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a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the <t>EasySpin</t> toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.
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a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the <t>EasySpin</t> toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.
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a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the <t>EasySpin</t> toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.
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a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the <t>EasySpin</t> toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.
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a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the <t>EasySpin</t> toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.
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a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the EasySpin toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.

Journal: Nature Communications

Article Title: Substituted Fullerenes for Enhanced Optical Nuclear Hyperpolarization in Random Orientations

doi: 10.1038/s41467-025-66211-y

Figure Lengend Snippet: a Schematic of triplet dynamic nuclear polarization. Following the photoexcitation of polarizing agents, spin-selective intersystem crossing generates spin-polarized triplet electrons. Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the EasySpin toolbox in MATLAB R2024a . The zero-field splitting (ZFS) parameters ( D and E ) and triplet sublevel populations ( p x , p y , p z ) used for the simulation are as follows: (C 60 : D = −342 MHz, E = 20 MHz, p x = 0.5, p y = 0.5, p z = 0, Pentacene: D = 1500 MHz, E = −50 MHz, p x = 0.6, p y = 0.3, p z = 0.1). c Decay of visualized ESR signals with T 1e = 2 µs (black line) and T 1e = 30 µs (red line). d Chemical structures of polarizing agents indene-C 60 mono-adducts (ICMA), indene-C 60 bis-adducts e-1, trans-1, trans-2, trans-3, and trans-4.

Article Snippet: Subsequently, the triplet-electron spin polarization is transferred to nuclear spins via an integrated solid effect (ISE). b ISE sequence and electron spin resonance (ESR) simulation using the EasySpin toolbox in MATLAB R2024a .

Techniques: Sequencing, Electron Paramagnetic Resonance