The excited state structural dynamics of phenyl absorbing S2（A＇）, S3（A＇）, and S6（A＇） states were troseopy and complete active space self-consistent and the UV absorption bands were assigned on azide （PhN3） ...The excited state structural dynamics of phenyl absorbing S2（A＇）, S3（A＇）, and S6（A＇） states were troseopy and complete active space self-consistent and the UV absorption bands were assigned on azide （PhN3） after excitation to the light studied using the resonance Raman specfield calculations. The vibrational spectra the basis of the Fourier transform （FT）- Raman, FT-infrared measurements, the density-functional theory computations and the normal mode analysis. The A-, B-, and C-bands resonance Raman spectra in cyclohex- ane, acetonitrile, and methanol solvents were, respectively, obtained at 273.9, 252.7, 245.9, 228.7, 223.1, and 208.8 nm excitation wavelengths to probe the corresponding structural dynamics of PhN3. The results indicated that the structural dynamics in the S2 （A＇）, S3（A＇）, and S6（A＇） states were significantly different. The crossing points of the potential energy surfaces, S2S1（1） and S2S1（2）, were predicted to play a key role in the low-lying excited state decay dynamics, in accordance with Kasha＇s rule, and NT=N8 dissociation. Two decay channels initiated from the Franck-Condon region of the S2（A＇） state were predicted： the radiative S2,min→S0 radiative decay and the S2→S1 internal conversion through the crossing points S2S1 （1）/S2S1（2）.展开更多
The decay dynamics of N, N-dimethylthioacetamide after excitation to the S3（ππ＊） state was studied by using the resonance Raman spectroscopy and complete active space self- consistent field method calculations. T...The decay dynamics of N, N-dimethylthioacetamide after excitation to the S3（ππ＊） state was studied by using the resonance Raman spectroscopy and complete active space self- consistent field method calculations. The UV-absorption and vibrational spectra were as- signed. The A-band resonance Raman spectra were obtained in acetonitrile, methanol and water with the laser excitation wavelengths in resonance with the first intense absorption band to probe the Franck-Condon region structural dynamics. The CASSCF calculations were carried out to determine the excitation energies and optimized structures of the lower- lying singlet states and conical intersection point. The A-band structural dynamics and the corresponding decay mechanism were obtained by the analysis of the resonance Raman in- tensity pattern and the CASSCF calculated structural parameters. The major decay channel of S3,FC （ππ＊）→S3（ππ＊）/S1 （nπ＊）→S1（nπ＊） is proposed.展开更多
The photophysics of 3-dimethylamino-2-methyl-propenal （DMAMP） after excitation to the S2 （ππ^＊） electronic state was studied using the resonance Raman spectroscopy and complete active space self-consistent fiel...The photophysics of 3-dimethylamino-2-methyl-propenal （DMAMP） after excitation to the S2 （ππ^＊） electronic state was studied using the resonance Raman spectroscopy and complete active space self-consistent field method calculations. The transition barriers of the ground state tautomerization reactions between DMAMP and its three isomers were determined at B3LYP/6-311＋＋G（d,p） level of theory. The vibrational spectra were assigned. The A- band resonance Raman spectra were obtained in acetonitrile with excitation wavelengths in resonance with the first intense absorption band to probe the structural dynamics of DMAMP. The B3LYP-TD computation was carried out to determine the relative A-band resonance Raman intensities of the fundamental modes, and the result indicated that the vibronic-coupling existed in Franck-Condon region. Complete active space self-consistent field （CASSCF） calculations were carried out to determine the excitation energies of