Saiya Fujiwara's research while affiliated with RIKEN and other places

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Publications (16)


Modulation of triplet quantum coherence by guest-induced structural changes in a flexible metal-organic framework
  • Preprint

May 2024

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19 Reads

Akio Yamauchi

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Saiya Fujiwara

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[...]

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Quantum sensing using molecular qubits is expected to provide excellent sensitivity due to the proximity of the sensor to the target analyte. However, many molecular qubits are used at cryogenic temperatures, and how to make molecular qubits respond to specific analytes remains unclear. Here, we propose a new material design in which the coherence time changes in response to a variety of analytes at room temperature. We used the photoexcited triplet, which can be initialized at room temperature, as qubits and introduce them to a metal–organic framework that can flexibly change its pore structure in response to guest adsorption. By changing the local molecular density around the triplet qubits by adsorption of a specific analyte, the mobility of the triplet qubit can be changed, and the coherence time can be made responsive.

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Fig. 2. Characterizations of Pn-MOF. (A) chemical structure of PdBA. (B) Simulated PXRd pattern of Pn-MoF (black line) and experimental PXRd patterns of Pn-MoF (red line), Pn-MoF in paraffin (green line), and paraffin (blue line). a.u., arbitrary units. (C) uv-vis absorption spectra of 1 mM PdBA in dMF (black line), Pn-MoF (red line), neat PdBA solid (blue line), and Pn-MoF in paraffin (green line). (D) Simulated structure of Pn-MoF with uio-68-type topology. (E) The nearest and second nearest pentacene moieties in Pn-MoF.
Fig. 3. TAS measurements of Pn-MOF. (A) experimentally observed spectral evolution of the femtosecond TAS (excitation wavelength, 600 nm) of Pn-MoF in paraffin. (B) Temporal change of transient absorption at selected wavelengths and fitting curves from global analysis. (C) eAS obtained from global analysis based on the sequential model based on two components. eAS1 and eAS2 indicate the first and second components of eAS, respectively. (D) Temperature dependence of the transient absorption at 530 nm of Pn-MoF.
Fig. 5. Model of the density matrix formalism analysis. different multiexcitons, (A) strongly coupled triplet pair 5 TT ( 5 TT 1 and 5 TT 2 ), (B) weakly coupled ScTP (T + T), and (C) noncorrelated two triplets T + T, are included with considering molecular rotation, exciton migration, and reencounter processes.
Fig. 6. Transient nutation of the quintet state at room temperature. (A) Pulse sequence of the transient nutation measurement. (B) Two main quantum gates detected by the pulsed microwave at B 0 = 348.1 mT in the quintet sublevels. (C) echo-detected ePR spectrum at τ delay = 1.1 μs. The durations of the first and second pulses are x = 8 ns and t 2 = 16 ns, respectively. Fitting result using eq. S15 and table S5 is shown as a red line. (D) Transient nutation profiles as a function of x in (A) at τ delay = 1.1 μs using t 2 = 16 ns. The simulated profile is shown by a red line considering the anisotropic sublevel populations. At the bottom, decomposition of the computed nutation data by the gates Q 0,±1 and Q ±2,±1 are shown by purple and green lines, respectively. (E) Simulated profiles by the different rotation models. The red solid line corresponding to the red line in (d) is computed by the conformation motion between the dihedral angles of β = 130° and 122° of the T B molecule in the T A T B pair for TT 1 and TT 2 , respectively. Green dashed line is obtained with considering the large dihedral angle change between β = 130° and 150° in Fig. 4B. (F) dependence of τ delay on the echo intensity (black line) employing x = 8 ns, t 2 = 16 ns, and τ echo = 200 ns with B 1 = 0.45 mT together with delay time dependence of the cW-TRePR intensity at 351 mT in Fig. 4A (blue line). Fitting result using eq. S1 and table S5 is shown as a red line.
Fig. 7. Synthetic route of PDBA.
Room-temperature quantum coherence of entangled multiexcitons in a metal-organic framework
  • Article
  • Full-text available

