CN114890914B - High-efficiency red light emitting organic crystal and application thereof in low-temperature fluorescence sensing - Google Patents

High-efficiency red light emitting organic crystal and application thereof in low-temperature fluorescence sensing Download PDF

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CN114890914B
CN114890914B CN202210352303.4A CN202210352303A CN114890914B CN 114890914 B CN114890914 B CN 114890914B CN 202210352303 A CN202210352303 A CN 202210352303A CN 114890914 B CN114890914 B CN 114890914B
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卢革宇
王晨光
代佳男
刘方猛
孙鹏
闫旭
刘晓敏
贾晓腾
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Abstract

The invention discloses an organic high-efficiency red light emitting organic crystal with linear response to extremely low temperature and application thereof in low-temperature fluorescence sensing, belonging to the technical field of temperature sensing. The invention obtains a strong red light emitting organic crystal by a solvent volatilization method, the maximum emission wavelength of the crystal is 693nm, the fluorescence quantum efficiency is up to 73 percent, and the structural formula is shown as the formula (I). The invention also discloses application of the crystal emitting red light in low-temperature fluorescence sensing. Experiments prove that the maximum emission wavelength of the crystal has good linear response to extremely low temperature which is difficult to measure under the traditional condition, can sensitively react to temperature change at the extremely low temperature, and has wide application prospect in the aspect of low-temperature fluorescence sensing.
Figure DDA0003581176770000011

Description

一种高效率红光发射的有机晶体及其在低温荧光传感中的 应用An organic crystal with high-efficiency red light emission and its application in low-temperature fluorescence sensing application

技术领域technical field

本发明属于温度传感技术领域,具体涉及一种高效率红光发射的有机晶体及其在低温荧光传感中的应用。The invention belongs to the technical field of temperature sensing, and in particular relates to an organic crystal emitting red light with high efficiency and its application in low-temperature fluorescence sensing.

背景技术Background technique

温度作为重要的基本热力学参数之一,与人们的生产生活息息相关,如何实现对不同条件下包括极限环境下的温度准确测量,一直是我们必须解决的问题。传统的温度测量原理是根据与温度相关的体积、电导和电阻变化来衡量温度的数值,但是从实际应用的角度,基于该原理所开发的温度测量仪器并不能很好的满足微机电系统、海洋研究和航空工业等行业所需的原位测量。因此,开发出适用于极限环境下可对温度进行原位测量的温度传感器具有非常广阔的应用前景。As one of the important basic thermodynamic parameters, temperature is closely related to people's production and life. How to achieve accurate temperature measurement under different conditions, including extreme environments, has always been a problem that we must solve. The traditional temperature measurement principle is to measure the value of temperature according to the temperature-related volume, conductance and resistance changes, but from the perspective of practical application, the temperature measurement instrument developed based on this principle cannot meet the needs of micro-electromechanical systems, oceans, etc. In-situ measurements required by industries such as research and the aerospace industry. Therefore, the development of temperature sensors suitable for in-situ temperature measurement in extreme environments has very broad application prospects.

由于一些对温度敏感的荧光材料可以很好的响应温度变化,所以基于荧光响应的温度传感器正不断被开发出来去精确的检测温度。目前研究者的兴趣主要集中在对温度敏感的发光有机染料、聚合物、纳米晶体和镧系材料等材料的开发上,但上述材料在对极限条件下尤其是对极低温度的测量上的表现显得有些差强人意。由于稀土金属的高价格和低溶解度,聚合物、纳米晶体操作的复杂性,我们把目光集中在对温度敏感的发光有机染料小分子上,目前报道的有机染料荧光传感大多数是在溶液、聚合物掺杂薄膜中进行温度测量,在极低温度下上述溶液、聚合物掺杂薄膜会因凝固、冻裂无法对温度进行有效测量。因此,迫切地需要一种可对极低温度进行测量的有机发光小分子荧光传感器。Because some temperature-sensitive fluorescent materials can respond well to temperature changes, temperature sensors based on fluorescent responses are being developed to detect temperature accurately. At present, researchers' interests are mainly focused on the development of materials such as temperature-sensitive luminescent organic dyes, polymers, nanocrystals and lanthanide materials, but the performance of these materials under extreme conditions, especially at extremely low temperatures It seems a little unsatisfactory. Due to the high price and low solubility of rare earth metals, the complexity of polymer and nanocrystal operation, we focus on small molecules of luminescent organic dyes that are sensitive to temperature. Most of the organic dye fluorescence sensors reported so far are in solution, The temperature is measured in the polymer-doped film. At extremely low temperatures, the above-mentioned solutions and polymer-doped films cannot effectively measure the temperature due to solidification and freezing cracks. Therefore, there is an urgent need for an organic light-emitting small molecule fluorescent sensor that can measure extremely low temperatures.