the lower-lying singlet and triplet excited states, the conical intersection points and the intersystem crossing points. The A-band short-time structural dynamics and the corresponding decay dynamics of DMAMP were obtained by analysis of the resonance Raman intensity pattern and CASSCF computations. It was found that a sudden de-conjugation between C1=O6 and C2=C3 occurred at the Franck-Condon region of the S2（ππ^＊） state, while the enhancement of the conjugation interaction between C3 and N（CH3）2, and between C1 and C2 evolutions shortly after the wavepacket leaves away the Pranck-Condon region via the excited state charge redistribution. The de-conjugation interaction between C1=O6 and C2=C3 made the rotation of C3=N（CH3）2 group around the C2-C3 bond much easier, while the enhanced conjugation between C1 and C2, and between C3 and N（CH3）2 made the rotation around the C1-C2 bond and C3-N5 more difficult. It was revealed that the initial structural dynamics of DMAMP was predominantly towards the CI-I（S2/S0） point, while the opportunities towards either CI-2（S2/S0） or CI-3（S2/S0） point were negligible. Two decay channels of DMAMP from S2,FC（ππ^＊） to So or Tl,min via various CIs and ISCs were proposed.展开更多
By using a bi-dentate phosphine oxide ligand L(L=bis(diphenylphosphino)methane dioxide),two mononuclear lanthanide complexes[LnL_(2)(DMF)Cl_(2)]Cl(Ln=Sm,1;Dy,2)with a D_(5h)equatorial ligand field(LF)are obtained.Ab i...By using a bi-dentate phosphine oxide ligand L(L=bis(diphenylphosphino)methane dioxide),two mononuclear lanthanide complexes[LnL_(2)(DMF)Cl_(2)]Cl(Ln=Sm,1;Dy,2)with a D_(5h)equatorial ligand field(LF)are obtained.Ab initio CASSCF calculations suggest that the equatorial LF promotes the magnetic anisotropy of the central Sm^(III)and impair that of DyIII.Alternating current(ac)susceptibility measurements reveal that the samarium complex is the first Sm^(III)mono-nuclear complex with slow magnetic relaxation.The isostructural DyIII compound,in contrast,relaxes much faster.Further magnetic property studies were then performed to probe the origin of magnetic anisotropy and magnetic relaxations.展开更多
By reacting a 3,6-ditriazolyl-2,5-dihydroxybenzoquinone(H_(2)trz_(2)An)anilato linker with Ln^(Ⅲ) ions(Ln^(Ⅲ)=Dy,Tb,Ho),two different series of polymorphs,formulated as[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(4)]n·10H_(...By reacting a 3,6-ditriazolyl-2,5-dihydroxybenzoquinone(H_(2)trz_(2)An)anilato linker with Ln^(Ⅲ) ions(Ln^(Ⅲ)=Dy,Tb,Ho),two different series of polymorphs,formulated as[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(4)]n·10H_(2)O(Dy^(Ⅲ),1a;Tb^(Ⅲ),2a,Ho^(Ⅲ),3a)and[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(4)]n·7H_(2)O(Dy^(Ⅲ),1b,Tb^(Ⅲ),2b,Ho^(Ⅲ),3b)have been obtained.In these series the two Dy^(Ⅲ)-coordination networks(1a and 1b)and the Tb^(Ⅲ)-coordination polymer(2b)show a Single Ion Magnet(SIM)behavior.1–3a MOFs show reversible structural flexibility upon removal of a coordinated water molecule from a distorted hexagonal 2D framework to a distorted 3,6-brickwall rectangular 3D structure in[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(2)]n·2H_(2)O(Dy^(Ⅲ),1a_des;Tb^(Ⅲ),2a_des,Ho^(Ⅲ),3a_des)involving shrinkage/expansion of the hexagonal–rectangular networks.Noteworthy,2b represents the first example of a Tb^(Ⅲ)–anilate-based coordination polymer showing SIM behaviour to date and the best SIM properties within the polymorphs.Theoretical investigation via ab initio CASSCF calculations supports this behavior,since 2b shows less mixing between the mJ states of the ground state among all the studied complexes.展开更多
基金This work is supported by the National Natural Science Foundation of China （No.21473163, No.21033002, No.21202032） and the National Basic Research Program of China （No.2013CB834604）.
