germanium-vacancy ($\mathrm{Ge}\text{\ensuremath{-}}V$) centers. The excited state lifetime was estimated, via Hanbury Brown--Twiss interferometry measurements on single $\mathrm{Sn}\text{\ensuremath{-}}V$ quantum emitters, to be $\ensuremath{\sim}5\text{ }\text{ }\mathrm{ns}$. The order of the experimentally obtained optical transition energies, compared with those of $\mathrm{Si}\text{\ensuremath{-}}V$ and $\mathrm{Ge}\text{\ensuremath{-}}V$ centers, was in good agreement with the theoretical calculations.