eMagRes 2017
DOI: 10.1002/9780470034590.emrstm1510
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Pulse EPR

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Cited by 14 publications
(10 citation statements)
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“…Importantly, under microwave pulses of various power and length, MgHOTP exhibits oscillations of spin orientations with frequencies ω Rabi that are linearly dependent on B 1 (Figures b and S12), providing key evidence that radicals in MgHOTP are suitable for single-qubit quantum gate operations . More practically, an electron spin qubit must also possess long spin–lattice relaxation time ( T 1 ) and phase memory time ( T m ) to ensure sufficient duration of its polarization and coherence. , To measure T 1 and T m , we employed inversion recovery and Hahn echo decay pulse sequences, respectively, on dry powders of MgHOTP. Depending on the synthetic conditions of each batch of MgHOTP, these measurements gave room-temperature values of T 1 ranging from 9.48 to 21.34 μs and T m ranging from 153 to 239 ns at 296 K (Figures c,d and S13), qualifying MgHOTP as a potential candidate for quantum sensing of chemical analytes under ambient conditions.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Importantly, under microwave pulses of various power and length, MgHOTP exhibits oscillations of spin orientations with frequencies ω Rabi that are linearly dependent on B 1 (Figures b and S12), providing key evidence that radicals in MgHOTP are suitable for single-qubit quantum gate operations . More practically, an electron spin qubit must also possess long spin–lattice relaxation time ( T 1 ) and phase memory time ( T m ) to ensure sufficient duration of its polarization and coherence. , To measure T 1 and T m , we employed inversion recovery and Hahn echo decay pulse sequences, respectively, on dry powders of MgHOTP. Depending on the synthetic conditions of each batch of MgHOTP, these measurements gave room-temperature values of T 1 ranging from 9.48 to 21.34 μs and T m ranging from 153 to 239 ns at 296 K (Figures c,d and S13), qualifying MgHOTP as a potential candidate for quantum sensing of chemical analytes under ambient conditions.…”
Section: Resultsmentioning
confidence: 99%
“…Notably, CP-ESEEM with MgHOTP enables quantitative detection of even lower concentrations of Li + because the ESEEM signal from 7 Li can be referenced to that of an internal standard, here 1 H (see theoretical analysis in the Supporting Information). , We took advantage of the narrow line width of MgHOTP (Figures a and S25) and adopted an optimal CP-ESEEM delay time τ = 120 ns, which gives maximum modulation depth from 7 Li (Figures c and S26–S28). With these parameters, all CP-ESEEM measurements display 1 H peaks with the same line shape for any [Li + ] in the range 1 × 10 –4 –2 mol/L (Figure d), showing minimal influence of 7 Li nuclear spins on the radical– 1 H interactions.…”
Section: Resultsmentioning
confidence: 99%
“…However, it has been shown that the superposition of nuclear frequencies does not lead to large errors in the determination of D ( Fursman and Hore, 1999 ). 4) The typical deadtime of a pulsed EPR spectrometer ( Stoll, 2017 ) precludes detection of the early response to the application of the OOP ESEEM pulse sequence (typically ≈100 ns after the last microwave pulse). Hence, one has to cope with a “truncated” time trace.…”
Section: Resultsmentioning
confidence: 99%
“…The radical signature is clearly asymmetric because the electron-Zeeman anisotropy, determined by the g -matrix of FADH • , exceeds the inhomogeneous spectral linewidth. By recording ENDOR spectra at different magnetic field positions in the resonance range one can now detect molecules with particular orientations with respect to the direction of the external magnetic field vector B 0 29 , 38 , 39 . For example, recording ENDOR at a magnetic-field strength B 0 corresponding to the principal value g Z of FADH • reveals hyperfine data of those molecules whose principal Z axis is aligned parallel to B 0 thus resembling data from a partially oriented sample.…”
Section: Resultsmentioning
confidence: 99%