发明内容Contents of the invention

针对现有低温传感材料的不足,本发明要解决的问题是提供一种高效率红光发射的有机晶体及其在低温荧光传感中的应用。Aiming at the deficiency of existing low-temperature sensing materials, the problem to be solved by the present invention is to provide an organic crystal with high-efficiency red light emission and its application in low-temperature fluorescence sensing.

Figure SMS_1
Figure SMS_1

本发明所述的高效率红光发射的有机晶体,其分子结构简单,合成步骤简洁,易于结晶,其是由式(I)所示化合物通过溶剂蒸发法制备得到,该化合物的规范命名为(2Z,2'Z)-3,3'-(2,5-双(二苯氨基)-1,4-亚苯基)双(2-(4-(二丁基氨基)苯基)丙烯腈)。The high-efficiency red light-emitting organic crystal of the present invention has simple molecular structure, simple synthesis steps, and is easy to crystallize. It is prepared from the compound represented by formula (I) by solvent evaporation. The standard name of the compound is ( 2Z,2'Z)-3,3'-(2,5-bis(diphenylamino)-1,4-phenylene)bis(2-(4-(dibutylamino)phenyl)acrylonitrile ).

式(I)所示化合物的制备反应式如下:The preparation reaction formula of compound shown in formula (I) is as follows:

Figure SMS_2
Figure SMS_2

针对现有低温荧光传感材料在检测极低温度方面的不足,本发明开发了具有较高荧光量子效率且可对极低温度进行准确测量的红光有机晶体。本发明中制备的红光有机晶体实现了较强的红光发射,这是非常难得的,因为绝大多数红光发射的荧光分子尤其是在晶体状态通常聚集诱导荧光淬灭大大降低了荧光量子效率,难以实现较强的红光发射。而本发明制备的高效红光有机晶体,因其特有结构在实现较强的红光发射的同时还可以对极低温度进行很好的测量。目前还很少有关于高效红光有机晶体实现低温精准测量的文献报道,正是由于上述优点,高效红光发射的有机晶体对极低温度的检测具有非常广阔的应用前景。Aiming at the shortcomings of the existing low-temperature fluorescent sensing materials in detecting extremely low temperatures, the present invention develops a red-light organic crystal with high fluorescence quantum efficiency and which can accurately measure extremely low temperatures. The red-light organic crystals prepared in the present invention achieve strong red-light emission, which is very rare, because most of the red-light-emitting fluorescent molecules, especially in the crystal state, usually aggregate to induce fluorescence quenching, which greatly reduces the fluorescence quantum efficiency, it is difficult to achieve strong red emission. However, the high-efficiency red-light organic crystal prepared by the present invention, because of its unique structure, can achieve very good measurement of extremely low temperatures while achieving strong red light emission. At present, there are few literature reports on high-efficiency red light-emitting organic crystals for precise low-temperature measurement. Due to the above advantages, high-efficiency red light-emitting organic crystals have very broad application prospects for extremely low temperature detection.

实验结果证实,本发明所述的对极低温度敏感的红光有机晶体,因其结构特异性,实现了高效率红光发射,并且因该有机分子的易结晶性,非常容易得到高效率红光有机晶体。该晶体克服了有机染料在溶液、薄膜状态下无法精准测量极低温度的不足,这为有机染料在低温传感领域提供了一个强有力的工具,更重要的是该晶体的设计思路能够为高效红光晶体以及极低温度传感的设计提供一个通用的指导。Experimental results confirm that the ultra-low temperature-sensitive red light organic crystals of the present invention realize high-efficiency red light emission due to their structural specificity, and it is very easy to obtain high-efficiency red light due to the easy crystallization of the organic molecules. Optical organic crystals. The crystal overcomes the inability of organic dyes to accurately measure extremely low temperatures in the state of solution and thin film, which provides a powerful tool for organic dyes in the field of low-temperature sensing, and more importantly, the design of the crystal can be used for efficient Red light crystals and extremely low temperature sensing designs provide a general guideline.

