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. 2020 Dec 2;27(1):316–325. doi: 10.1002/chem.202003143

Table 2.

Signal‐to‐noise (SNrel) ratios (relative to 1H=100 %) and gain and loss factors for indirect (by CPMG‐HSQMBC) versus direct 77Se NMR detection.

77Se detection method

77Se direct

1H[77Se] CPMG‐HSQMBC

signal halfwidth

3.0 Hz

1.5 Hz

SNrel=SN/√number‐of‐scans

0.077 %

1.763 %

f gain=SNrel(1H[77Se])/SNrel(77Se)[a]

23

f theor=(γ H/γ Se)⋅(γ H/γ Se)1.5[b]

62.5

f 100 %=100 %/7.63 %[c]

13.1

13.1

SN100 %=SNrelf 100 % [d]

1.0 %

23.1 %

f INEPT=√SN100 %(1H[77Se])[e]

48.1 %

f coil,Se =SN100 %f theor [f]

63.5 %

Spectra were recorded with the same FID resolution (0.5 Hz), receiver gain, long total interscan delay (6.3 s>3⋅T1), and were processed identically after exponential line broadening with the indicated natural signal halfwidth. For the CPMG‐HSQMBC experiment, the SN of H1 was multiplied by 2 to compensate a 50 % loss from gradient coherence selection. [a] f gain is the experimentally achieved gain with the CPMG‐HSQMBC indirect versus direct 77Se detection scheme. [b] f theor is the theoretical gain for indirect 77Se detection with an 1H↔77Se out‐and‐back transfer scheme, relative to direct 77Se detection. [c] f 100 % is the gain from 100 % enrichment of 77Se. [d] SN100=SNrel compensated for natural 77Se isotope abundance. [e] f INEPT is the transfer efficiency of each CPMG‐INEPT step in the CPMG‐HSQMBC experiment (with Δ opt=70 ms, BCPMG=1371 Hz, δ CPMG=157.3 μs). [f] f coil,Se is the outer‐coil 77Se detection sensitivity relative to inner‐coil 1H detection (BRUKER 600 MHz TBI probehead).