January 2024

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75 Reads

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4 Citations

Science Advances

Singlet fission can generate an exchange-coupled quintet triplet pair state ⁵ TT, which could lead to the realization of quantum computing and quantum sensing using entangled multiple qubits even at room temperature. However, the observation of the quantum coherence of ⁵ TT has been limited to cryogenic temperatures, and the fundamental question is what kind of material design will enable its room-temperature quantum coherence. Here, we show that the quantum coherence of singlet fission–derived ⁵ TT in a chromophore-integrated metal-organic framework can be over hundred nanoseconds at room temperature. The suppressed motion of the chromophores in ordered domains within the metal-organic framework leads to the enough fluctuation of the exchange interaction necessary for ⁵ TT generation but, at the same time, does not cause severe ⁵ TT decoherence. Furthermore, the phase and amplitude of quantum beating depend on the molecular motion, opening the way to room-temperature molecular quantum computing based on multiple quantum gate control.

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Fig. 2. Characterizations of Pn-MOF. (A) Chemical structure of PDBA. (B) Simulated PXRD pattern of Pn-MOF (black line) and experimental PXRD patterns of Pn-MOF (red line), Pn-MOF in paraffin (green line), and paraffin (blue line). (C) UV-vis absorption spectra of 1 mM PDBA in DMF (black line), Pn-MOF (red line), neat PDBA solid (blue line), and Pn-MOF in paraffin (green line). (D) Simulated structure of Pn-MOF with UiO-68 type topology. (E) The nearest and second nearest pentacene moieties in Pn-MOF.
Fig. 5. Transient nutation of the quintet state at room temperature. (A) Pulse sequence of the transient nutation measurement. (B) Two main quantum gates detected by the pulsed microwave at B0 = 348.1 mT in the quintet sublevels. (C) Echo detected EPR spectrum at delay = 1.1 s. The durations of the first and second pulses are x = 8 ns and t2 = 16 ns, respectively. Fitting result using eq. S1 and Table S2 is shown as a red line. (D) Molecular model of the TT-state conformation motions at a frequency of í µí¼ˆ̅ = 22 cm -1 that explains anisotropy of the sublevel populations in (B). (E) Transient nutation profiles as a function of x in (A) at delay = 1.1 s using t2 = 16 ns. The simulated profile is shown by a red line considering the anisotropic sublevel populations. At the bottom, decomposition of the computed nutation data by the gates í µí±„ , and í µí±„ , are shown by purple and green lines, respectively. (F) Simulated profiles by the different rotation models. The red solid line corresponding to the red line in (E) is computed by the conformation motion between the dihedral angles of  = 130 degrees and 122 degrees of the TB molecule in the TATB pair for TT1 and TT2, respectively. Green dotted line is obtained with considering the large dihedral angle change between  = 130 degrees and 150 degrees in Fig. 4B. (G) Dependence of delay on the echo intensity employing x = 16 ns, t2 = 32 ns and τecho = 184 ns with B1 = 0.70 mT. Fitting result using eq. S1 and Table S2 is shown as a red line.
Room-temperature quantum coherence of entangled multiexcitons in a metal-organic framework

April 2023

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143 Reads

Singlet fission (SF) can generate an exchange-coupled quintet triplet pair state 5TT, which could lead to the realization of quantum computing and quantum sensing using entangled multiple qubits even at room temperature. However, the observation of the quantum coherence of 5TT has been limited to cryogenic temperatures, and the fundamental question is what kind of material design will enable its room-temperature quantum coherence. Here we show that the quantum coherence of SF-derived 5TT in a chromophore-integrated metal-organic framework (MOF) can be over hundred nanoseconds at room temperature. The subtle motion of the chromophores in the MOF leads to the enough fluctuation of the exchange interaction necessary for 5TT generation, but at the same time does not cause severe 5TT decoherence. Furthermore, the phase and amplitude of quantum beating can be controlled by molecular motion, opening the way to room-temperature molecular quantum computing based on multiple quantum gate control.