总之,本发明所述的极低温传感材料是一种全新的红光有机晶体,与其它温度传感材料相比,该晶体不需要多余的制备过程,能实现高效红光发射,比较容易检测到光学信号的变化,最大发射波长对于传统条件下难以测量的极度低温具有很好的线性响应,在极低温度下可以灵敏的反应温度变化。鉴于上述优点,其在低温荧光传感方面的应用具有广阔前景。In a word, the ultra-low temperature sensing material described in the present invention is a brand-new red light organic crystal. Compared with other temperature sensing materials, the crystal does not require redundant preparation process, can realize high-efficiency red light emission, and is relatively easy to detect To the change of the optical signal, the maximum emission wavelength has a good linear response to the extremely low temperature that is difficult to measure under traditional conditions, and can sensitively respond to temperature changes at extremely low temperatures. In view of the above advantages, its application in low-temperature fluorescence sensing has broad prospects.

附图说明Description of drawings

图1:本发明实施例1中制备的有机荧光染料晶体的核磁氢谱;Fig. 1: the nuclear magnetic hydrogen spectrum of the organic fluorescent dye crystal prepared in the embodiment 1 of the present invention;

图2:本发明实施例1中制备的有机荧光染料晶体的核磁碳谱;Fig. 2: the carbon nuclear magnetic spectrum of the organic fluorescent dye crystal prepared in the embodiment 1 of the present invention;

图3:本发明实施例1中制备的有机荧光染料晶体的吸收(a)和发射光谱 (b);表明该晶体的最大发射波长为693nm,荧光量子效率高达73%;Figure 3: Absorption (a) and emission spectrum (b) of the organic fluorescent dye crystal prepared in Example 1 of the present invention; show that the maximum emission wavelength of the crystal is 693nm, and the fluorescence quantum efficiency is as high as 73%;

图4:本发明实施例1中制备的有机荧光染料晶体的结构解析图;表明所得晶体为三斜晶系;Figure 4: Structural analysis diagram of the organic fluorescent dye crystal prepared in Example 1 of the present invention; it shows that the obtained crystal is a triclinic crystal system;

图5:本发明实施例1中制备的有机荧光染料晶体在日光(a)和365nm紫外灯(b)下的光学照片;说明了该晶体的易结晶性(- 图 5 中的 a )和高效红光发光性质 (- 图 5中的 b );Fig. 5: Optical photo of the organic fluorescent dye crystal prepared in Example 1 of the present invention under sunlight (a) and 365nm ultraviolet lamp (b); illustrates the easy crystallization (a in- Fig. 5) and high efficiency of the crystal Red light emitting properties (- b in Figure 5);

图6:本发明实施例1中制备的有机荧光染料晶体在77~295K的荧光光谱曲线(-图 6 中的 a 、- 图 6 中的 b )及665nm和697nm处荧光强度的比值与温度变化的关系曲线(- 图 6 中的 c );Fig. 6: Fluorescence spectrum curve (a in Fig. 6, b in Fig. 6) and the ratio of fluorescence intensity at 665nm and 697nm at 77 to 295K of the organic fluorescent dye crystal prepared in Example 1 of the present invention and the temperature change The relationship curve (- c in Figure 6);

具体实施方式Detailed ways

实施例1:(2Z,2'Z)-3,3'-(2,5-双(二苯氨基)-1,4-亚苯基)双(2-(4-(二丁基氨基) 苯基)丙烯腈)的合成Example 1: (2Z,2'Z)-3,3'-(2,5-bis(diphenylamino)-1,4-phenylene)bis(2-(4-(dibutylamino) Synthesis of phenyl)acrylonitrile)

