CN114671855B - Acridine ligand for photo-thermal material, cuprous iodide cluster-based coordination polymer with photo-thermal property, and preparation method and application thereof - Google Patents

Acridine ligand for photo-thermal material, cuprous iodide cluster-based coordination polymer with photo-thermal property, and preparation method and application thereof Download PDF

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CN114671855B
CN114671855B CN202210432107.8A CN202210432107A CN114671855B CN 114671855 B CN114671855 B CN 114671855B CN 202210432107 A CN202210432107 A CN 202210432107A CN 114671855 B CN114671855 B CN 114671855B
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cui
dpa
cluster
cuprous iodide
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CN114671855A (en
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王春琼
范鸿川
陈丹
曾彦波
孙浩巍
张轲
张晓伟
蔡洁云
秦世春
龙杰
魏佳
杨艺敏
张庆刚
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Yunnan tobacco quality supervision and inspection station
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    • C07D401/00Heterocyclic compounds containing two or more hetero rings, having nitrogen atoms as the only ring hetero atoms, at least one ring being a six-membered ring with only one nitrogen atom
    • C07D401/14Heterocyclic compounds containing two or more hetero rings, having nitrogen atoms as the only ring hetero atoms, at least one ring being a six-membered ring with only one nitrogen atom containing three or more hetero rings
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Abstract

A cuprous iodide cluster-based coordination polymer with photo-thermal property, a preparation method and application thereof, wherein CuI and 2, 7-di (pyridine-4-yl) acridine are mixed with a solvent to obtain the cuprous iodide cluster-based coordination polymer. The synthesized ligand DPA is utilized, and the alpha-, beta-and gamma-CuI-DPA with different space topological structures can be prepared by only adjusting the proportion of metal and ligand, and the synthesized three cuprous iodide cluster-based coordination polymers are used for the first time, so that CPs with different space topological structures are built on the basis of the same molecular block for the first time; in synthetic gamma-CuI-DPA, there is rare [ Cu ] 2 I 2 ]The three-dimensional structure constructed by six links provides a charge transport channel for gamma-CuI-DPA, so that the conductivity and the photo-thermal conversion efficiency are higher than those of alpha-CuI-DPA and beta-CuI-DPA, and a foundation is laid for designing and preparing conductive CPs with metal ion chains.

Description

Acridine ligand for photo-thermal material, cuprous iodide cluster-based coordination polymer with photo-thermal property, and preparation method and application thereof
Technical Field
The invention relates to the technical field of functional materials, in particular to an acridine ligand for a photo-thermal material, a cuprous iodide cluster-based coordination polymer with photo-thermal property, a preparation method and application thereof.
Background
Coordination polymers (Coordination polymers, CPs) are self-assembled molecular assemblies, and can be assembled into one-dimensional, two-dimensional or three-dimensional networks through regulating metal ions, organic ligands and synthesis condition groups to obtain unique structures and functions, so that the high-crystallinity materials can be applied to gas adsorption, catalysis, sensors, biological imaging, optoelectronics and the like. Based on copper iodide clusters ([ CuI)] n ) Not only does the CPs of (1) produce a superior topology due to the multi-core structure, but also brings unique properties to the crystalline material such as luminescence, conductivity, and photocatalysis.
In the current research, the research group of Li designed and synthesized a series of inorganic-organic hybrid materials composed of [ Cu ] based on different ligands 4 I 4 ]One, two, three-dimensional expansions of the structure and a strong network. Lang's group constructed [ Cu-based ] in different solvent systems using the same ligand 1, 3-bis (4-pyridyl) propane 2 I 2 ]-and [ Cu ] 4 I 4 ]Is a CPs of (C). However, in the prior art, coordination polymers constructed based on different molecular blocks have never been reported for constructing CPs with different spatial topologies based on the same molecular block, which also hinders researchers from exploring the possibility of relationship between the structure and performance of different CuI-CPs with similar molecular components.
Disclosure of Invention
The invention aims to overcome the defect that the prior art lacks related researches on constructing CPs with different space topological structures based on the same molecular block, and provides an acridine ligand for a photo-thermal material, a cuprous iodide cluster-based coordination polymer with photo-thermal property, and a preparation method and application thereof.
The aim of the invention is achieved by the following technical scheme:
an acridine ligand for photo-thermal material is 2, 7-di (pyridine-4-yl) acridine.