Schematic illustration of DNP using SF-born quintet electron polarization
A Nuclear spins in the thermal equilibrium state. The red and blue arrows indicate α spin state and β spin state, respectively, and the gray circles indicate the populations of each spin state. B Polarization transfer from electron spins in the quintet state (|Q0〉 state, green arrows) generated by photo-induced SF to nuclear spins and the subsequent diffusion of hyperpolarized nuclear spins. The green circles indicate the populations of polarized quintet state. DNP increases the α spin population (red circle) and decrease the β spin population (blue circle), resulting in the hyperpolarized nuclear spin state (red square). C Pulse sequence of quintet/triplet-DNP. D Molecular structures of NaPDBA and γ-cyclodextrin (γCD) and supramolecular assembly of only NaPDBA and the NaPDBA-γCD inclusion complex. E Absorption spectra of NaPDBA in water-glycerol at 143 K (black), NaPDBA-γCD in water-glycerol (1:1) at 143 K (blue), and NaPDBA in methanol at room temperature (red). The concentrations of NaPDBA and γCD were 1 and 5 mM, respectively.
MD simulation of the supramolecular assemblies
A, B MD simulation snapshots of NaPDBA ([NaPDBA] = 1 mM) in water-glycerol (1:1) at 300 K. Parallel oriented dimers are shown in yellow. C, D MD simulation snapshots of NaPDBA and γCD ([NaPDBA] = 1 mM, [γCD] = 5 mM) in water-glycerol (1:1) at 243 K.
Fs-transient absorption spectroscopy (TAS) measurements of the supramolecular assemblies
Overview of fs-TAS analysis of A–E NaPDBA and F–J NaPDBA-γCD in water-glycerol (1:1) at 143 K ([NaPDBA] = 1 mM, [γCD] = 5 mM). A, F Pseudo-2D plots of experimentally observed fs-TAS (excitation: 635 nm for NaPDBA and 600 nm for NaPDBA-γCD), B, G spectral evolution of the TAS, and C, H temporal change of transient absorption at selected wavelengths and fitting curves from global analysis. D, I Evolution-associated spectra (ESA) and E, J corresponding concentration kinetics obtained from global analysis based on sequential models. EAS1, EAS2, and EAS3 indicate the first, second and third components of EAS, respectively.
Time-resolved ESR measurements of the supramolecular assemblies
Time-resolved ESR spectra of A NaPDBA and B NaPDBA-γCD in water-glycerol (1:1) at 143 K ([NaPDBA] = 1 mM, [γCD] = 5 mM) just after photoexcitation at 527 nm and simulated spectra of C NaPDBA and D for NaPDBA-γCD, attributing transitions between each energy level of the quintet in the ESR spectra. The fitting parameters of the ISC-born triplet and SF-born quintet are summarized in Supplementary Tables 1 and 2, respectively.
DNP using SF-born quintet electron spin polarization
A, B¹H-NMR signals under thermal conditions (black lines, 5 scans every 10 min) and after quintet-DNP (red lines, ISE sequence for 5 min, 1 scan) of water-glycerol (glycerol-d8:D2O:H2O = 5:4:1) containing A NaPDBA and B NaPDBA-γCD at 100 K ([NaPDBA] = 1 mM, [γCD] = 5 mM). The photo-excitation wavelength and frequency were 527 nm and 500 Hz, respectively. DNP was performed by matching the magnetic field to the quintet peaks. The microwave power and frequency were 20 W and 17.30 GHz, respectively, the laser powers were 2.7 W for A and 1.5 W for B. The magnetic field sweep width was 10 μs. Magnetic field dependence of the signal intensity of the ¹H NMR by DNP and time-resolved ESR spectra in water-glycerol containing C NaPDBA, D NaPDBA-γCD, and E NaPDBA-βCD ([NaPDBA] = 1 mM, [βCD] = [γCD] = 5 mM). Water-glycerol glass (glycerol-d8:D2O:H2O = 5:4:1) was used for the DNP measurement at 100 K. ISE sequence for 20 s (C, E) and 30 s (D) and 1 scan; microwave power and frequency were 20 W and 17.25 GHz, respectively; laser power: 1.5 W; magnetic field sweep width: 10 μs. Water-glycerol glass (glycerol:H2O = 5:5) was used for the time-resolved ESR measurements at 143 K. ESR spectra were integrated for 10 μs after photoexcitation in order to compare the DNP profile with the ISE sequence for 10 μs. F Microwave power dependence of DNP enhancement. The gray dashed line indicates the microwave power when the ¹H-NMR signal is at its maximum. The red arrow indicates the peak top shift from triplet-DNP to quintet-DNP. Triplet-DNP was performed at 27.4 MHz (ISE sequence for 10 s and 4 scans with a laser power of 2.7 W, microwave frequency of 17.30 GHz and sweep width of 25 μs). Quintet-DNP was performed at 26.9 MHz (ISE sequence for 10 s and 10 scans with a laser power of 2.7 W, microwave frequency of 17.30 GHz and sweep width of 10 μs).
Singlet fission as a polarized spin generator for dynamic nuclear polarization