向双口烧瓶中加入2-(4-(二丁基氨基)苯基)乙腈(153mg 0.626mmol),2,5- 双(二苯基氨基)对苯二甲醛(117mg,0.250mmol),叔丁醇钾(71mg,0.63mmol) 和四丁基氢氧化铵(214mg,0.63mmol),再加入10mL叔丁醇和5mL四氢呋喃作为溶剂,并将所得混合物在50℃下搅拌4h。冷却至室温后,将混合物倒入 50mL甲醇中,过滤沉淀物并通过硅胶色谱法进一步纯化,得到177mg(0.200 mmol,77%)产物,为红黑色固体,即(2Z,2'Z)-3,3'-(2,5-双(二苯氨基)-1,4-亚苯基) 双(2-(4-(二丁基氨基)苯基)丙烯腈)。Add 2-(4-(dibutylamino)phenyl)acetonitrile (153mg 0.626mmol), 2,5-bis(diphenylamino)terephthalaldehyde (117mg, 0.250mmol) to the two-necked flask, tert Potassium butoxide (71mg, 0.63mmol) and tetrabutylammonium hydroxide (214mg, 0.63mmol), and 10mL of tert-butanol and 5mL of tetrahydrofuran were added as solvents, and the resulting mixture was stirred at 50°C for 4h. After cooling to room temperature, the mixture was poured into 50 mL of methanol, and the precipitate was filtered and further purified by silica gel chromatography to obtain 177 mg (0.200 mmol, 77%) of the product as a red-black solid, namely (2Z,2'Z)-3 ,3'-(2,5-bis(diphenylamino)-1,4-phenylene)bis(2-(4-(dibutylamino)phenyl)acrylonitrile).

取10mg该产物放置在试管中,加入5mL二氯甲烷完全溶解该化合物,在二氯甲烷溶剂层上缓慢加入10mL的石油醚溶剂,使二氯甲烷和石油醚分层,用棉花封住试管口,通过溶剂挥发得到红光有机晶体。1H NMR(400MHz,CDCl3): δ7.86(s,2H),7.30–7.26(m,7H),7.25(s,3H),7.09(t,12H),6.97(t,J=7.3Hz,4H),6.46(d,J=8.5Hz,4H),3.24(t,8H),1.55–1.47(m,8H),1.39–1.26(m,8H),0.96(t, 12H).13C NMR(101MHz,CDCl3):δ148.65,147.62,143.24,134.33,132.72,129.54, 129.41,127.08,122.65,122.49,120.63,117.56,113.88,111.16,50.64,29.34,20.28,13.96。晶体中晶胞参数a=8.4810(3),b=11.4818(5),c=14.0570(6),α= 89.7366(15),β=87.7218(16),γ=86.1781(15),三斜晶系。图1、图2、图4及上述数据表明得到了所述结构产物。Take 10 mg of the product and place it in a test tube, add 5 mL of dichloromethane to completely dissolve the compound, slowly add 10 mL of petroleum ether solvent on the dichloromethane solvent layer to separate layers of dichloromethane and petroleum ether, and seal the test tube mouth with cotton , red light organic crystals were obtained by solvent evaporation. 1 H NMR (400MHz, CDCl3): δ7.86(s,2H),7.30–7.26(m,7H),7.25(s,3H),7.09(t,12H),6.97(t,J=7.3Hz, 13 C NMR (101MHz, CDCl3): δ148.65, 147.62, 143.24, 134.33, 132.72, 129.54, 129.41, 127.08, 122.65, 122.49, 120.63, 117.56, 113.88, 111.16, 50.64, 29.38, 13.9 The unit cell parameters in the crystal are a=8.4810(3), b=11.4818(5), c=14.0570(6), α=89.7366(15), β=87.7218(16), γ=86.1781(15), triclinic Tie. Figure 1, Figure 2, Figure 4 and the above data show that the product of the structure is obtained.