A processing method of cuprous iodide cluster-based coordination polymer with photo-thermal property comprises the steps of mixing CuI and 2, 7-di (pyridine-4-yl) acridine with a solvent, heating to react, and cooling to obtain a solid, namely the cuprous iodide cluster-based coordination polymer.
Preferably, the molar ratio of the CuI to the 2, 7-di (pyridin-4-yl) acridine is 1:10-10:1.
Preferably, the reaction temperature is 120-150 ℃.
Preferably, the temperature is reduced to 18-50 ℃.
Preferably, the solvent is one or more of tetrahydrofuran, acetone, ethyl acetate, chloroform, ethanol, N-dimethylformamide and acetonitrile.
A cuprous iodide cluster-based coordination polymer with photothermal properties, comprising at least one of α -CuI-DPA, β -CuI-DPA, and γ -CuI-DPA.
Preferably, the cuprous iodide cluster-based coordination polymer is α -CuI-DPA when the molar ratio of CuI to 2, 7-bis (pyridin-4-yl) acridine is 1:1;
when the molar ratio of CuI to 2, 7-di (pyridin-4-yl) acridine is 2:1, the cuprous iodide cluster-based coordination polymer is beta-CuI-DPA;
when the molar ratio of CuI to 2, 7-bis (pyridin-4-yl) acridine is 4:1, the cuprous iodide cluster-based coordination polymer is gamma-CuI-DPA.
Use of cuprous iodide cluster-based coordination polymer with photo-thermal properties in photo-thermal imaging.
The invention has the following advantages:
1. the synthesized ligand 2, 7-di (pyridine-4-yl) acridine (DPA) is utilized, and the alpha-, beta-and gamma-CuI-DPA with different space topological structures can be prepared only by adjusting the proportion of metal and the ligand, so that the synthesized three cuprous iodide cluster-based coordination polymers are used for the first time, and CPs with different space topological structures are built based on the same molecular block for the first time.
2. In synthetic gamma-CuI-DPA, there is rare [ Cu ] 2 I 2 ]Six-linked three-dimensional structures, the unique chains provide charge transport channels for the gamma-CuI-DPA three-dimensional structure, resulting in conductivity (-10) -6 S m -1 ) And the light-heat conversion efficiency (. Eta.) 808nm And (23%) is higher than alpha-CuI-DPA and beta-CuI-DPA, and lays a foundation for designing and preparing conductive CPs with metal ion chains.
3. In addition, the synthesized gamma-CuI-DPA also has higher photo-thermal conversion efficiency, and plays an important role in promoting non-radiative migration and triggering photo-thermal conversion.
4. The technology related to constructing different CPs by using the same molecular block provides a potential research object for researching and analyzing the structure-performance relationship of the CPs, and also opens the way for synthesizing novel photo-thermal conversion CPs or conductive CPs.
Drawings
FIG. 1 shows a scheme for DPA synthesis.
Fig. 2 is a graph of copper iodide cluster-based coordination polymers (mode of attachment of asymmetric ligands to three cuis and spatial structure along the axis) formed in different proportions for CuI and DPA.
FIG. 3 is a view of the spatial structure of the α -CuI-DPA along (a) b-axis and (b) c-axis, and the laminate (c).
Fig. 4 is a PXRD analysis and comparison chart.
PXRD analysis of samples reacted in different CuI-DPA proportions; c-d simulation of alpha-, beta-, and gamma-CuI-DPA and comparison of experimental PXRD results.
Fig. 5 is a view of the spatial structure of β -CuI-DPA along (a) b-axis and (b) c-axis, and the stack (c).
Fig. 6 is a view of the spatial structure of γ -CuI-DPA along (a) b-axis and (b) c-axis, and stacked layers (c).
Fig. 7 is an X-ray diffraction (PXRD) analysis of three synthetic powders.
FIG. 8 is a schematic diagram of the gamma-CuI-DPA production and conversion process.
(a) The structure of gamma-CuI-DPA can be seen as three chains interwoven together; (b) a simplified three-dimensional spatial structure; (c) interconversion patterns between three CPs.