March 2023

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274 Reads

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16 Citations

Nature Communications

Singlet fission (SF), converting a singlet excited state into a spin-correlated triplet-pair state, is an effective way to generate a spin quintet state in organic materials. Although its application to photovoltaics as an exciton multiplier has been extensively studied, the use of its unique spin degree of freedom has been largely unexplored. Here, we demonstrate that the spin polarization of the quintet multiexcitons generated by SF improves the sensitivity of magnetic resonance of water molecules through dynamic nuclear polarization (DNP). We form supramolecular assemblies of a few pentacene chromophores and use SF-born quintet spins to achieve DNP of water-glycerol, the most basic biological matrix, as evidenced by the dependence of nuclear polarization enhancement on magnetic field and microwave power. Our demonstration opens a use of SF as a polarized spin generator in bio-quantum technology.


Spin-Polarized Radicals with Extremely Long Spin-Lattice Relaxation Time at Room Temperature in a Metal-Organic Framework

February 2023

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43 Reads

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1 Citation

The generation of spin polarization is key in quantum information science and dynamical nuclear polarization. Polarized electron spins with long spin-lattice relaxation times (T1) at room temperature are important for these applications, but have been difficult to achieve. We report the realization of spin-polarized radicals with extremely long T1 at room temperature in a metal-organic framework (MOF) in which azaacene chromophores are densely integrated. Persistent radicals are generated in the MOF by charge separation after photoexcitation. Spin polarization of triplet generated by photoexcitation are successfully transferred to the persistent radicals. Pulse ESR measurements reveal that the T1 of the polarized radical in the MOF is as long as 274 s at room temperature. The achievement of extremely long spin polarization in MOFs with nanopores accessible to guest molecules will be an important cornerstone for future highly sensitive quantum sensing and efficient dynamic nuclear polarization.


Fig. 2. Guest-dependent T 2 of DAT triplets in D-MIL-53. a, Spin echo sequence used for T2 measurement. The intervals of microwave pulses and echo detection were varied. b, Plot of T2 obtained by the single-exponential fitting of the spin echo decay curves against the unit cell volume of MIL-53. Only the T2 obtained from the low field peaks where the effect of ESEEM was small is plotted. c, Spin echo decay curves after pulsed photoexcitation at 532 nm for empty (D-MIL-53⸧DAT) and guest-filled (D-MIL-53⸧[DAT+guest]) samples at room temperature. The decay curves of each sample at the magnetic field corresponding to the higher and lower EPR peaks (Fig. 3a) are shown at the top and bottom, respectively. Single-exponential fitting curves for each sample are also shown. Echo signals were not observed when the guest was h-Tol, EtOH, or AcNt.
Fig. 3. Time-resolved EPR measurements of DAT in D-MIL-53. a, Time-resolved EPR spectra at 0.1-0.5 µs for empty (D-MIL-53⸧DAT) and guest-filled (D-MIL-53⸧[DAT+guest]) samples at room temperature. The simulated EPR spectra are shown as red lines. b, Decays of the ESR peaks at higher and lower magnetic field after pulsed photoexcitation at 532 nm for empty (D-MIL-53⸧DAT) and guest-filled (D-MIL-53⸧[DAT+guest]) samples at room temperature. Decay curves were fitted by a single exponential function and the fitting results are shown as red curves.
Quantum chemical sensing using molecular triplet qubits in a flexible metal–organic framework

