CN113603722B - 一种极性荧光探针及其制备方法和应用 - Google Patents
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Abstract
本发明属于荧光探针领域,具体涉及一种极性荧光探针及其制备方法和应用。为解决通过荧光强度变化来检测极性的荧光探针在实际应用时易受探针浓度及环境因素干扰等问题,本发明提供了一种通过波长变化来检测极性的荧光探针。该探针结构中包含着D‑A‑D结构,其发射波长随着体系极性的增大而逐渐红移,发射波长与0.020‑0.287的极性范围呈良好的线性关系。因此,该探针为准确检测化学溶剂或者细胞内的极性变化提供了一个潜在的工具。
Description
技术领域
本发明属于荧光探针领域,具体涉及一种极性荧光探针及其制备方法和应用。
背景技术
极性不仅是化学和化工领域中一个非常重要的化学参数,也是细胞微环境的重要参数之一。细胞极性是细胞中某些胞质成分按照一定空间顺序的不均等分布,从而形成各种细胞内容物的浓度梯度,正是由于细胞极性的存在导致了细胞的不对称分裂。在生物体系中,极性在调节细胞迁移、增殖、分化、囊泡转运、激素分布和免疫反应等关键生理过程中发挥着关键作用。例如,蛋白质可以通过改变构象调节其内部极性,来控制酶促反应速率;小管上皮细胞的极性是小管吸收、分泌排泄和交换等功能的基础等。细胞内极性微环境的异常还与某些代谢性疾病的发生和发展密切相关,如常染色体显性遗传性多囊肾、肝硬化及肿瘤等。因此,开发能检测细胞极性的荧光探针对于研究蛋白质的生理功能或防治疾病等均具有重要意义。
鉴于高敏感性、可视化、非侵袭性、无辐射、实时检测、低成本等特点,荧光技术已经是生物学、医学、药学等领域不可或缺的研究手段,在食品与药品安全检测、环境监测、医学诊断等方面发挥了重要作用。近年来,极性荧光探针因具有检测灵敏性高,生物兼容性好等优点,被认为是检测细胞内极性变化的理想工具。目前报道的极性荧光探针的常用设计策略是基于分子内电荷转移(ICT)机理,即探针结构中包含着推/拉电子体系,当体系的极性发生改变时会引起探针荧光强度或者波长的改变。基于荧光强度改变的极性探针在实际应用时可能会受到探针浓度、生物自发荧光或者环境因素的影响,而基于波长改变的极性探针则可以有效避免上述问题。针对这一问题,本发明开发了一种基于苯基磷氧吡啰红酮荧光团的新型极性荧光探针,该探针可以通过波长变化来检测极性的改变,不受探针浓度、生物自发荧光或者环境因素的、干扰,因此,该探针为准确检测化学溶剂或者细胞内的极性变化提供了一个潜在的工具。
发明内容
针对上述问题本发明提供了一种极性荧光探针及其制备方法和应用,该探针结构中包含着D-A-D结构,其发射波长随着体系极性的增大而逐渐红移,探针的发射波长与0.020-0.287的极性范围呈良好的线性关系。因此,该探针有望成为准确检测化学溶剂或者细胞内极性的重要工具。
为了达到上述目的,本发明采用了下列技术方案:
一种极性荧光探针,所述探针的结构式为:
一种极性荧光探针的制备方法,其特征在于,包括以下步骤:
(1)将3-溴-N,N-二甲基苯胺(化合物1)溶解在冰醋酸中,向上述溶液中逐滴滴入福尔马林溶液,进行搅拌反应,反应结束后,将冰醋酸旋干,得到的固体经饱和NaHCO3溶液中和、萃取、洗涤、干燥和柱色谱分离后得到4,4’-亚甲基双(N,N-二甲基苯胺)(化合物2)。
(2)将4,4’-亚甲基双(N,N-二甲基苯胺)(化合物2)溶解在无水THF中,反应体系在无水无氧条件下冷却至-78℃,向上述溶液中逐滴加入正丁基锂,维持此温度搅拌;将苯基二氯膦溶解在无水THF中,并将此溶液逐滴滴入上述反应液中,反应液升至室温并反应过夜;反应结束后加盐酸溶液猝灭反应,反应液经萃取、洗涤、干燥和柱色谱分离后得到二氢苯基磷吡啰红(化合物3)。
