Abstract:Magnetic properties of organic charge transfer salts Ag(DX) 2 (DX = 2,5-dihalogeno-N,N'-dicyanoquinonediimine; X = Cl, Br, I) were modified by UV irradiation from paramagnetism to diamagnetism in an irreversible way. The temperature dependence of susceptibility revealed that such change in magnetic behavior could be continuously controlled by the duration of irradiation. The observation with scanning electron microprobe revealed that the original appearance of samples, e.g. black well-defined needle-shaped shi… Show more
“…Similarly to the photochemical transformation of α to γ, Ag(DX) 2 (X = Cl, Br, I) changed to nonmagnetism during UVirradiation ( Figure 27), 91 while before irradiation, they exhibited Pauli paramagnetism, which is the characteristic behavior of metallic substances. Consistent changes were observed in their IR reflectance spectra measured on single crystals (Figure 28), indicating that irradiation altered the conduction properties from that of metal to that of non-metal.…”
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confidence: 95%
“…Consistent changes were observed in their IR reflectance spectra measured on single crystals (Figure 28), indicating that irradiation altered the conduction properties from that of metal to that of non-metal. 91 The phenomena occurring during irradiation have turned out different between Ag(DX) 2 and Ag(DM) 2 (α-to-γ), though the initial and final magnetic properties are qualitatively the same. The differences in phenomena, in its turn, originated from the different chemistry of substituents, which will be discussed later.…”
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confidence: 97%
“…Change in magnetic susceptibility during UVirradiation upon Ag(DCl) 2 . 91 During irradiation, the magnetism gradually changes from paramagnetism to diamagnetism. The pristine sample exhibits the magnetic transition of Pauli paramagnetism to diamagnetism around 60 K. The upturn of » observed at low temperature (¯2030 K) is ascribed to lattice defects, i.e., Curie tail, which once increases from 0 to 3 h, then decreases from 3 to 48 h. Adapted with permission from ref 91. some differences after irradiation since the physical properties qualitatively differed from what they were before irradiation.…”
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confidence: 99%
“…Polarized (a) reflectance and (b) conductivity spectra measured on pristine and UV-irradiated (6 h) single crystals of Ag(DI) 2 . 91 The polarization is (a) parallel or perpendicular, and (b) parallel to the c axis, i.e., the highest conducting direction. Both spectra clearly show that Ag(DI) 2 is metallic before irradiation, but that it is nonmetallic with much lower conductivity after 6-h irradiation.…”
mentioning
confidence: 99%
“…Adapted with permission from ref 91. . 91 Reprinted with permission from ref 91. single crystal. In order to clarify which is the case, the irradiated crystals were viewed by transmission electron microscopy (TEM) in order to directly observe the inner structure of the irradiated crystals ( Figure 33).…”
This study concerns development of a non-destructive method to control conduction and magnetism of molecular solids such as single crystals of charge-transfer complexes. The method is named “optical doping”, where appropriate irradiation is utilized under ambient conditions. Owing to this feature, it can be applied to a wide range of substances while measuring the properties during the control. In addition, the method adds unique conduction and magnetic properties to common insulators. Unlike other doping methods, optical doping only affects the properties and/or structures of the irradiated part of a sample while leaving the rest of the sample unchanged. There are two patterns in the optical doping. Irreversible optical doping produces junction-structures on the single molecular crystals, which exhibit characteristic behavior of semiconductor devices such as diodes and varistors. Reversible optical doping produces “giant photoconductors” and “photomagnetic conductors” by realizing unprecedented metallic photoconduction. In the latter case, localized spins are also excited to produce a Kondo system, where carriers and localized spins interact with each other. Not only the control of conduction and magnetism, the optical doping has realized the observation of physical properties in molecular crystals hardly observed under any thermodynamic condition.
