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Electron ionization

Electron ionization (EI), also known as electron impact ionization, is an ionization technique fundamental to , wherein neutral in the gas phase are bombarded by a high-energy beam of electrons to produce positive radical . This process typically involves accelerating electrons from a heated to an energy of 70 electron volts (eV), which ejects an electron from the , forming a molecular (M⁺•) while imparting excess that often leads to extensive fragmentation into daughter . As a hard ionization method, EI generates reproducible mass spectra rich in structural information, making it particularly suitable for the identification of volatile organic compounds through comparison with extensive spectral libraries. The origins of electron ionization trace back to the early development of in the early 20th century, with the first practical implementation for analyzing gases and vapors described by Henry D. Smyth in using a magnetic sector instrument. By the late 1930s, Alfred O. Nier refined the EI source, establishing it as a standard technique that propelled advancements in isotope separation and organic analysis during . In 1929, further innovations by Bleakney extended EI to inorganic vapors, solidifying its role in producing positive ions via electron-molecule collisions in a high-vacuum environment. In the EI process, gaseous analyte molecules—introduced via direct insertion probes, (GC), or vaporization—intersect perpendicularly with the electron beam in the , where collisions occur according to the Franck-Condon principle, resulting in vertical electronic transitions without immediate nuclear rearrangement. The 70 electron energy exceeds typical potentials (8–12 ), distributing excess energy non-thermally to the molecular , which then fragments via mechanisms described by the Quasi-Equilibrium , yielding ions up to approximately 600 . These spectra feature prominent molecular ions alongside abundant fragment ions, enabling detailed elucidation of molecular structures but often obscuring the intact molecular weight due to the hard nature of the . EI's primary applications lie in gas chromatography-mass spectrometry (GC-MS) systems for , forensic analysis, and pharmaceutical quality control, where its high (ionizing about 1 in 1,000 molecules) and spectral reproducibility support automated library matching against databases containing over 100,000 compounds. Its simplicity and low cost make it a cornerstone of routine analyses, though limitations include the requirement for thermally stable, volatile samples and incompatibility with liquid chromatography (LC) due to the need for a vacuum-compatible gas phase. Despite these constraints, remains indispensable for generating standardized, fragmentation-based fingerprints that facilitate compound identification across diverse scientific fields.

Fundamentals

Principle of Operation

Electron ionization (EI), also known as electron impact ionization, is a hard ionization technique utilized in mass spectrometry wherein a beam of high-energy electrons, typically accelerated to 70 eV, interacts with gas-phase analyte molecules. This process primarily involves the ejection of a valence electron from the analyte, resulting in the formation of a radical molecular ion denoted as M⁺•. Due to the excess energy transferred during the collision—often exceeding the ionization energy of the molecule—extensive fragmentation occurs, producing a characteristic array of fragment ions that provide structural information about the analyte. The operational sequence begins with the emission of electrons from a heated , commonly constructed from materials such as or , which are thermionically heated to release free s. These s are then accelerated to energies ranging from 50 to 100 through an applied potential difference before entering the region, where they collide with vaporized molecules maintained in a high-vacuum environment. The collision dynamics are governed by , in which the incident transfers sufficient to a bound in the molecule, overcoming the and ejecting it if the transferred energy surpasses the threshold. This inelastic process contrasts with , where no net energy transfer occurs, and can also lead to electronic excitation without full . The fundamental ion formation reaction is represented as: \ce{M + e^- -> M^{+•} + 2e^-} where M denotes the neutral analyte molecule, and the ejected electron joins the incident electron. The molecular ion M⁺• is often unstable due to the surplus energy (typically 3–7 eV above the ionization energy), prompting rapid dissociation into fragment ions via processes such as cleavage of bonds: \ce{M^{+•} -> A^+ + B•} Here, A⁺ is a charged fragment and B• is a neutral radical. The extent of fragmentation is influenced by the appearance energy (AE), defined as the minimum electron energy required to produce a specific fragment ion, which includes the ionization energy plus the energy needed for bond dissociation. In contrast, the ionization energy (IE) is the threshold electron energy for forming the intact molecular ion M⁺• without fragmentation. These energies determine ion stability and the resulting fragmentation patterns, with standard 70 eV conditions favoring reproducible, library-matchable spectra.