August 2022

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93 Reads

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2 Citations

Quantum sensing using molecular qubits is expected to provide excellent sensitivity due to the proximity of the sensor to the target analyte. However, many molecular qubits are used at cryogenic temperatures, and how to make molecular qubits respond to specific analytes remains unclear. Here, we propose a new quantum sensor design in which the coherence time changes in response to a variety of analytes at room temperature. We used the photoexcited triplet, which can be initialized at room temperature, as qubits and introduce them to a metal–organic framework that can flexibly change its pore structure in response to guest adsorption. By changing the local molecular density around the triplet qubits by adsorption of a specific analyte, the mobility of the triplet qubit can be changed, and the coherence time can be made responsive.


Singlet fission as a polarized spin generator for biological nuclear hyperpolarization

April 2022

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49 Reads

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1 Citation

Singlet fission (SF), converting a singlet excited state into a spin-correlated triplet-pair state, is the sole way to generate a spin quintet state in organic materials. Although its application to photovoltaics as an exciton multiplier has been extensively studied, use of its unique spin degree of freedom is largely unexplored. Here, we demonstrate that the spin polarization of the quintet multiexcitons generated by SF improves the sensitivity of biological magnetic resonance through dynamic nuclear polarization (DNP). We form supramolecular assemblies of a few pentacene chromophores and use SF-born quintet spins to achieve DNP of water-glycerol, the most basic biological matrix, at lower microwave intensities than for conventional triplet-based DNP. Our demonstration opens a new use of SF as a “polarized spin generator” in bio-quantum technology.


a) Typical scheme of triplet‐DNP. ISC: intersystem crossing, IC: internal conversion. b) Schematic representation of the hyperpolarization of target nuclei in a flexible MOF by triplet‐DNP and CP.
a) Chemical structures of host D‐MIL‐53, polarizing agent DAT, and target 5‐FU. b) CO2 adsorption isotherms at room temperature for D‐MIL‐53 and D‐MIL‐53⊃DAT. c) PXRD patterns of D‐MIL‐53⊃[DAT+5‐FU] (green) and simulated MIL‐53 in the LP phase (gray).[40] The lozenge diagonal lengths are summarized in Table S1. d) Saturation‐recovery curves of D‐MIL‐53 with/without the guest molecules at 9.4 T (400 MHz), room temperature, fitted with single‐exponential functions.
a) Time‐resolved ESR spectrum of D‐MIL‐53⊃[DAT+5‐FU] just after photoexcitation at 527 nm and simulated spectrum. Fitting parameters are summarized in Table S2. b) ESR decay at 353 mT under pulsed excitation at 527 nm and the result of single‐exponential fitting. c) ¹H‐DNP build‐up curve of D‐MIL‐53⊃[DAT+5‐FU] and bi‐exponential fitting. Fitting parameters are shown in Table S3. d) 0.66 T (28.2 MHz) ¹H NMR signals of under thermal conditions (100 scans) and after triplet‐DNP (ISE sequence for 3 min, 1 scan).
a) Sequence of the triplet‐DNP‐CP process. b) 0.66 T (26.5 MHz) ¹⁹F NMR signals of D‐MIL‐53⊃[DAT+5‐FU] under thermal conditions (1500 scans) and after triplet‐DNP‐CP (ISE sequence for 100 s followed by CP, 15 scans).
Triplet Dynamic Nuclear Polarization of Guest Molecules through Induced Fit in a Flexible Metal–Organic Framework