“…Similarly to the photochemical transformation of α to γ, Ag(DX) 2 (X = Cl, Br, I) changed to nonmagnetism during UVirradiation ( Figure 27), 91 while before irradiation, they exhibited Pauli paramagnetism, which is the characteristic behavior of metallic substances. Consistent changes were observed in their IR reflectance spectra measured on single crystals (Figure 28), indicating that irradiation altered the conduction properties from that of metal to that of non-metal.…”
mentioning
confidence: 95%
“…Consistent changes were observed in their IR reflectance spectra measured on single crystals (Figure 28), indicating that irradiation altered the conduction properties from that of metal to that of non-metal. 91 The phenomena occurring during irradiation have turned out different between Ag(DX) 2 and Ag(DM) 2 (α-to-γ), though the initial and final magnetic properties are qualitatively the same. The differences in phenomena, in its turn, originated from the different chemistry of substituents, which will be discussed later.…”
mentioning
confidence: 97%
“…Change in magnetic susceptibility during UVirradiation upon Ag(DCl) 2 . 91 During irradiation, the magnetism gradually changes from paramagnetism to diamagnetism. The pristine sample exhibits the magnetic transition of Pauli paramagnetism to diamagnetism around 60 K. The upturn of » observed at low temperature (¯2030 K) is ascribed to lattice defects, i.e., Curie tail, which once increases from 0 to 3 h, then decreases from 3 to 48 h. Adapted with permission from ref 91. some differences after irradiation since the physical properties qualitatively differed from what they were before irradiation.…”
mentioning
confidence: 99%
“…Polarized (a) reflectance and (b) conductivity spectra measured on pristine and UV-irradiated (6 h) single crystals of Ag(DI) 2 . 91 The polarization is (a) parallel or perpendicular, and (b) parallel to the c axis, i.e., the highest conducting direction. Both spectra clearly show that Ag(DI) 2 is metallic before irradiation, but that it is nonmetallic with much lower conductivity after 6-h irradiation.…”
mentioning
confidence: 99%
“…Adapted with permission from ref 91. . 91 Reprinted with permission from ref 91. single crystal. In order to clarify which is the case, the irradiated crystals were viewed by transmission electron microscopy (TEM) in order to directly observe the inner structure of the irradiated crystals ( Figure 33).…”
This study concerns development of a non-destructive method to control conduction and magnetism of molecular solids such as single crystals of charge-transfer complexes. The method is named “optical doping”, where appropriate irradiation is utilized under ambient conditions. Owing to this feature, it can be applied to a wide range of substances while measuring the properties during the control. In addition, the method adds unique conduction and magnetic properties to common insulators. Unlike other doping methods, optical doping only affects the properties and/or structures of the irradiated part of a sample while leaving the rest of the sample unchanged. There are two patterns in the optical doping. Irreversible optical doping produces junction-structures on the single molecular crystals, which exhibit characteristic behavior of semiconductor devices such as diodes and varistors. Reversible optical doping produces “giant photoconductors” and “photomagnetic conductors” by realizing unprecedented metallic photoconduction. In the latter case, localized spins are also excited to produce a Kondo system, where carriers and localized spins interact with each other. Not only the control of conduction and magnetism, the optical doping has realized the observation of physical properties in molecular crystals hardly observed under any thermodynamic condition.
Metal‐cyanoquinone complex shows great potential in various applications due to its unique molecular structure and physicochemical properties, but has not been reported in electromagnetic protection (absorption and shielding) field. In this work, a series of metal‐cyanoquinone complexes including Cu‐TCNQ, Cu‐DCNQI, and Ag‐DCNQI is first synthesized, and then their electromagnetic protection behaviors are systematically investigated. The results suggest that Cu‐DCNQI shows better electromagnetic wave absorption (EMA) performance compared to Cu‐TCNQ and Ag‐DCNQI, where its maximal absorption reaches −33.2 dB under ultrathin thickness of 0.9 mm with a filler‐loading ratio of 20 wt%. Experimental results and first‐principles calculations indicate that Cu‐DCNQI exhibits good electrical conductivity and narrow bandgap, which are considered to be the main two reasons for its excellent EMA performance. Interestingly, when the filler‐loading ratio of CU‐DCNQI increases to 40 wt%, it shows excellent electromagnetic wave interference (EMI) shielding effectiveness (SE). Under the ultrathin thickness of 0.08 mm, its EMI SE exceeds 10 dB in the X‐band, and the maximum SE reaches 76.8 dB at 8.4 GHz. This research broadens the application scope of metal‐cyanoquinone complexes, and provides a new platform for the design and development of novel ultrathin electromagnetic protection materials.
We have recently found that organic conductors Ag(DR) 2 (DR = 2,5-disubsituted-N,N 0 -dicyanoquinone diimine; substituent (R) = CH 3 , Cl, Br, I) irreversibly vary their electrical and magnetic properties by UV irradiation. By selecting the irradiation conditions (wavelengths, temperature, atmosphere, duration), one can accurately control the physical properties from metallic to insulating behavior while retaining their crystal structures. In order to clarify the mechanism of the conductivity change in the case of R = Cl, Br, and I, structure analysis of the irradiated crystals has been carried out. Transmittance electron microscopy and X-ray single crystal structure analysis clarified that the Ag(DCl) 2 crystals after 72 h irradiation (375 nm) contained single crystals of nearly three-dimensionally ordered AgCl (0.9 in mole fraction) with varying dimensions (∼1-50 nm). Owing to such a unique hybrid crystal structure, a highly nonlinear current-voltage characteristic unlike any existing electronic devices is observed on irradiated single Ag(DCl) 2 crystals.
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