Temperature measurements of proton
T1 (24.7 MHz), deuteron (deuterated hydroxyl
group)
T1 (55.2 MHz),and proton
T1
ges/gifchars/rho.gif" BORDER=0 > (
B1 = 9 G) spin-lattice relaxation times of 2,5-dinitrobenzoic acid have been performed. Ananalysis of present experimental data to
gether with previously published proton
T1 (55.2 MHz) data has revealedthe followin
g molecular motions: proton/deuteron transfer in the hydro
gen bond and two-site hoppin
g of thewhole dimer. It is shown that the proton-transfer dynamics are characterized by two correlation times
![](/ima<font color=)
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ov and
![](/ima<font color=)
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tu, describin
g two fundamentally different motional processes, namely, thermally activated jumps over thebarrier and tunnelin
g throu
gh the barrier. The temperature dependence of 1/
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tu is the solution of Schr&
ouml;din
ger'sequation, which also yields the temperature
Ttun, where be
gins the tunnel pathway for proton transfer. A newequation for the spectral density function of complex motion consistin
g of the three motions is derived. Thethird motion (two-site hoppin
g of the whole dimer characterized by
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ges/
gifchars/tau.
gif" BORDER=0 >
lib correlation time) is responsible for aproton
T1
ges/gifchars/rho.gif" BORDER=0 > minimum in hi
gh temperatures, just below the meltin
g point. Such a minimum is not reached by
T1 temperature dependencies. The minimum of
T1
ges/gifchars/rho.gif" BORDER=0 > assi
gned to the classical hoppin
g of a hydro
gen-bondedproton occurs in the same low-temperature re
gime in which the flattenin
g of the temperature dependenciesof
T1 points to the dominance of incoherent tunnelin
g. This experimental fact denies the known theoriespredictin
g the intermediate temperature re
gime where a smooth transition between classical and quantumtunnelin
g dynamics is expected. The fit of the derived theoretical equations to the experimental data
T1
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T1 is satisfactory. The correlation times obtained for deuterons indicate deuteron-transfer dynamics muchslower than proton-transfer dynamics. It is concluded that the classical proton transfer takes place over thewhole temperature re
gime, while the incoherent tunnelin
g occurs below 46.5 (hydro
gen) or 87.2 K (deuterium)only.