January 2022

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21 Reads

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24 Citations

Angewandte Chemie International Edition

Angewandte Chemie International Edition

Dynamic nuclear polarization utilizing photoexcited triplet electrons (triplet‐DNP) has great potential for room‐temperature hyperpolarization of nuclear spins. However, the polarization transfer to molecules of interest remains a challenge due to the fast spin relaxation and weak interaction with target molecules at room temperature in conventional host materials. Here, we demonstrate the first example of DNP of guest molecules in a porous material at around room temperature by utilizing the induced‐fit‐type structural transformation of a crystalline yet flexible metal–organic framework (MOF). In contrast to the usual hosts, ¹H spin‐lattice relaxation time becomes longer by accommodating a pharmaceutical model target 5‐fluorouracil as the flexible MOF changes its structure upon guest accommodation to maximize the host–guest interactions. Combined with triplet‐DNP and cross‐polarization (CP), this system realizes an enhanced ¹⁹F NMR signal of guest target molecules.


Citations (11)


... However, until recently, 5 TT could only be realized at cryogenic temperatures below 75 K. A Yamauchi (Kyushu University, Japan) et al. have managed to obtain for the first time room-temperature 5 TT with the quantum coherence time of more than 100 ns [4]. This was achieved by confining chromophore-based molecular qubits (a penthacene compound) within a porous metal-organic framework consisting of both metal and organic ligands. ...

Reference:

Physics news on the Internet: February 2024
Room-temperature quantum coherence of entangled multiexcitons in a metal-organic framework

Science Advances

... Quantum processes play a critical role in many natural systems such as light-harvesting and photosynthetic complexes [1][2][3][4], biological vision [5,6] and light sensing [7][8][9][10] systems as well as in artificial photocatalytic [11][12][13][14] and photovoltaic [15][16][17] materials, materials for quantum sensing applications [18][19][20], or qubits [21][22][23], to name a few. Quantum coherence facilitates efficient and directional excitation energy transfer in the light-harvesting complexes [24][25][26], coupled electron-proton transfer [27][28][29], quantum tunneling [30][31][32], is critical to biological systems [33], and nonradiative energy relaxation, which realizes mechanisms of protection from the photodamage [34][35][36][37][38]. Exciton and multiple exciton generation [39,40], singlet fission [41][42][43][44][45][46][47], triplet energy transfer and sensitization [48][49][50], charge transfer [51][52][53] and charge carrier trapping [54,55] are examples of processes that determine the operation of artificial energy-harvesting and conversion materials. ...

Spin-Polarized Radicals with Extremely Long Spin-Lattice Relaxation Time at Room Temperature in a Metal-Organic Framework
  • Citing Article
  • December 2023

Journal of the American Chemical Society

... 1-4 Its unique quality of producing high-spin electronic states has also raised interest for dynamic nuclear polarization. [5][6][7][8][9] SF is realized by the transformation of one optically bright singlet excited state (S1) into two longlived triplet states (T1), which is facilitated by a number of intermediaries, such as the correlated triplet pair states ( x [TT], x = 1, 3,5), as summarized by the general mechanism 10 ...

Singlet fission as a polarized spin generator for dynamic nuclear polarization

Nature Communications

... For the poten al of chemical quantum sensing, the interac ons between adsorbed guest molecules and qubits can be understood by es ma ng relaxa on me and hyperfine interac ons with electron spin resonance (ESR) measurements. 9,20 We have previously reported that MOFs consis ng of pyridylmodified 5,12-diazatetracene (DAT) ligands (DPyDAT) and Zn ions undergo charge separa on from the photo-excited DAT chromophore, and that the resul ng DAT radicals exhibit rela vely long coherence mes T 2 . 21,24 However, due to the instability of the MOF structure, the response of T 2 to various guest molecules could not be evaluated. ...