FIG. 9 FT-IR (a) and Raman spectra (b) of DPA and three CPs
FIG. 10 shows variable temperature PXRD (a-c) and thermogravimetric analysis (d) of alpha-, beta-and gamma-CuI-DPA
Fig. 11 is a PXRD analysis used to study solvent stability. (a) alpha-CuI-DPA, (b) beta-CuI-DPA and (c) gamma-CuI-DPA
FIG. 12 is a graph showing performance testing of three CPs.
(a) Ultraviolet-visible-near infrared solid absorption spectra of three CPs and reactants (DPA and CuI); (b) Photocurrent response, (c) I-V plot and (d) energy level plot of α -, β -and γ -CuI-DPA. (e) Photothermal conversion curve of CPs powder during three cycles of heating and cooling (806 nm,1.0Wcm -2 10 mg). (f) Near infrared laser (806 nm,1.5 Wcm) -2 ,0.2mL,50mgmL -1 ) The photothermal reaction to the aqueous CPs suspension is followed by turning off the laser.
FIG. 13 shows the application of three CPs in photothermography
(a) An optical camera photograph; (b-d) photothermographic photographs (α -CuI-DPA on the outside and γ -CuI-DPA on the inside); (b) no illumination; (c) a xenon lamp light source; (d) a xenon lamp source with a 750nm long pass filter.
Detailed Description
For the purpose of making the objects, technical solutions and advantages of the embodiments of the present invention more apparent, the technical solutions of the embodiments of the present invention will be clearly and completely described below with reference to the accompanying drawings in the embodiments of the present invention, and it is apparent that the described embodiments are some embodiments of the present invention, but not all embodiments. The components of the embodiments of the present invention generally described and illustrated in the figures herein may be arranged and designed in a wide variety of different configurations.
Thus, the following detailed description of the embodiments of the invention, as presented in the figures, is not intended to limit the scope of the invention, as claimed, but is merely representative of selected embodiments of the invention. All other embodiments, based on the embodiments of the invention, which are apparent to those of ordinary skill in the art without inventive faculty, are intended to be within the scope of the invention.
In addition, the embodiments of the present invention and the features of the embodiments may be combined with each other without collision.
It should be noted that: like reference numerals and letters denote like items in the following figures, and thus once an item is defined in one figure, no further definition or explanation thereof is necessary in the following figures.
General materials and methods
All reagents were purchased from energy chemical industry (Shanghai, china) and used as such unless otherwise indicated. Nuclear magnetic resonance spectra were recorded using an AVANCED RX400 nuclear magnetic resonance spectrometer (Bruker, germany) operating at 400 MHz. High Resolution Mass Spectrometry (HRMS) was measured by an Agilent 6540Q-TOF mass spectrometer (Agilent, usa). Fourier transform infrared (FT-IR) spectrum is obtained by using a Thermo Nicolet spectrometer and KBr particles (Thermo Nicolet 365) at 4000-400cm -1 Recorded in range. The Raman spectrum is 2000-200cm -1 Using high resolution in the range of (2)The evolution instrument (LABRAM HR EVO, horiba, japan) was recorded under laser excitation at 633 nm. TGA was performed under an N2 atmosphere using a Mettler-Toledo 1600LF instrument with a heating rate of 10deg.C/min -1 . The PXRD structure was prepared by Smartlab SE X-ray diffractometer (Rigaku, japan) with Cu K at 40kV and 200mA α Radiation shooting, scanning speed of 20 DEG min -1 The step size is 0.02 °. The specific surface area was measured by the BET method using nitrogen adsorption/desorption at 77K.
Example 1:
the embodiment provides a processing method of a cuprous iodide cluster-based coordination polymer with photo-thermal property, which comprises the steps of mixing CuI and ligand 2, 7-di (pyridine-4-yl) acridine with a solvent, heating to 120-150 ℃ for reaction, and then cooling to below 50 ℃, wherein the temperature is preferably 18-25 ℃ at room temperature, and the precipitated solid is the cuprous iodide cluster-based coordination polymer, wherein the cuprous iodide cluster-based coordination polymer comprises at least one of alpha-CuI-DPA, beta-CuI-DPA and gamma-CuI-DPA; wherein the solvent is one or more of tetrahydrofuran, acetone, ethyl acetate, chloroform, ethanol, N-dimethylformamide and acetonitrile, preferably N, N-dimethylformamide and acetonitrile; the molar ratio of CuI to 2, 7-di (pyridin-4-yl) acridine is 1:10-10:1:
when the molar ratio of CuI to 2, 7-di (pyridin-4-yl) acridine is 1:1, the cuprous iodide cluster-based coordination polymer is alpha-CuI-DPA;
when the molar ratio of CuI to 2, 7-di (pyridin-4-yl) acridine is 2:1, the cuprous iodide cluster-based coordination polymer is beta-CuI-DPA;
when the molar ratio of CuI to 2, 7-bis (pyridin-4-yl) acridine is 4:1, the cuprous iodide cluster-based coordination polymer is gamma-CuI-DPA.