Efficiency of Ionization

Ionization efficiency in electron ionization (EI) is defined as the ratio of ions produced to electrons emitted from the filament, typically ranging from $10^{-4} to $10^{-2} ions per electron in optimized sources. This low yield arises because only a small fraction of electron-molecule collisions result in ionization, with the process being a rare resonance event. The probability of ionization per collision is quantified by the ionization cross-section \sigma, which represents the effective target area and is approximated as \sigma \approx \pi r^2, where r is the effective collision radius. For 70 eV electrons and small molecules, typical \sigma values are on the order of $2 \times 10^{-16} cm^2. These cross-sections peak near 70 eV, reflecting the balance between sufficient energy for ionization and minimal excess for scattering. Efficiency is influenced by several key factors. Electron energy, optimized at 70-100 , maximizes \sigma while promoting characteristic fragmentation; deviations reduce ion yield or alter spectra. Analyte pressure, typically $10^{-5} to $10^{-7} , determines molecular n; insufficient pressure limits collisions, while excess risks unwanted reactions. Space charge effects from electron-ion repulsion distort beam paths and limit flux at higher currents, reducing overall production. Ion collection , governed by repeller plates that apply a repelling field to direct s out of the source, typically achieves near-complete extraction in well-designed systems but can drop due to misalignment or field inhomogeneities. The resulting ion current I_\text{ion} is given by I_\text{ion} = I_e \times (n \times \sigma \times l), where I_e is the electron current, n is the analyte density, \sigma is the cross-section, and l is the electron path length through the gas; typical I_\text{ion} values range from $10^{-9} to $10^{-8} A. EI's limitations include a relatively low duty cycle—defined as the fraction of produced ions effectively analyzed, often below 10% in scanning instruments—and poorer sensitivity compared to soft ionization techniques, stemming from extensive fragmentation that disperses ion current across multiple m/z values rather than concentrating it on the molecular ion.

Historical Development

Origins and Early Experiments

The foundational observations in electron impact ionization trace back to J.J. Thomson's work in the early , where he analyzed positive rays (anode rays) produced in gas discharge tubes, demonstrating the creation of positive ions through interactions involving and residual gases, laying the groundwork for mass analysis of ions. In these experiments, Thomson used modified apparatus to detect and measure the charge-to-mass ratios of positively charged particles, confirming electron-molecule collisions as a key . Building on this, conducted systematic studies in 1913 at the General Electric Research Laboratory, investigating electron-gas interactions within tubes to understand the effects of residual gases on from hot filaments. Langmuir's work quantified key parameters, including potentials, by measuring the currents of positive ions formed when accelerated s collided with gases such as mercury vapor, providing early empirical data on the thresholds required for . These experiments highlighted the role of in initiating processes and laid groundwork for controlling gas purity in devices. A significant advancement came in 1918 with Arthur J. Dempster's invention of the first practical spectrometer, which integrated an electron ionization source with a 180-degree magnetic sector analyzer to separate ions based on their mass-to-charge ratios. Dempster's apparatus ionized gases or vapors by bombarding them with electrons from a heated , then deflected the resulting positive ions in a to achieve isotopic separation, marking the initial coupling of electron ionization with for precise studies. In 1922, Henry D. Smyth described the first practical implementation of electron ionization for analyzing gases and vapors using a magnetic sector instrument, advancing the technique for chemical analysis. This was followed by Addison Bleakney's 1929 innovations, which extended EI to inorganic vapors and solids through electron-molecule collisions in high-vacuum environments, producing positive ions with a transverse electron beam setup. Prior to the , electron ionization techniques were extensively applied in technology and gas discharge investigations to determine atomic ionization energies. Researchers utilized controlled beams in low-pressure environments to measure the minimum electron energies needed to ionize elements like and , contributing essential data for understanding behavior and electronic device performance. By the late , Alfred O. Nier refined the EI source design, establishing it as a standard that supported advancements in and organic analysis during .