文摘The excited state structural dynamics of phenyl absorbing S2（A＇）, S3（A＇）, and S6（A＇） states were troseopy and complete active space self-consistent and the UV absorption bands were assigned on azide （PhN3） after excitation to the light studied using the resonance Raman specfield calculations. The vibrational spectra the basis of the Fourier transform （FT）- Raman, FT-infrared measurements, the density-functional theory computations and the normal mode analysis. The A-, B-, and C-bands resonance Raman spectra in cyclohex- ane, acetonitrile, and methanol solvents were, respectively, obtained at 273.9, 252.7, 245.9, 228.7, 223.1, and 208.8 nm excitation wavelengths to probe the corresponding structural dynamics of PhN3. The results indicated that the structural dynamics in the S2 （A＇）, S3（A＇）, and S6（A＇） states were significantly different. The crossing points of the potential energy surfaces, S2S1（1） and S2S1（2）, were predicted to play a key role in the low-lying excited state decay dynamics, in accordance with Kasha＇s rule, and NT=N8 dissociation. Two decay channels initiated from the Franck-Condon region of the S2（A＇） state were predicted： the radiative S2,min→S0 radiative decay and the S2→S1 internal conversion through the crossing points S2S1 （1）/S2S1（2）.
基金This work was supported by the National Natu- ral Science Foundation of China （No.21033002 and No.21202032） and the National Basic Research Pro- gram of China （No.2013CB834604）.
文摘The decay dynamics of N, N-dimethylthioacetamide after excitation to the S3（ππ＊） state was studied by using the resonance Raman spectroscopy and complete active space self- consistent field method calculations. The UV-absorption and vibrational spectra were as- signed. The A-band resonance Raman spectra were obtained in acetonitrile, methanol and water with the laser excitation wavelengths in resonance with the first intense absorption band to probe the Franck-Condon region structural dynamics. The CASSCF calculations were carried out to determine the excitation energies and optimized structures of the lower- lying singlet states and conical intersection point. The A-band structural dynamics and the corresponding decay mechanism were obtained by the analysis of the resonance Raman in- tensity pattern and the CASSCF calculated structural parameters. The major decay channel of S3,FC （ππ＊）→S3（ππ＊）/S1 （nπ＊）→S1（nπ＊） is proposed.
基金ACKNOWLEDGMENTS This work was supported by the National Natural Science Foundation of China （No.21033002 and No.21202032） and the National Basic Research Program of China （No.2013CB834604）.
文摘The photophysics of 3-dimethylamino-2-methyl-propenal （DMAMP） after excitation to the S2 （ππ^＊） electronic state was studied using the resonance Raman spectroscopy and complete active space self-consistent field method calculations. The transition barriers of the ground state tautomerization reactions between DMAMP and its three isomers were determined at B3LYP/6-311＋＋G（d,p） level of theory. The vibrational spectra were assigned. The A- band resonance Raman spectra were obtained in acetonitrile with excitation wavelengths in resonance with the first intense absorption band to probe the structural dynamics of DMAMP. The B3LYP-TD computation was carried out to determine the relative A-band resonance Raman intensities of the fundamental modes, and the result indicated that the vibronic-coupling existed in Franck-Condon region. Complete active space self-consistent field （CASSCF） calculations were carried out to determine the excitation energies of the lower-lying singlet and triplet excited states, the conical intersection points and the intersystem crossing points. The A-band short-time structural dynamics and the corresponding decay dynamics of DMAMP were obtained by analysis of the resonance Raman intensity pattern and CASSCF computations. It was found that a sudden de-conjugation between C1=O6 and C2=C3 occurred at the Franck-Condon region of the S2（ππ^＊） state, while the enhancement of the conjugation interaction between C3 and N（CH3）2, and between C1 and C2 evolutions shortly after the wavepacket leaves away the Pranck-Condon region via the excited state charge redistribution. The de-conjugation interaction between C1=O6 and C2=C3 made the rotation of C3=N（CH3）2 group around the C2-C3 bond much easier, while the enhanced conjugation between C1 and C2, and between C3 and N（CH3）2 made the rotation around the C1-C2 bond and C3-N5 more difficult. It was revealed that the initial structural dynamics of DMAMP was predominantly towards the CI-I（S2/S0） point, while the opportunities towards either CI-2（S2/S0） or CI-3（S2/S0） point were negligible. Two decay channels of DMAMP from S2,FC（ππ^＊） to So or Tl,min via various CIs and ISCs were proposed.