Example 2:
synthesis of novel ligand 2, 7-di (pyridin-4-yl) acridine (DPA)
Ligand DPA is synthesized by suzuki coupling, and the specific scheme is shown in figure 1:
(1) a solution of benzyltriethylammonium bromide (TEBA, 12 g, 44 mmol) in methanol (100 ml) was added to acridine (2.16 g, 12 mmol). The reaction was then stirred at 60℃for 16 hours with a reflux condenser. After cooling to room temperature, the crude product was filtered and washed with a small amount of pyridine and dichloromethane. After evaporation in vacuo at 50℃2, 7-dibromoacridine was obtained as a pale yellow solid.
(2) 2, 7-dibromoacridine (0.67 mg, 2.0 mmol), pyridine-4-boronic acid (0.59 g, 2.4 mol), csF (2.8 g, 18 mmol) and Pd (PPh) 3 ) 4 (0.130 g, 0.12 mmol) in dimethoxymethane (40 ml) in N 2 Stirring for 3 days at 90℃under an atmosphere. And the crude product was purified by chromatography (methanol/chloroform=1:50) to give a yellow powder (0.3 g, yield 45%).
Example 3:
synthesis of novel CuI-DPA
(1) Let 1 through CuI and DPA: 1 to synthesize alpha-CuI-DPA. CuI (0.012 g, 0.06 mmol) and DPA (0.019 g, 0.06 mmol) were added to a solution of N, N "-dimethylformamide (DMF, 4 ml) and acetonitrile (4 ml). The mixture was stirred at room temperature for several minutes, then poured into a 25 ml teflon lined stainless steel vessel, heated to 120 ℃ for 48 hours, cooled to room temperature, and after which the red bulk crystals were collected, yield: 56% based on CuI.
(2) The ratio of CuI to DPA was 2:1 to synthesize beta-CuI-DPA. CuI (0.024 g, 0.12 mmol) and DPA (0.019 g, 0.06 mmol) were added to a solution of DMF (4 ml) and acetonitrile (4 ml). The mixture was stirred at room temperature for several minutes, then poured into a 25 ml teflon lined stainless steel vessel, heated to 120 ℃ for 48 hours, cooled to room temperature and the dark red rod-like crystals collected. Yield: 58% based on CuI.
(3) The ratio of CuI to DPA was 4:1 to synthesize gamma-CuI-DPA. CuI (0.24 g, 0.12 mmol) and DPA (0.010 g, 0.03 mmol) were added to a solution of DMF (4 ml) and acetonitrile (4 ml). The mixture was stirred at room temperature for several minutes, then poured into a 25 ml teflon lined stainless steel vessel, heated to 150 ℃ for 48 hours, cooled to room temperature and the brown bulk crystals collected. Yield: 57% based on CuI.
The solvent in this embodiment is a mixture of N, N '-dimethylformamide and acetonitrile, and may be replaced by N, N' -dimethylformamide or acetonitrile or other solvents, and the total amount of the solvent may be 2 mL, 4 mL, 6 mL, 8 mL, 10 mL, 12 mL, 14 mL, 16 mL, 18 mL or more, and the reactant in the preferred system is 3-4.5 mg/mL, and the different concentrations of the reactant and the product may affect the reaction rate and the collection difficulty of the product. The heating time in this example is preferably 24 to 60 hours in consideration of the yield of the product, the balance of the reaction, and the continuous conversion between the various crystal forms of the product in the system.
