Asymmetric adiabatic pulses for NH selection.

Many types of NMR experiments demand the use of frequency-selective pulses to invert magnetization within discrete frequency limits. For certain experiments, only one side of the inversion band must be sharply demarcated, in which case this transition bandwidth can be narrowed when using an asymmetric adiabatic full passage. In the present study, a highly efficient asymmetric adiabatic full passage was created from a combination of two adiabatic half passages which used different modulation functions (HS12 and tanh/tan). Each adiabatic half passage occupied a different amount of time in the total pulse and performed one-half of the inversion. On one side, HS12 produced a sharp transition between inverted and noninverted states which was approximately 2.5 times narrower than the transition bandwidth afforded by a symmetric hyperbolic secant pulse of equal length. On the other side of the narrow transition band, the tanh/tan pulse achieved broadband inversion. These asymmetric pulses were applied to select NH groups immediately adjacent to the water signal in water-flip-back HSQC experiments using a double spin echo for the reverse INEPT step.

[1]  B. Sykes,et al.  Water Eliminated Fourier Transform NMR Spectroscopy , 1972 .

[2]  Michael Garwood,et al.  Improved Performance of Frequency-Swept Pulses Using Offset-Independent Adiabaticity , 1996 .

[3]  P. V. van Zijl,et al.  Improved sensitivity of HSQC spectra of exchanging protons at short interscan delays using a new fast HSQC (FHSQC) detection scheme that avoids water saturation. , 1995, Journal of magnetic resonance. Series B.

[4]  M. Garwood,et al.  Reduction of sideband intensities in adiabatic decoupling using modulation generated through adiabatic R-variation (MGAR) , 1996 .

[5]  M. Garwood,et al.  Fast broadband inversion by adiabatic pulses. , 1998, Journal of magnetic resonance.

[6]  G. Bodenhausen,et al.  Natural abundance nitrogen-15 NMR by enhanced heteronuclear spectroscopy , 1980 .

[7]  L. Kay,et al.  Analytical description of the effect of adiabatic pulses on IS, I2S, and I3S spin systems. , 1998, Journal of magnetic resonance.

[8]  Alan R. Rath,et al.  Optimization of modulation functions to improve insensitivity of adiabatic pulses to variations in B1 magnitude , 1988 .

[9]  A. J. Shaka,et al.  Computer-optimized decoupling scheme for wideband applications and low-level operation , 1985 .

[10]  M. Garwood,et al.  OPTIMIZED EXCITATION AND AUTOMATION FOR HIGH-RESOLUTION NMR USING B1-INSENSITIVE ROTATION PULSES , 1996 .

[11]  A. J. Shaka,et al.  Water Suppression That Works. Excitation Sculpting Using Arbitrary Wave-Forms and Pulsed-Field Gradients , 1995 .

[12]  Pines,et al.  Broadband and adiabatic inversion of a two-level system by phase-modulated pulses. , 1985, Physical review. A, General physics.

[13]  Rosenfeld,et al.  Analytic solutions of the Bloch equation involving asymmetric amplitude and frequency modulations. , 1996, Physical review. A, Atomic, molecular, and optical physics.

[14]  M. S. Silver,et al.  Highly selective {π}/{2} and π pulse generation , 1984 .

[15]  R. Freeman,et al.  Optimized Adiabatic Pulses for Wideband Spin Inversion , 1996 .

[16]  Christopher J. Hardy,et al.  Efficient adiabatic fast passage for NMR population inversion in the presence of radiofrequency field inhomogeneity and frequency offsets , 1986 .

[17]  Michael Garwood,et al.  Symmetric pulses to induce arbitrary flip angles with compensation for rf inhomogeneity and resonance offsets , 1991 .

[18]  Design of selective adiabatic inversion pulses using the adiabatic condition , 1997, Journal of magnetic resonance.

[19]  M. Garwood,et al.  Adiabatic DANTE sequences for B1-insensitive narrowband inversion , 1992 .

[20]  R. Freeman,et al.  Compensation for Spin–Spin Coupling Effects during Adiabatic Pulses , 1997 .

[21]  Gareth A. Morris,et al.  Enhancement of nuclear magnetic resonance signals by polarization transfer , 1979 .

[22]  Y Zur,et al.  Design of adiabatic pulses for fat‐suppression using analytic solutions of the bloch equation , 1997, Magnetic resonance in medicine.

[23]  M. Bendall Heteronuclear J Coupling Precession during Spin-Lock and Adiabatic Pulses. Use of Adiabatic Inversion Pulses in High-Resolution NMR , 1995 .