Key Milestones and Evolution

In the 1940s, electron ionization (EI) mass spectrometry saw significant refinements for the analysis of molecules, particularly in the where it was applied to quantify small hydrocarbons in process streams, building on earlier foundational work to enable more practical structural elucidation. During the and , the standardization of 70 electron energy emerged as a key advancement to ensure reproducible fragmentation patterns and library-compatible spectra for compounds. The 1960s marked the commercialization of EI instruments by companies such as Varian and the newly founded Finnigan (established in 1968), which introduced quadrupole-based systems tailored for routine use, enhancing accessibility for . A pivotal development was the 1959 coupling of (GC) with EI by R.S. Gohlke, using a time-of-flight analyzer to separate and identify complex mixtures, laying the groundwork for GC-MS as a hyphenated . From the 1970s to 1980s, EI integrated with advanced mass analyzers like quadrupoles (commercialized post-1953 invention by ) and ion traps (refined by George Stafford in the early 1980s), improving sensitivity and selectivity for trace-level detection. Concurrently, the establishment of comprehensive spectral libraries, such as the NIST/EPA/NIH database originating from the 1973 EPA/NIH collaboration and expanding in the 1980s, standardized compound identification through matched EI spectra at 70 eV. In the 1990s and 2000s, high-resolution EI advanced with (FT-ICR) mass spectrometry, pioneered by Comisarow and Marshall in 1974 and refined for exact mass measurements in complex samples. analyzers, introduced commercially in 2005, also supported EI modes in later GC-MS configurations, particularly for and residue analysis, offering resolutions exceeding 100,000. Recent 2020s innovations include liquid electron ionization (LEI) interfaces for LC-MS compatibility, enabling EI-like spectra from liquid effluents while preserving fragmentation for library searching. Over this period, evolved from a primarily qualitative for structural confirmation—reliant on reproducible fragmentation—to a quantitative method in environmental and forensic applications, where stable and selected in GC--MS provide precise measurements of pollutants and drugs at ppb levels.

Instrumentation

Core Components

The source in electron ionization () systems primarily consists of a thermionic , typically constructed from a or wire coiled or shaped as a to maximize surface area for emission. This is resistively heated to approximately 2000 using a heating current of 3–4 A (with a typical of 5–10 V across the ), enabling thermionic of according to the Richardson-Dushman equation, where the emission current is controlled at 50–500 μA to ensure stable beam generation. filaments are robust but prone to oxidation, while variants offer longer lifetimes and reduced background ions from oxide formation. Electron optics encompass acceleration lenses and focusing electrodes that direct the emitted electrons into the ionization chamber with precise energy, typically 70 eV, to optimize ionization efficiency. The filament is biased at -70 V relative to ground potential, accelerating electrons across this potential difference, while electrostatic lenses collimate and focus the beam to minimize and ensure uniform interaction with the gas. Additional elements, such as a V-shaped repeller plate near the filament, enhance flux by reflecting stray electrons back into the path. The is a compact enclosure, typically with a volume of about 1 cm³, designed to confine the gas and facilitate electron-molecule collisions. It features repeller and extractor plates: the repeller, often positively biased, pushes positive s toward the extractor, which is grounded or negatively biased to draw ions axially out of the chamber for subsequent mass analysis. These plates maintain the analyte in a controlled , promoting efficient ion extraction while the chamber operates at 180–220 °C to prevent . The vacuum system is critical for EI operation, employing turbo-molecular pumps to achieve and sustain pressures around 10⁻⁶ in the source region, thereby minimizing electron-neutral collisions and preserving beam integrity. These pumps, often backed by roughing pumps, evacuate the chamber to prevent filament oxidation and ensure the of electrons exceeds the chamber dimensions. Safety features include filament bias circuits that modulate emission to avoid overloads and interlock systems that disable high voltages if the is compromised or access panels are opened, preventing arcing from electrical discharges. These measures protect both the and operators from hazards associated with the high currents and voltages involved.