(3)将二氢苯基磷吡啰红(化合物3)溶解在THF中,逐渐加入四氯苯醌,室温搅拌后旋干溶剂,得到的固体经柱色谱分离后得到所述极性荧光探针PPyK。
进一步,所述步骤(1)中福尔马林溶液的质量分数为37%,所述3-溴-N,N-二甲基苯胺与福尔马林溶液的摩尔体积比为5mol:1mL。
进一步,所述步骤(1)中搅拌反应的温度为90℃,时间为1h,所述萃取用二氯甲烷,所述洗涤用盐水,所述干燥用无水硫酸镁,所述柱色谱分离展开剂乙酸乙酯:正己烷的体积比为1:30。
进一步,所述步骤(2)中4,4’-亚甲基双(N,N-二甲基苯胺)、正丁基锂与苯基二氯膦的摩尔比为1:2:1。
进一步,所述步骤(2)中搅拌的时间为1.5h,所述盐酸溶液的浓度为2mol/L,所述萃取用二氯甲烷,所述洗涤用盐水,所述干燥用无水硫酸镁,所述柱色谱分离展开剂二氯甲烷:石油醚的体积比为2:5。
进一步,所述步骤(3)中二氢苯基磷吡啰红与四氯苯醌的摩尔比为1:3。
进一步,所述步骤(3)中室温搅拌的时间为15分钟,所述柱色谱分离展开剂二氯甲烷:甲醇体积比为20:1。
一种极性荧光探针的应用,在制备检测化学溶剂或者细胞内极性试剂的应用。
与现有技术相比本发明具有以下优点:
(1)探针合成步骤简单,原料便宜;
(2)探针通过波长变化来检测极性的改变,不受探针浓度及环境因素干扰;
(3)该探针生物兼容性好,有望应用于活体中。
附图说明
图1为化合物2的1H NMR图(CDCl3,600MHz);
图2为化合物2的13C NMR图(CDCl3,150MHz);
图3为化合物2的HRMS图;
图4为化合物3的1H NMR图(CDCl3,600MHz);
图5为化合物3的13C NMR图(CDCl3,150MHz);
图6为化合物3的HRMS图;
图7为探针PPyK的1H NMR图(CDCl3,600MHz);
图8为探针PPyK的13C NMR图(CDCl3,150MHz);
图9为探针PPyK的HRMS图;
图10为探针PPyK在不同溶剂中的紫外可见吸收光谱图。
图11为探针PPyK在不同溶剂中归一化的荧光光谱图;
图12(A)为探针PPyK在不同比例的水和1,4-二氧六环中归一化的荧光光谱图;图12(B)为探针的最大发射波长与溶剂极性的线性关系图。
具体实施方式
实施例1
一种极性荧光探针,其特征在于,所述探针的结构式为:
一种所述极性荧光探针的制备方法,其特征在于,包括以下步骤:
(1)将化合物1(5g,25mmol)溶解在冰醋酸(40mL)中,向上述溶液中逐滴滴入37%的福尔马林溶液(5mL),混合物在90℃下搅拌反应1h;反应结束后,将冰醋酸旋干,得到的固体经饱和NaHCO3中和、二氯甲烷(3×100mL)萃取、盐水洗涤、无水硫酸镁干燥和柱色谱分离(乙酸乙酯:正己烷=1:30)后得到化合物2(6.18g,60.0%)。
1H NMR(600Hz,CDCl3)δ7.20(m,7H),7.06(d,J=12.0Hz,2H),6.70(d,J=8.4Hz,2H),3.63(s,2H),2.90(s,12H);13C NMR(150MHz,CDCl3)δ152.0,151.9,141.4,141.3,138.2,135.1,135.0,134.2,131.4,131.1,131.0,130.6,121.8,121.5,116.3;ESI-MS:[M+H]+calcd for413.01,Found 413.00.
