电喷雾电离(ESI)是一种用于质谱分析的技术,利用电喷雾产生离子,其中向液体施加高电压以产生气溶胶。它在使大分子产生离子方面特别有用,因为其克服了使大分子电离时被碎裂的倾向。电喷雾电离不同于其他电离过程(例如基质辅助激光解吸/电离(MALDI)),其可以产生多电荷离子,有效地扩大分析仪的测量范围,并可蛋白质及其相关多肽片段实验中探测到的kDa-MDa数量级的电离大分子。[1][2]
使用电喷雾质谱技术的质谱被称为电喷雾电离质谱,或者被称为电喷雾质谱。电喷雾电离是一种所谓的“软电离”技术,因为几乎没有碎片,因此比较有利。因为分子离子(或者更准确地说是伪分子离子)可以被检测到,然而从从简单质谱只能获得非常少的结构信息。其可以通过将电喷雾电离与串联质谱联用来克服。电喷雾电离的另一个重要优点是液相信息可以保留在气相中。
电喷雾电离技术由山下正道和约翰·芬于1984年首次报道。二者因[3]电喷雾电离用于生物大分子分析的发展[4]获得了2002年诺贝尔化学奖。[5]芬恩博士使用的原始仪器之一后来在宾夕法尼亚州费城的科学历史研究所展出。
目标分析物的液滴通过电喷雾,[14]分散成细气溶胶。因为离子形成涉及大量溶剂蒸发(也称为去溶剂化),电喷雾电离的典型溶剂是通过将水与挥发性有机化合物(例如甲醇[15]乙腈)混合来制备的。为了减小初始液滴尺寸,通常向溶液中加入增加电导率的化合物(如乙酸)。这些物质还提供质子源来促进电离过程。除了电喷雾源的高温之外,大流量电喷雾还可以受益于加热的惰性气体如氮气或二氧化碳的雾化。[16]气溶胶通过带有大约3000伏电位差的毛细管后被进入到质谱仪的第一级真空,毛细管可以被加热以帮助从带电液滴中进一步蒸发溶剂。溶剂从带电液滴蒸发,直到达到瑞利极限时变得不稳定。此时,液滴变形,因为液滴尺寸不断减小,从而出现电荷静电排斥的力强于将液滴表面张力的现象。[17]在这一点上,液滴经历库仑裂变,从而原始液滴“分裂”,产生许多更小、更稳定的液滴。新液滴经历去溶剂化和随后的库仑破裂。裂变过程中,液滴损失了一小部分质量(1.0-2.3%),同时也损失了相对大部分电荷(10-18%)。[18]
解释气相离子最终产生的主要理论有两种:离子蒸发模型(IEM)和电荷残留模型(CRM)。IEM理论认为,当液滴达到一定半径时,液滴表面的场强变得足够大,从而导致溶剂化离子解吸。[19][20] CRMR认为电喷雾液滴经历蒸发和分裂循环,最终导致含有大约一个分析物离子的子代液滴。[21]气相离子在剩余的溶剂分子蒸发后形成,留下分析物和液滴携带的电荷。
大量证据直接或间接表明,小离子(来自小分子)通过离子蒸发机制释放到气相中,[[20][21][22]而较大离子(例如来自折叠蛋白)通过带电残留物机制形成。 [23][24][25]
现已经提出了第三种模型,该模型是组合电荷剩余电场诱发粒子释放的模式。[26]另一个被称为链弹射模型(CEM)的模型是针对无序聚合物(未折叠蛋白质)提出的。[27]
质谱观察到的离子可以是通过添加氢阳离子产生的准分子离子,表示为[M + H]+,或另一种阳离子,例如钠离子,[M +钠]+,或去除氢核,[M-H]。经常观察到多电荷离子,如[M + nH]n+离子。对于大分子来说,可以有许多电荷态,从而产生一个特征电荷态包络。所有这些都是偶电子离子种类:电子(单独的)不被添加或移除,不同于其他一些电离源。分析物有时涉及电化学过程,导致质谱中相应峰的移动。这种效应在使用电喷雾对铜、银和金等贵金属的直接电离中得到证明。[28]
在低流速下运行的电喷雾产生更小的初始液滴,这确保了更高的电离效率。1993年盖尔和理查德·史密斯报告指出,使用较低的流速,灵敏度可以显著提高,降至200 nL/min。[29] 1994年,两个研究小组将在低流速下工作的电喷雾命名为微电喷雾。当电喷雾以300–800 nL/min的速度运行时,埃米特和卡普里奥利证明了高效液相色谱-质谱分析方法的的性能提高。[30] 威尔姆和曼恩证明,约25 nL/min的毛细管流可以维持通过将玻璃毛细管拉至几微米而制造的极其细的电喷雾毛细管中。[31] 后者于1996年更名为纳米电喷雾。[32][33] 目前纳米喷雾的名称也用于通过泵推动以低流速供给的电喷雾模式中,[34] 其不仅仅用于自供给电喷雾。虽然电喷雾、微喷雾和纳米电喷雾可能没有明确的流速范围,[35]但 研究了“离子释放前液滴分裂过程可知液滴的缩小进程快于离子的释放过程。[35] 其结果是通过对照其他三组的数据以及[36][37][38] 测量不同流速下的[Ba2++ Ba+]/[BaB+]信号强度比而得出的。