1 test and characterization of cuprous iodide Cluster-based coordination Polymer
1.1 Crystal Structure
The ratio of metal to ligand, solvent environment, bridging ligand and counter anion structure, and even numerous factors such as reaction temperature and pH will result in (CuI) n The difference in clusters means that when CuI-based complexes are synthesized, a slight difference may result in the formation of different derivatives. In this study, therefore, various synthesis conditions were explored to selectively obtain pure compounds. A high quality single crystal suitable for single crystal X-ray diffraction analysis was obtained by solvothermal method in a mixed solvent of acetonitrile and DMF. Table 1 lists the main crystallographic data of all CPs. Different synthesis ratios of CuI and DPA lead to [ Cu ] with different coordination modes 2 I 2 ]Based on a structure, i.e. based on analogous [ Cu ] 2 I 2 ]1-dimensional, 2-dimensional, 3-dimensional CPs (1D-, 2D-, and 3D-CPs) of structures and DPA ligands, see in particular FIG. 2.
TABLE 1 crystallographic data of CPs
FIGS. 2 and 3 show the single crystal X-ray diffraction structure of alpha-CuI-DPA and show that alpha forms a 1D structure at P2 1 Crystallization in n space group. The asymmetric unit comprises one DPA molecule and half of [ Cu ] 2 I 2 ]Structure is as follows. Adjacent [ Cu ] 2 I 2 ]The structure is linked by two DPA ligands. [ Cu ] 2 I 2 ]The structure shows planar four coordination and is attached to the pyridinyl-N of DPA. However, acridine-N in DPA is uncoordinated, DPA ligands are linked as banana-like binary ligands [ Cu2I2]And (3) forming a one-dimensional extension chain. While chains are stacked together by weak interactions at a distance of 3.5The sliding distance is 7.5 +.>The layers are formed in one direction as in fig. 4, and then the layers are stacked to form alpha crystals with an angle of 52.3 deg. between them.
Structural analysis of beta-CuI-DPA shows that a two-dimensional coordination network is formed and at P2 1 Crystallization in n space group as shown in FIGS. 2 and 5. While the asymmetric unit comprises one [ Cu ] 2 I 2 ]A structure and a DPA ligand. Unlike α, [ Cu ] in β 2 I 2 ]The structure shows a three-coordinate, whereas DPA is also a three-plane coordinate. [ Cu ] due to steric hindrance of acridine-N in DPA 2 I 2 ]One Cu (I) in the structure is singly coordinated to acridine-N via a Cu-N bond, while the other Cu (I) is linked to two pyridyl-N groups of the DPA ligand. Thus, a three-connection [ Cu ] 2 I 2 ]Is linked to three DPA ligands, extending to form a planar two-dimensional network. Adjacent layers are antiparallel at a distance of 3.6Beta crystals are formed as shown in figure 4.
gamma-CuI-DPA crystallizes in the P-1 space group and the coordination appears to be more complex, see fig. 2 and 6. Likewise, [ Cu ] can be observed 2 I 2 ]SBUs, but coordinate in a three-dimensional six-way rather than planar. I atoms not only co-ordinating with Cu (I) to form [ Cu ] 2 I 2 ]SBUs, and also joined by another Cu (I) (Cu 4) to form [ (Cu) 2 I 2 )Cu]A chain. And [ Cu ] 2 I 2 ]Cu (I) (Cu 1 andcu 5) is connected to DPA with pyridinyl-N. [ Cu ] 4 (CN) 4 ]Two Cu (I) (Cu) 2 And Cu 3 ) The three chains together form a three-dimensional gamma crystal linked to DPA with acridinyl-N, as shown in FIG. 4.
1.2 interconversion
Three stable phases were found during the synthesis in the metal ligand ratio range from 1:10 to 10:1 according to powder X-ray diffraction (PXRD) analysis, see (a) in fig. 7. Further screening gave an optimal CuI-to-DPA ratio of 1: 1. 2:1 and 4:1 and the resulting samples were designated α -CuI-DPA, β -CuI-DPA and γ -CuI-DPA, respectively. The PXRD pattern showed that the CPs as synthesized were pure phase, as was the case with the simulated patterns of these three CPs, see (b) - (c) in fig. 7. As shown in FIG. 8, when the same amount of CuI was added to the α -CuI-DPA in DMF/acetonitrile reaction mixture and the reaction system was subjected to additional solvothermal treatment, β -CuI-DPA was produced, as demonstrated by the PXRD structure, as shown in FIG. 9. This means that α -CuI-DPA can be converted to β -CuI-DPA. Further experiments confirm successful interconversions between α -, β -and γ -CuI-DPA. Furthermore, these results indicate that interconversion can occur between CuI or DPA when they are added precisely to achieve ratios that meet the conditions for formation of another CPs in the α -, β -or γ -CuI-DPA system.