实施例2:实施例1中制备的有机晶体的吸收、发射光谱的测量Embodiment 2: the measurement of the absorption of the organic crystal prepared in embodiment 1, emission spectrum

将实施例1得到的晶体分散在硫酸钡基底上,用紫外-可见分光光度计在300~900nm波段扫描得到吸收光谱。用荧光光谱仪在405nm激发下扫描得到荧光发射光谱,用Origin软件将两组数据做图,得到如图3所示的有机晶体的吸收 -发射光谱(左侧部分为吸收光谱,右侧部分为发射光谱)。说明了红光有机晶体的吸收-发射峰位以及它的大斯托克斯位移。The crystals obtained in Example 1 were dispersed on the barium sulfate substrate, and the absorption spectrum was obtained by scanning in the 300-900 nm band with a UV-visible spectrophotometer. Use a fluorescence spectrometer to scan under 405nm excitation to obtain the fluorescence emission spectrum, and use the Origin software to map the two groups of data to obtain the absorption-emission spectrum of the organic crystal as shown in Figure 3 (the left part is the absorption spectrum, and the right part is the emission spectrum. spectrum). The absorption-emission peak position and its large Stokes shift of the red organic crystal are illustrated.

实施例3:实施例1中制备的有机晶体的变温(77~295K)荧光测试Embodiment 3: Fluorescence test of the variable temperature (77~295K) of the organic crystal prepared in embodiment 1

对实施例1得到的晶体进行制样,放置于装样品的腔中,在降温装置中倒入77K的液氮,使用375nm LED激发光源对晶体样品进行激发,对荧光发射光谱进行采集,然后通过控制系统程序升温,每升高20K,对荧光发射光谱进行一次采集。用Origin软件将数据进行处理得到如图6所示的晶体的变温(77~295 K)荧光测试结果,- 图 6 中的 (a) 为175~295K的荧光测试结果(随着温度的升高,荧光发射峰的强度变弱),- 图 6 中的 (b) 为77~175K的荧光测试结果(随着温度的升高,665nm处的荧光发射峰的强度变弱,697nm处的荧光发射峰的强度增强);- 图 6 中的 c 为将- 图 6 中的 a 和- 图 6 中的 b 中665nm和697nm处的荧光强度比与温度变化用Origin 软件进行数据处理得到的关系曲线(曲线方程y=1.37-0.00689x,R2=0.9999,其中y表示665nm和697nm处的荧光强度比,x表示温度)。进一步测量上述红光有机晶体在未知环境温度下的荧光发射光谱,计算665nm和697nm处的荧光强度比,代入上述关系曲线,可以计算得到环境温度,从而实现低温(77~175 K)范围的精确测量。The crystal obtained in Example 1 is sample-prepared, placed in a sample chamber, poured into a cooling device with 77K liquid nitrogen, and a 375nm LED excitation light source is used to excite the crystal sample, and the fluorescence emission spectrum is collected, and then passed The temperature of the control system is programmed to rise, and the fluorescence emission spectrum is collected once every time the temperature rises by 20K. Process the data with Origin software to obtain the fluorescence test results of crystals with variable temperature (77-295 K) as shown in Figure 6, - (a) in Figure 6 is the fluorescence test results of 175-295K (with the increase of temperature , the intensity of the fluorescence emission peak becomes weaker), - (b) in Figure 6 is the fluorescence test result of 77 ~ 175K (as the temperature increases, the intensity of the fluorescence emission peak at 665nm becomes weaker, and the fluorescence emission at 697nm The intensity of the peak is enhanced); -c in Figure 6 is the relationship curve obtained by processing the data processing of the fluorescence intensity ratio at 665nm and 697nm in -a in Figure 6 and -b in Figure 6 with the temperature change ( Curve equation y=1.37-0.00689x, R 2 =0.9999, where y represents the fluorescence intensity ratio at 665 nm and 697 nm, and x represents temperature). Further measure the fluorescence emission spectrum of the above-mentioned red-light organic crystal at an unknown ambient temperature, calculate the fluorescence intensity ratio at 665nm and 697nm, and substitute the above relationship curve, the ambient temperature can be calculated, so as to realize the accurate measurement in the range of low temperature (77-175 K) Measurement.

Claims (3)

1. A red light-emitting organic crystal prepared from a compound represented by formula (I) by a solvent evaporation method is a triclinic system, and the unit cell parameters in the crystal are a =8.4810 (3), b =11.4818 (5), c =14.0570 (6), α =89.7366 (15), β =87.7218 (16), γ =86.1781 (15),
Figure FDA0004053508850000011
2. use of a red-emitting organic crystal according to claim 1 in low temperature fluorescence sensing.
3. Use of a red-emitting organic crystal according to claim 2 in low temperature fluorescence sensing, wherein: the low-temperature sensing range is 77-175K.
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