冷喷雾电离是电喷雾的一种形式,其中含有样品的溶液被通过一个小的冷毛细管(10-80°C )进入电场,产生冷带电液滴的细雾。[39] 该方法的应用包括分析脆弱分子和不能用常规电喷雾电离研究的蛋白间相互作用。
电喷雾电离也可以在低至25托的压力下实现,理查德·史密斯及其同事开发出两级离子漏斗界面的纳米电喷雾压力电离模式。[40]由于使用了有助于将离子限制和转移到质谱仪低压区域的离子漏斗,自旋实施提供了更高的灵敏度。纳米电喷雾发射器由细毛细管制成,小孔径约为1-3微米。为了获得足够的导电性,该毛细管通常溅射涂覆有导电材料,例如金。纳米电喷雾电离只消耗几微升样品并形成更小的液滴。[41]低压操作对于低流速特别有效,其中较小的电喷雾液滴尺寸允许实现有效的去溶剂化和离子形成。因此,研究人员后来能够证明,将离子从液相转移到气相中作为离子,并通过双离子漏斗界面转移到质谱仪,总电离利用效率超过50%。[42]
在环境电离中,离子的形成发生在质谱仪之外,无需样品制备。[43][44][45] 电喷雾形成的离子是由环境离子源提供的。
解吸电喷雾电离是一种环境电离技术,其中溶剂电喷雾直接针对样品。[46][47] 通过对样品施加电压,电喷雾被吸引到表面。样品化合物被提取到溶剂中,溶剂再次以高电荷液滴的形式雾化,蒸发形成高电荷离子。电离后,离子进入质谱仪的大气压界面。DESI允许样品在大气压下的环境电离,样品制备很少。
萃取电喷雾电离是一种喷雾型环境电离方法,使用两种方法合并喷雾,其中一种由电喷雾产生。[44]
基于激光的电喷雾环境电离模式是一个两步过程,其中使用脉冲激光从样品中解吸或烧蚀材料表面,材料末流与电喷雾相互作用产生离子。[44]对于环境电离,样品材料沉积在电喷雾附近的靶上。激光从表面喷出的样品中解吸或烧蚀材料,然后电离粒子进入产生高电荷离子的电喷雾中。这类型模式包括有电喷雾激光解吸电离、基质辅助激光解吸电喷雾电离和激光烧蚀电喷雾电离。
静电喷雾电离(ESTASI)涉及位于平坦或多孔表面或微通道内部的样品分析。将含有分析物的液滴沉积在样品区域,向样品区域施加脉冲高压。当静电压力大于表面张力时,液滴和离子被喷射。
二次电喷雾电离(SESI)是一种喷雾型环境电离方法,其中充电离子通过电喷雾产生。当这些离子与它们碰撞时,会给气相中的蒸汽分子充电。
在纸喷雾电离中,样品被施加到一张纸上,添加溶剂,并且高电压被施加到纸上,然后产生离子。
电喷雾电离是液相色谱和质谱联用的离子源。分析可以在线进行,将液相色谱柱洗脱的液体直接送至电喷雾模组,其操作也可以离线进行,收集馏分后在纳米电喷雾质谱装置中进行分析。在电喷雾质谱的众多操作参数中,[51]研究表明:[52]电喷雾电压已被确定为电喷雾液相色谱/质谱梯度洗脱中需要考虑的一个重要参数。[53]各种溶剂组合物[55](如TFA[54][56)或醋酸铵,[55]或增压试剂,[55][56][57][58] 或衍生基团[59]或喷涂条件[60]对电喷雾-液相色谱质谱和/或纳米电喷雾-质谱都具有一定影响。[61]
毛细管电泳-质谱分析是由理查德·史密斯和其太平洋西北国家实验室的同事开发并获得专利的电喷雾质谱方法,它在分析非常小的生物和化学化合物混合物时具有优势,甚至可以用于研究到单个生物细胞方面的探究中,具有广泛的用途。
电喷雾电离也被用于研究非共价气相相互作用。电喷雾过程被认为能够将液相非共价复合物转移到气相中,而不破坏非共价相互作用。当用电喷雾质谱或纳米电喷雾质谱研究配体底物复合物时,发现[55][62] 非特异性相互作用的问题。[63]一个有趣的例子是研究酶和作为酶抑制剂的药物之间的相互作用。电喷雾电离方式被用于[64][65][66] stat 6和抑制剂[66][67][68] 之间的竞争实验,其模式也演变为筛选潜在新药靶标分子的。
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