1.3 characterization
The CPs obtained in FIG. 9 were characterized by Fourier transform infrared (FT-IR) spectra, and the differences between CPs and DPA in FT-IR spectra showed coordination effects. As for Raman spectroscopy, the complexation effect was also further confirmed.
The thermal stability of these CPs was studied by temperature swing PXRD and thermogravimetric analysis (TGA) as shown in figure 10. The alpha-, beta-and gamma-CuI-DPA all show good thermal stability. Meanwhile, we tested the solvent stability in various common solvents, and the results are shown in fig. 11. CPs were soaked in different solvents for three days, and the PXRD patterns of alpha-and gamma-CuI-DPA soaked in different solvents were not significantly changed, indicating good solvent stability. However, the PXRD pattern for β -CuI-DPA varies slightly in some solvents and can be recovered after soaking in DMF.
The UV-Vis-NIR absorption of CuI-DPA CPs becomes more intense than the ligand, the absorption range produces a red shift with intense visible light absorption. As shown in FIG. 12 (a), the diffuse reflectance spectrum shows that the absorption of CuI and DPA is mainly in the ultraviolet region (270-410 nm), while the absorption of CuI is also strong in the near infrared (1700 nm). The near infrared absorption of gamma-CuI-DPA is stronger and wider than that of beta-CuI-DPA, while alpha-CuI-DPA is the weakest of the three CPs. Alpha-and beta-CuI-DPA have strong absorption in the ultraviolet to visible region (220-570-nm).
1.4 Electrical Properties
Among materials formed from inorganic and organic components, electrical conduction is well understood, but their combination to produce a conductive CPs network is an emerging, rapidly evolving field of research. As shown in FIGS. 12 (b) - (c), the strongest photocurrent response of gamma-CuI-DPA (-0.5. Mu.A cm) -2 ) And the highest conductivity (-10-6S m) -1 ) Meaning that more free charge carriers are generated under illumination and electron transport is easier. For alpha-and beta-CuI-DPA they show a weak photocurrent response (0.1-0.15. Mu.A cm -2 ) And low conductivity (-10-8S m) -1 ). These results indicate that three-dimensional gamma-CuI-DPA has better photocurrent response and conductivity than one-dimensional alpha-and two-dimensional beta-CuI-DPA. As shown in (d) of fig. 12, HOMO levels of the three CPs do not change much, and LUMO levels vary with different topologies of CPs. gamma-CuI-DPA enjoys the narrowest electronic bandgap (eg=1.40 eV) and lowest LUMO level (elumo= -3.34 eV), whereas alpha-and beta-CuI-DPA exhibit wider electronic bandgaps (eg=1.90 eV and 1.65 eV) and higher LUMO levels (elumo= -3.07eV and-2.97 eV).
1.5 photothermal conversion
Light-to-heat conversion materials have attracted increasing attention over the last decades, and many such materials have been utilized by scientists. Planar DPA stacks in CuI-DPA CPs networks with varying degrees of non-covalent interactions have been pointed out as important factors in promoting non-radiative migration and initiating photothermal conversion. However, these three CPs consisting of two luminescent components, DPA and CuI, do not show a range from visible to visible under UV or visible light irradiationNear infrared emission. Therefore, cuI-DPA has the potential as a photothermal material. As shown in FIG. 12 (e), the photothermal conversion curve of these CPs powders after three heating and cooling cycles directly shows that the CuI-DPA powder was laser-irradiated at 808nm (1.0W cm) -2 ) Lower photo-thermal capability. Under near infrared irradiation, the temperatures of α -, β -and γ -CuI-DPA rise rapidly from room temperature (22 ℃) and stabilize at 68 ℃, 118 ℃ and 183 ℃ respectively in 180 seconds. For further quantitative comparison, the photothermal conversion efficiency of the aqueous dispersion was measured using water as a heat conducting medium. The temperature of the dispersion of these CPs (10 mg dispersed in 0.2 ml water) was increased under irradiation with 808nm laser light. According to the cooling curve at the time of turning off the laser, as in (f) of fig. 12, α -CuI-DPA shows a small temperature rise (Δt=10.4 ℃, from 21.0 to 31.4 ℃) corresponding to 8.6% of the photothermal conversion efficiency, whereas β -CuI-DPA has a slightly higher temperature rise (Δt=15.1 ℃, from 21.0 to 36.1 ℃) of the photothermal conversion efficiency of 11.5%. Interestingly, γ -CuI-DPA showed a significant temperature rise (Δt=53.1 ℃, from 21.0 ℃ to 74.1 ℃) with a corresponding photo-thermal conversion efficiency of 23.9%.
