Central-line intensity optimization with a two-pulse sequence in solid-state MAS NMR using a JDK1.3 applet

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Example 2 of two-pulse MAS simulation

The example, which is complementary to Example 1, also deals with the central-line intensity of a spin I = 3/2 in a powder sample rotating at the magic angle with a rotor speed of 10 kHz.

The strength of the RF magnetic field is 100 kHz.

The values of the two quadrupole parameters are 1000 kHz for the quadrupole coupling constant QCC and 0 for the asymmetry parameter eta.

The simulation associated with the two-pulse sequence is A()B(p2), where the second-pulse length p2 increases from 0 to 10 µs by 0.25 µs step; the first-pulse length p1 is 6 µs. There is no interpulse delay (tau1 = 0, this is an approximation) whereas experimental tau1 is about 10 µs.

The pulse length to pulse increment ratios are integers.

The number of integration steps for alpha and for beta Euler angles are MaxAlpha = 20, that for gamma Euler angle is MaxGamma = 10.

The first pulse excites the ±3-quantum coherences simultaneously.

IMAGE: Effect of the second-pulse length on the simulation

The sign of the central-line intensity changes several times for a range of the second-pulse length p2 that is much shorter than that of the first-pulse length p1 in Example 1.

Solid-state NMR bibliography for:

Aluminum-27
Antimony-121/123
Arsenic-75
Barium-135/137
Beryllium-9
Bismuth-209
Boron-11
Bromine-79/81
Calcium-43
Cesium-133
Chlorine-35/37
Chromium-53
Cobalt-59
Copper-63/65
Deuterium-2
Gallium-69/71
Germanium-73
Gold-197
Hafnium-177/179
Indium-113/115
Iodine-127
Iridium-191/193
Krypton-83
Lanthanum-139
Lithium-7
Magnesium-25
Manganese-55
Mercury-201
Molybdenum-95/97
Neon-21
Nickel-61
Niobium-93
Nitrogen-14
Osmium-189
Oxygen-17
Palladium-105
Potassium-39/41
Rhenium-185/187
Rubidium-85/87
Ruthenium-99/101
Scandium-45
Sodium-23
Strontium-87
Sulfur-33
Tantalum-181
Titanium-47/49
Vanadium-51
Xenon-131
Zinc-67
Zirconium-91
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