1979
DOI: 10.1016/0022-2364(79)90064-7
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Spin-lattice relaxation of carbon-13 in the rotating frame

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Cited by 15 publications
(8 citation statements)
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“…One category comprises the CAMELSPIN (13) or ROESY (for rotating-frame Overhauser enhancement spectroscopy) (14), the rotating frame counterparts of the homonuclear NOE spectroscopy. The other category is T 1 measurements for heteronuclei with spin 1 2 (15)(16)(17)(18) and with higher spin quantum number (6, 19 -21). This technique allows one to sample spectral densities at frequencies of the order of RF field strength, thus making slow processes effective.…”
Section: Introductionmentioning
confidence: 99%
“…One category comprises the CAMELSPIN (13) or ROESY (for rotating-frame Overhauser enhancement spectroscopy) (14), the rotating frame counterparts of the homonuclear NOE spectroscopy. The other category is T 1 measurements for heteronuclei with spin 1 2 (15)(16)(17)(18) and with higher spin quantum number (6, 19 -21). This technique allows one to sample spectral densities at frequencies of the order of RF field strength, thus making slow processes effective.…”
Section: Introductionmentioning
confidence: 99%
“…To avoid complications from the decoupling source during the locking time, the proton decoupler was turned on only during FID collection time. 19 The center of the spectrum was carefully set to be less than 5 Hz away from the main peak to avoid any error caused by offresonance conditions. All T1F data were collected at 75 MHz 13 C Larmor frequency.…”
Section: Methodsmentioning
confidence: 99%
“…The actual power used was equivalent to the magnetic field for 2 kHz 13 C Larmor frequency. To avoid complications from the decoupling source during the locking time, the proton decoupler was turned on only during FID collection time . The center of the spectrum was carefully set to be less than 5 Hz away from the main peak to avoid any error caused by off-resonance conditions.…”
Section: Methodsmentioning
confidence: 99%
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“…In particular, the component of the magnetization vector initially transverse to B eff will remain transverse to B eff , and the relaxation of the magnetization during that time is dominated by T 2ρ (24). Analytical expressions for T 1ρ and T 2ρ relaxation times have been worked out for a few cases (49,50). In liquid samples dominated by fast dipolar interactions, T 1 ρ → T 2 and T2ρ1(1/2)(T11+T21)1 (22,23,50).…”
Section: Theorymentioning
confidence: 99%