Quantum chemical sensing using molecular triplet qubits in a flexible metal–organic framework

... SF is a photophysical process that occurs in molecular systems, wherein an optically prepared singlet (spin-0) exciton forms a pair of triplet (spin-1) excitons on neighbouring chromophores [12]. The process has been the subject of fundamental spectroscopic studies since the 1960s [13,14], and has received renewed interest this century due to its potential use in photovoltaic devices [15][16][17][18] and medical imaging [19]. ...

Singlet fission as a polarized spin generator for biological nuclear hyperpolarization

... Few devices can match the exceptionally low noise temperatures of masers, 1 the microwave analog of lasers. Following the discovery of the first solid-state material that could mase at room temperature, pentacene-doped para-terphenyl (PcPTP), 2 there has been a surge in research exploring further such room-temperature maser materials and coherent microwave sources, [3][4][5][6][7] studying their use in ultrasensitive sensing and communication, 8,9 performance in cavity quantum electrodynamics (cQED), [10][11][12][13] use as polarizers for triplet dynamic nuclear polarization, 14,15 and as microwave mode coolers. [16][17][18] Masers have the potential to revolutionize medical imaging and long-range communications through their ultra-low noise amplification, 19 but even though room-temperature gain media have immensely simplified the maser device by removing the need for cryogenics and vacuum, the contrast between masers and their laser descendants is stark; the latter can be purchased from vendors straight to a home tabletop, while the former has remained in the domain of specialized laboratories, having not yet transcended to a more portable form. ...

Triplet Dynamic Nuclear Polarization of Guest Molecules through Induced Fit in a Flexible Metal–Organic Framework
Angewandte Chemie International Edition

Angewandte Chemie International Edition

... Here, we report the first room-temperature observation of the quantum coherence of SF-derived 5 TT by the suppressed molecular motion in a metal-organic framework (MOF). MOFs are nanoporous crystalline materials composed of metal ions and organic ligands (30)(31)(32)(33)(34)(35)(36)(37). By integrating chromophores into the ligand, the distance and angle between chromophores can be precisely regulated in MOFs (31)(32)(33). ...

Triplet Dynamic Nuclear Polarization of Guest Molecules through Induced Fit in a Flexible Metal‐Organic Framework
  • Citing Article
  • December 2021

Angewandte Chemie

... For time-resolved ESR measurements, the polarizing agents were dispersed in β-estradiol glass. β-estradiol forms a colorless glass that is stable at room temperature, making it a convenient matrix for ESR measurements (28). Parent pentacene and phenyl-modified pentacene, 6,13-diphenylpentacene (DPP) were used in addition to DBFP, DBTP, and DTP for comparison ( Fig. 2A). ...

Design Guidelines to Elongate Spin–Lattice Relaxation Times of Porphyrins with Large Triplet Electron Polarization
  • Citing Article
  • May 2021

The Journal of Physical Chemistry A

... In contrast, DNP via photoexcited triplet electron spins (triplet-DNP) can produce hyperpolarization under milder conditions. [30][31][32][33][34] Photoexcited triplets have large nonequilibrium spin polarizations (∼70% for pentacene 35 ) that are independent of temperature, which enables DNP at higher temperatures and lower magnetic elds. Fig. 1A depicts triplet-DNP. ...

Materials chemistry of triplet dynamic nuclear polarization
  • Citing Article
  • May 2020

Chemical Communications

... Here, we report the first room-temperature observation of the quantum coherence of SF-derived 5 TT by the suppressed molecular motion in a metal-organic framework (MOF). MOFs are nanoporous crystalline materials composed of metal ions and organic ligands (30)(31)(32)(33)(34)(35)(36)(37). By integrating chromophores into the ligand, the distance and angle between chromophores can be precisely regulated in MOFs (31)(32)(33). ...

Dynamic Nuclear Polarization of Metal–Organic Frameworks Using Photoexcited Triplet Electrons
  • Citing Article
  • November 2018

Journal of the American Chemical Society