Operational Configuration

In electron ionization (EI) mass spectrometry, the source is integrated with the mass analyzer through an ion exit slit that allows ions to be extracted into the analyzer region, such as a quadrupole, time-of-flight (TOF), or magnetic sector instrument, using low voltage gradients typically in the range of 5-20 V to focus and accelerate the ions without excessive fragmentation. This extraction setup ensures efficient transmission of ions while maintaining the high vacuum environment necessary for analyzer performance. Tuning the EI source involves adjusting key parameters to optimize ion yield and spectral quality. Electron energy is commonly set to 70 for standard fragmentation patterns but can be varied from 50 to 200 eV depending on the desired and molecular . Repeller voltage, applied to an opposite the exit slit, ranges from 0 to 10 V to control ion focusing and efficiency, with lower values minimizing contact cooling effects on the cloud. Filament current regulates the of electrons, typically maintaining an emission current of 50–250 μA to achieve stable beam intensity without overheating the . These parameters are often fine-tuned using standard compounds like perfluorotributylamine (PFTBA) to maximize abundance at diagnostic m/z values. Sample introduction into the EI chamber occurs primarily through gas inlets for volatile compounds or direct insertion probes for solids and semi-volatiles, allowing controlled volatilization under to prevent pressure spikes. The system employs vacuum interlocking mechanisms to isolate during sample loading, preventing or loss of vacuum in the analyzer. To achieve and maintain conditions (typically <10^{-6} Torr in the source), bakeout protocols heat the chamber and components to 150-250°C for several hours, removing adsorbed gases and restoring baseline performance. Routine maintenance includes filament replacement every 50-100 hours of operation, as evaporation and contamination degrade emission efficiency over time. Common troubleshooting addresses filament burnout from excessive current or oxygen exposure, often resolved by checking emission stability and cleaning the source, and low ion yield due to contamination, which manifests as elevated background noise and requires solvent rinses or full disassembly. These procedures ensure reliable, long-term operation of the EI source in mass spectrometric workflows.

Applications

Direct Probe and Vacuum Methods

The direct insertion probe serves as a key inlet system for introducing solid or semi-solid samples into the electron ionization (EI) source of a mass spectrometer without prior chromatographic separation. In this method, a small sample aliquot is placed in a quartz or ceramic crucible mounted on a probe rod, which is then inserted through a vacuum lock directly into the ionization chamber. The probe is resistively heated, typically from ambient temperature up to 400–500°C, to volatilize the sample analytes for subsequent at standard energies around 70 eV, promoting characteristic fragmentation patterns. This approach is well-suited for low-volatility or thermally stable compounds, including those prone to decomposition, as it minimizes exposure time in the hot source environment. The vacuum manifold, often referred to as a batch inlet system, provides an alternative for handling gaseous or highly volatile liquid samples in standalone EI setups. This configuration consists of a small, evacuated glass or metal chamber connected to the ion source via a molecular leak or valve, allowing precise introduction of microliter-scale sample volumes without significantly perturbing the high vacuum. Samples are admitted in batches, equilibrating briefly before ionization, which enables efficient analysis of limited quantities of volatiles while maintaining instrument stability. These methods find application in the characterization of complex, non-routine samples, such as archaeological artifacts and synthetic nanomaterials. For instance, pyrolysis- using a direct insertion probe has been applied to analyze resins in ancient pottery and adhesives, revealing triterpenoid compositions through diagnostic fragment ions from heated degradation products. Similarly, EI fragmentation patterns of fullerenes like C60 and C70, introduced via direct probe, exhibit sequential losses of C2 units, aiding in structural confirmation of carbon clusters. The high reproducibility of EI spectra from these inlets supports qualitative identification by matching, as standardized fragmentation facilitates comparison with like NIST, enhancing structural elucidation for unknowns. A primary limitation arises from the absence of separation, which can yield convoluted spectra from multicomponent mixtures, necessitating prior sample purification for accurate interpretation.

