We measure electron- and nuclear-spin transition frequencies in the ground state of nitrogen-vacancy (N-) centers in diamond for two nitrogen isotopes (N- and N-) over temperatures ranging from 77 to 400 K. Measurements are performed using Ramsey interferometry and direct optical readout of the nuclear and electron spins. We extract coupling parameters (for N-), , , , and , and their temperature dependences for both isotopes. The temperature dependences of the nuclear-spin transitions within the spin manifold near room temperature are found to be 0.52(1) ppm/K for N-(| = -1⟩ ↔ | = +1⟩) and -1.1(1) ppm/K for N-(| = -1/2⟩ ↔ | = +1/2⟩). An isotopic shift in the zero-field splitting parameter between N- and N- is measured to be ~ 120 kHz. Residual transverse magnetic fields are observed to shift the nuclear-spin transition frequencies, especially for N-. We have precisely determined the set of parameters relevant for the development of nuclear-spin-based diamond quantum sensors with greatly reduced sensitivity to environmental factors.
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http://dx.doi.org/10.1103/PhysRevApplied.19.064084 | DOI Listing |
Dalton Trans
December 2024
Department of Chemistry, College of Humanities and Sciences, Nihon University, 3-25-40 Sakurajosui, Setagaya-ku, Tokyo 156-8550, Japan.
The spin coherence phenomena of a system consisting of a mononuclear 3d transition metal = 1/2 centre embedded in a polyoxometalate with low nuclear-spin abundance, [(-CH)N]H[SiWOCuZn], have been revealed for the first time. Variable-temperature Hahn-echo experiments using the pulsed electron spin resonance technique showed that its coherence lifetime remains at the submicrosecond level even above 100 K.
View Article and Find Full Text PDFJ Phys Chem A
December 2024
Institute of Physics, University of Kassel, Heinrich-Plett Str. 40, 34132 Kassel, Germany.
The high resolution ro-vibrational spectrum of the diatomic molecule vanadium oxide (VO) in the gas phase was measured around 1000 cm. In total, 1529 ro-vibrational transitions were assigned, in a spectral range of 984-1036 cm. For many transitions, the hyperfine structure resulting from the nuclear spin of V were resolved and the molecular parameters for the first ( = 1) and second ( = 2) excited vibrational state of VO were derived.
View Article and Find Full Text PDFNanophotonics
November 2024
Chimie ParisTech, PSL University, CNRS, Institut de Recherche de Chimie Paris, Paris, France.
Efforts to harness quantum hardware relying on quantum mechanical principles have been steadily progressing. The search for novel material platforms that could spur the progress by providing new functionalities for solving the outstanding technological problems is however still active. Any physical property presenting two distinct energy states that can be found in a long-lived superposition state can serve as a quantum bit (qubit), the basic information processing unit in quantum technologies.
View Article and Find Full Text PDFJ Phys Condens Matter
December 2024
Harish-Chandra Research Institute, a CI of Homi Bhabha National Institute, Chhatnag Road, Jhunsi, Allahabad 211019, India.
Symmetries play a crucial role in understanding phases of matter and the transitions between them. Theoretical investigations of quantum models with SU() symmetry have provided important insights into many-body phenomena. However, these models have generally remained a theoretical idealization, since it is very difficult to exactly realize the SU() symmetry in conventional quantum materials for large.
View Article and Find Full Text PDFPhys Rev Lett
October 2024
Department of Physics, University of Nevada, Reno, Nevada 89557, USA.
We propose a general technique to produce cold spin-polarized molecules in the electronic states of Σ symmetry, in which rotationally excited levels are first populated by coherent microwave excitation, and then allowed to spin flip and relax via collisional quenching, which populates a single final spin state. The steady-state spin polarization is maximized in the regime, where collisional slip-flipping transitions in the ground rotational manifold (N=0) are suppressed by a factor of ≥10 compared to those in the first rotationally excited manifold (N=1), as generally expected for Σ-state molecules at temperatures below the rotational spacing between the N=0 and N=1 manifolds. We theoretically demonstrate the high selectivity of the technique for ^{13}C^{16}O molecules immersed in a cold buffer gas of helium atoms, achieving a high degree (≥95%) of nuclear spin polarization at 1 K.
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