Comprehensive Inorganic Chemistry III 2023
DOI: 10.1016/b978-0-12-823144-9.00027-3
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Dynamic nuclear polarization in inorganic solids from paramagnetic metal ion dopants

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Cited by 5 publications
(13 citation statements)
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“…78 Saturation of these transitions is generally not achieved in MIDNP and is therefore a major limiting factor of signal enhancement. 16 The analytical expression for the saturation efficiency, assuming that the polarizing agent is at the same time the main source of relaxation, is related to T 1e and T 2e according to 23,49 assuming that one can replace τ 1e by T 1e . A more detailed derivation of this relation was given in previous studies.…”
Section: Discussionmentioning
confidence: 99%
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“…78 Saturation of these transitions is generally not achieved in MIDNP and is therefore a major limiting factor of signal enhancement. 16 The analytical expression for the saturation efficiency, assuming that the polarizing agent is at the same time the main source of relaxation, is related to T 1e and T 2e according to 23,49 assuming that one can replace τ 1e by T 1e . A more detailed derivation of this relation was given in previous studies.…”
Section: Discussionmentioning
confidence: 99%
“…SE DNP can occur between a nucleus coupled to a single electron upon microwave irradiation on either the zero or double quantum transition. Since these transitions are formally forbidden, the effective nutation frequency ω̃ 1 will be scaled by the strength of the dipolar coupling divided by the nuclear Larmor frequency, ω̃ 1 ω 1 ω d ω n . Saturation of these transitions is generally not achieved in MIDNP and is therefore a major limiting factor of signal enhancement . The analytical expression for the saturation efficiency, assuming that the polarizing agent is at the same time the main source of relaxation, is related to T 1e and T 2e according to , Δ p D Q / Z Q = Δ p D Q / Z Q , e q 1 + ω̃ 1 2 [ R 2 e false( 2 R 1 D Q + 2 R 1 n false) ] 1 where normalΔ p D Q / Z Q is the polarization of the irradiated (DQ or ZQ) transition.…”
Section: Discussionmentioning
confidence: 99%
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“…Amidst the metal ions presenting an accessible EPR resonance, those which experience a strong broadening of their EPR line induced by zero eld splitting (ZFS) or spin orbit coupling (SOC) are also hampered by the subsequent inefficiency of their saturation upon microwave irradiation. 121 In a seminal study published by Corzilius and Griffin in 2011, manganese Mn(II) and gadolinium Gd(III), with S = 5/2 and S = 7/ 2 respectively, were shown to have g factors sufficiently close to that of the free electron and EPR lines sufficiently narrow to produce DNP at 5 T. 122 Thanks to their respective ground states being 6 S and 8 S, the SOC vanishes, leading to narrow central transitions in both cases. Their satellite transitions are signicantly broadened by the rst order ZFS, while the central transition is only affected at the second order, resulting in an overall narrow pseudo spin S = 1/2 EPR prole in highly symmetric highspin complexes for these two metals.…”
Section: Exogenous Molecular Metal Ion Complexes For Mas Dnpmentioning
confidence: 99%
“…An alternative way to introduce the paramagnetic source is to dope the material itself with high-spin metal ions, such as Mn 2+ , Gd 3+ , Cr 3+ , or Fe 3+ . , Under microwave irradiation, the polarization is transferred from the metal ion to nearby nuclei, typically via the solid effect. , If the metal ions are distributed throughout the sample, this naturally results in an enhancement of the bulk spectrum. However, the distribution of enhancement within the sample depends on the dopant concentration, the relaxation properties, and potentially the rate of spin diffusion. , This method, which has been successfully applied to nucleic acid, along with various oxide materials for battery ,, and fuel cell applications, , is known as endogenous DNP.…”
Section: Introductionmentioning
confidence: 99%