Gas Chromatography-Mass Spectrometry

In gas chromatography-mass spectrometry (GC-MS) utilizing (EI), the effluent from a column, typically operating at low carrier gas flow rates of 1–2 mL/min, is directly introduced into the without the need for splitting due to the compatibility with the mass spectrometer's vacuum system. This interface is achieved via a heated transfer line maintained at temperatures around 250–300°C to prevent of volatile and semi-volatile analytes, ensuring efficient transport of the separated compounds into the where they undergo EI fragmentation. The standard workflow involves temperature-programmed separation in the column, where analytes are volatilized and separated based on their boiling points and interactions with the phase, followed by continuous at 70 eV to produce characteristic fragment ions for structural elucidation. These spectra are then matched against comprehensive libraries such as the NIST database for compound identification, enabling reliable qualitative analysis of complex mixtures. 's production of reproducible fragmentation patterns is particularly advantageous here, providing rich structural information that complements the chromatographic separation. This technique finds extensive use in environmental analysis, such as detecting pesticides in water samples at trace levels through and cleanup prior to GC-MS, allowing and quantification of contaminants like organochlorines. In biological fluid analysis, GC-EI-MS facilitates the profiling of steroids in , offering high for endogenous and exogenous compounds after derivatization to enhance volatility. Forensic toxicology applications include the screening and confirmation of drugs in biological matrices, where EI spectra aid in distinguishing metabolites and analogs in overdose cases. Additionally, in archaeological studies, it enables the characterization of biomarkers in artifacts, such as fatty acids from ancient residues, revealing insights into historical diets and vessel uses. For quantitative analysis, selected ion monitoring (SIM) mode in GC-EI-MS enhances sensitivity by focusing on target ions, achieving detection limits in the parts-per-billion (ppb) range for trace analytes in complex matrices. Recent advancements, such as fast GC-EI-MS, employ shorter columns and rapid temperature ramps to reduce analysis time to under 5 minutes per sample, supporting high-throughput screening in regulatory and clinical settings while maintaining EI's identification power.

Liquid Chromatography-Mass Spectrometry

Electron ionization (EI) has been adapted for liquid chromatography-mass spectrometry (LC-MS) to analyze non-volatile and thermally labile analytes, addressing the challenge of interfacing high liquid flow rates from LC systems, typically in the range of microliters per minute, with the gas-phase requirements of EI. Traditional approaches, such as (PB-EI) interfaces, involve nebulization of the LC effluent followed by solvent evaporation and momentum separation to deliver dry particles into the EI source, enabling desolvation without excessive dilution. Alternatively, direct liquid introduction methods use heated nebulization and evaporation to convert the stream into vapor for EI, though these can suffer from solvent overload in the . A significant recent advancement is liquid electron ionization (LEI), developed in the mid-2010s, which employs a microchannel to gently heat and evaporate s at sub-microliter flow rates, often assisted by nebulization or membrane diffusion, before introducing the gas-phase molecules into a standard source. This variant minimizes premature by separating from , with temperatures optimized up to 400 °C based on , and has been extended in the to variants like extractive-LEI for ambient sampling. LEI supports nanoflow LC rates of 500–1500 nL/min, while PB-EI accommodates higher flows up to 1 mL/min after splitting. In applications, LC-EI, particularly via or interfaces, is employed for pharmaceuticals such as cannabinoids and drug metabolites, where it complements soft ionization methods like (ESI) by providing characteristic EI fragmentation patterns for structural confirmation and library matching against NIST databases. For peptides and larger biomolecules, it is used selectively for smaller, more volatile species to generate interpretable spectra, though ESI remains preferred for intact analysis. Environmental monitoring benefits from LC-EI in detecting non-volatile contaminants like surfactants (e.g., ) and in complex matrices, leveraging EI's reproducibility for quantitative identification. These techniques are complementary to gas chromatography-mass spectrometry (GC-MS) for volatile compounds, extending EI's utility to polar and ionic species separated by LC. Performance-wise, LC-EI offers robust libraries for but exhibits lower than ESI, with limits of detection typically in the ng/mL for nonpolar s, due to the need for complete and potential suppression from residual solvents. It excels in producing standard 70-eV EI spectra suitable for database searching, with minimal matrix effects compared to soft ionizations. However, limitations include during the vaporization step, particularly for heat-sensitive compounds, which can lead to peak tailing or reduced recovery; this is mitigated in LEI by controlled heating but remains a challenge for larger molecules.