基金supported by the NSFC(21805048 and 21822508)the Natural Science Foundation of Guangdong Province(2018A030310066 and 2016A030313619)the Project of Educational Commission of Guangdong Province(2017KQNCX146).
文摘By using a bi-dentate phosphine oxide ligand L(L=bis(diphenylphosphino)methane dioxide),two mononuclear lanthanide complexes[LnL_(2)(DMF)Cl_(2)]Cl(Ln=Sm,1;Dy,2)with a D_(5h)equatorial ligand field(LF)are obtained.Ab initio CASSCF calculations suggest that the equatorial LF promotes the magnetic anisotropy of the central Sm^(III)and impair that of DyIII.Alternating current(ac)susceptibility measurements reveal that the samarium complex is the first Sm^(III)mono-nuclear complex with slow magnetic relaxation.The isostructural DyIII compound,in contrast,relaxes much faster.Further magnetic property studies were then performed to probe the origin of magnetic anisotropy and magnetic relaxations.
基金support from the EU(ERC Advanced Grant MOL-2D 788222)the Spanish MCIN(Grants PID2020-117264GB-I00 and PID2020-117152RB-I00 funded by MCIN/AEI/10.13039/501100011033 and Unidad de Excelencia María de Maeztu CEX2019-000919-M)and the Generalitat Valenciana(PROMETEO program),is acknowledged+3 种基金supported by MCIN with funding from the European Union NextGenerationEU(PRTR-C17.I1)and by Generalitat Valenciana.JJB and SD would like to thank EU(Grant No.2D-SMARTiES ERC-StG-101042680 and Marie Curie Fellowship SpinPhononHyb2D 101107713)the Plan Gent of Excellence of the Generalitat Valenciana(Grant No.CDEIGENT/2019/022)for the fundingfunded in Italy by Fondazione di Sardegna,Convenzione Triennale tra la Fondazione di Sardegna e gli Atenei Sardi,Regione Sardegna,L.R.7/2007 annualità2022,project VOC_3D“3D printed optical VOC sensors for indoor air quality evaluation”CUP F73C23001590007Alejandra Soriano-Portillo for PXRD measurements and J.M.Martínez-Agudo and G.Agustífor magnetic measurements.
文摘By reacting a 3,6-ditriazolyl-2,5-dihydroxybenzoquinone(H_(2)trz_(2)An)anilato linker with Ln^(Ⅲ) ions(Ln^(Ⅲ)=Dy,Tb,Ho),two different series of polymorphs,formulated as[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(4)]n·10H_(2)O(Dy^(Ⅲ),1a;Tb^(Ⅲ),2a,Ho^(Ⅲ),3a)and[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(4)]n·7H_(2)O(Dy^(Ⅲ),1b,Tb^(Ⅲ),2b,Ho^(Ⅲ),3b)have been obtained.In these series the two Dy^(Ⅲ)-coordination networks(1a and 1b)and the Tb^(Ⅲ)-coordination polymer(2b)show a Single Ion Magnet(SIM)behavior.1–3a MOFs show reversible structural flexibility upon removal of a coordinated water molecule from a distorted hexagonal 2D framework to a distorted 3,6-brickwall rectangular 3D structure in[Ln_(2)(trz_(2)An)_(3)(H_(2)O)_(2)]n·2H_(2)O(Dy^(Ⅲ),1a_des;Tb^(Ⅲ),2a_des,Ho^(Ⅲ),3a_des)involving shrinkage/expansion of the hexagonal–rectangular networks.Noteworthy,2b represents the first example of a Tb^(Ⅲ)–anilate-based coordination polymer showing SIM behaviour to date and the best SIM properties within the polymorphs.Theoretical investigation via ab initio CASSCF calculations supports this behavior,since 2b shows less mixing between the mJ states of the ground state among all the studied complexes.