Example 4:
application of
These CPs with photothermal conversion characteristics are potential photothermal agents and can be applied to photothermal imaging. Photothermal imaging is lossless, with higher imaging resolution and deeper imaging penetration than optical imaging. We produced Chinese tobacco LOGO with α -and γ -CuI-DPA, respectively. And light of different wavelengths is used to illuminate the letter structure through Xe lamps with different optical filters. Corresponding to their absorption spectra, α -and γ -CuI-DPA have strong absorption in the visible light band, and show indistinguishable brightness in photothermal images, as in (b) of fig. 13. When irradiated with visible light, both portions have luminance which is difficult to distinguish in a photothermal image, as in (c) - (d) in fig. 13. When irradiated with near infrared light, a clear pattern appears on the round card, as shown in fig. 13 (a). Therefore, under the light irradiation of different wavelengths, the photothermal conversion imaging can be realized through the photothermal conversion.
Although the present invention has been described with reference to the foregoing embodiments, it will be apparent to those skilled in the art that modifications may be made to the embodiments described, or equivalents may be substituted for elements thereof, and any modifications, equivalents, improvements and changes may be made without departing from the spirit and principles of the present invention.

Claims (4)

1. A processing method of a cuprous iodide cluster-based coordination polymer with photo-thermal property is characterized in that: mixing CuI and 2, 7-di (pyridine-4-yl) acridine with a solvent, heating to 120-150 ℃ for reaction, and cooling to 18-50 ℃ to obtain a solid which is the cuprous iodide cluster-based coordination polymer;
the molar ratio of the CuI to the 2, 7-di (pyridine-4-yl) acridine is 1:1-4:1;
the solvent is a mixture of N, N-dimethylformamide and acetonitrile.
2. A cuprous iodide cluster-based coordination polymer having photothermal properties obtained by the processing method of claim 1, characterized in that: comprisingα-CuI-DPA、β-CuI-DPA andγ-at least one of CuI-DPA;
α-CuI-DPA has the formula C 92 H 60 Cu 4 I 4 N 12 Monoclinic system with space group ofP2 1 /nUnit cell parametersabc8.3613 (3) A, 8.0390 (3) A, 28.8292 (11) A, respectively,αβγ90 DEG, 94.162 (2) DEG, 90 DEG respectively,Z=1;
β-CuI-DPA has the formula C 23 H 15 Cu 2 I 2 N 3 ·C 3 H 7 NO, monoclinic system, space groupP2 1 /cUnit cell parametersabc13.5613 (12) a, 19.2762 (17) a, 10.1201 (9) a, respectively,αβγ90 DEG, 101.918 (3) DEG, 90 DEG respectively,Z=4;
γ-CuI-DPA has the formula C 99.39 H 66 Cu 12 I 4.61 N 19.39 O 3 Triclinic system with space group ofPUnit cell parametersabc9.3687 (6) a, 13.5498 (8) a, 18.5065 (13) a, respectively,αβγ83.599 (2) °, 75.059 (2) °, 87.748 (2) °, respectively,Z=1。
3. the cuprous iodide-based coordination polymer with photothermal properties according to claim 2, wherein:
the molar ratio of the CuI to the 2, 7-di (pyridine-4-yl) acridine is 1:1, and the cuprous iodide cluster-based coordination polymer isα-CuI-DPA;
The molar ratio of the CuI to the 2, 7-di (pyridine-4-yl) acridine is 2:1, and the cuprous iodide cluster-based coordination polymer isβ-CuI-DPA;
The molar ratio of the CuI to the 2, 7-di (pyridine-4-yl) acridine is 4:1, and the cuprous iodide cluster-based coordination polymer isγ-CuI-DPA。
4. Use of a cuprous iodide cluster-based coordination polymer having photothermal properties as claimed in claim 2 or 3 in photothermal imaging.
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