Table 2.
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 %=SNrel⋅f 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).