(2)将化合物2(1.23g,3mmol)溶解在无水THF(10mL)中,反应体系在无水无氧条件下冷却至-78℃,向上述溶液中逐滴加入正丁基锂(6mmol),维持此温度搅拌1.5h;将苯基二氯膦(0.54g,3mmol)溶解在无水THF中(5mL),并将此溶液逐滴滴入上述反应液中,反应液缓慢升至室温并反应过夜;反应结束后加盐酸(2mol/L,10mL)猝灭反应,反应液经二氯甲烷(3×100mL)萃取、盐水洗涤、无水硫酸镁干燥和柱色谱分离(二氯甲烷:石油醚=2:5)后得到化合物3(0.571g,52.9%)。
1H NMR(600Hz,CDCl3)δ7.20(m,7H),7.06(d,J=12.0Hz,2H),6.70(d,J=8.4Hz,2H),3.63(s,2H),2.90(s,12H);13C NMR(150MHz,CDCl3)δ152.0,151.9,141.4,141.3,138.2,135.1,135.0,134.2,131.4,131.1,131.0,130.6,121.8,121.5,116.3;ESI-MS:[M+H]+calcd for 361.18,Found 361.18.
(3)将化合物3(0.36g,1mmol)溶解在THF(20mL)中,敞口逐批加入四氯苯醌(0.738g,3mmol),室温搅拌15分钟后旋干溶剂,得到的固体经柱色谱分离(二氯甲烷:甲醇=20:1)后得到探针PPyK(0.334g,85.6%)。
1H NMR(600Hz,CDCl3)δ8.33(d,J=9.0Hz,1H),8.31(d,J=9.0Hz,1H),7.60(m,2H),7.38(m,1H),7.32(m,2H),7.15(dd,J1=2.4Hz,J2=9.0Hz,2H),6.87(dd,J1=2.4Hz,J2=9.6Hz,2H),3.07(s,12H);13C NMR(150MHz,CDCl3)δ183.3,183.2,155.5,155.4,138.4,137.9,137.7,137.3,134.2,134.1,133.3,133.2,131.5,131.4,127.4,127.3,117.5,114.8,114.7,42.9;ESI-MS:calcd for 391.16,Found391.16.
实施例2
1.测试溶液配制
将探针用乙腈配成2mM的储存液,随后用不同溶剂或者不同比例的水和1,4-二氧六环溶液稀释至测试浓度。
2.光物理性质研究
将10μL的探针分别加到2mL不同极性的溶剂中,从紫外-可见吸收光谱可以看出,探针有两个吸收峰,分别在350nm处和430nm左右,且短波的吸收峰几乎不随溶剂极性的改变而发生位移,只有长波处的吸收峰会随着溶剂极性的增大发生红移(图10),因此,我们仅检测探针的长波长随溶剂极性的变化。随后,选取400nm为激发波长,测试探针在不同极性的溶剂的发射光谱,如图11所示,探针的发射波长随溶剂极性的增大而逐渐红移。上述结果说明,本发明提供的探针是一个对极性敏感的探针,即探针的发射波长随着环境极性的增大而红移,与传统荧光增强型极性探针相比,该探针不受探针浓度以及环境因素干扰。
3.探针波长与极性的关系研究
为模拟不同的极性,测试了探针在不同比例的水和1,4-二氧六环中的发射光谱,如图12(A)所示,探针的发射波长随水比例的增大而逐渐红移。为研究探针的发射波长与环境极性的定量关系,绘制了探针波长与不同比例的水和1,4-二氧六环对应的极性的线性关系图,如图12(B)所示,探针的波长与0.020-0.287(0-40%含水量)的极性范围呈良好的线性关系,线性相关系数R=0.999。因此,可以根据本探针在待检测溶剂中的波长,来精确检测0.020-0.287的极性范围。
以上所述仅为本发明的较佳实施例而已,并不用以限制本发明,凡在本发明的精神和原则之内,所作的任何修改、等同替换、改进等,均应包含在本发明的保护范围之内。
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