Advanced Mass Analyzer Integrations

Electron ionization (EI) sources are compatible with advanced mass analyzers that provide enhanced and , enabling detailed of complex samples through high accuracy and multi-stage fragmentation capabilities. These integrations leverage the characteristic fragmentation patterns produced by , which are ideal for library matching, while the analyzers offer precise measurements and structural elucidation beyond traditional systems. In time-of-flight (TOF) mass spectrometry, EI benefits from pulsed ion extraction, where ions generated by a continuous or gated beam are rapidly accelerated into the flight tube, allowing high-speed analysis with scan rates exceeding 100 spectra per second. This configuration is particularly advantageous in , where EI-TOF enables millisecond-resolution profiling of volatile metabolites from separations, achieving mass accuracies below 5 ppm for confident identification of hundreds of compounds in biological matrices like human . Fourier transform ion cyclotron resonance (FT-ICR) analyzers paired with EI sources deliver ultra-high resolution exceeding 10^5, facilitating exact mass determination of EI fragments for unambiguous molecular formula assignment. Although less common for large biomolecules due to EI's fragmentation, EI-FT-ICR has been applied in the analysis of complex mixtures such as and environmental samples, where the high resolves isobaric ions in detailed compositional studies. Ion trap mass spectrometers integrated with enable sequential isolation and fragmentation (^n, up to n=10), allowing iterative breakdown of precursor to reveal structural details not visible in single-stage spectra. In forensic applications, -ion trap systems excel at distinguishing structural isomers of psychoactive substances, such as positional variants of synthetic cathinones or phenethylamines, by comparing fragmentation pathways and abundance ratios in controlled analyses. Orbitrap analyzers in hybrid configurations with EI sources provide high-resolution accurate mass (HRAM) detection up to 240,000 FWHM, combining EI's reproducible fragmentation with sub-ppm accuracy for building comprehensive spectral libraries. Recent advancements since 2023 incorporate machine learning for spectral interpretation, where deep neural networks refine library matching by predicting fragment origins and resolving ambiguities in EI data from environmental or metabolomic samples. Hybrid configurations, such as quadrupole-TOF (Q-TOF) with EI sources, utilize the quadrupole for precursor ion selection and prior to TOF analysis, enhancing sensitivity and specificity in targeted workflows. These setups maintain EI's 70 eV ionization for compatibility while achieving resolutions over , as demonstrated in contaminant screening and differentiation.

Advantages and Disadvantages

Advantages

Electron ionization (EI) at the standard energy of 70 eV produces highly reproducible fragmentation patterns, allowing for the creation and utilization of extensive spectral that facilitate unambiguous compound identification. This has enabled the of comprehensive , such as the NIST/EPA/NIH EI library, which contains over 394,000 spectra for more than 347,000 compounds as of 2023. As a hard ionization technique, imparts sufficient energy to molecules to cause extensive bond cleavage, generating characteristic fragment ions that provide rich structural information essential for elucidating the identity of unknown compounds. These fragment patterns reveal molecular substructures and functional groups, making particularly valuable for detailed qualitative analysis in . EI operates under high conditions without the need for chemical , offering simplicity, robustness, and low operational costs that make it suitable for routine use. The absence of minimizes risks and requirements, while its with systems ensures reliable in standard mass spectrometer configurations. In selected ion monitoring (SIM) mode, EI delivers quantitative accuracy when paired with internal standards, supporting precise measurements across varying concentrations. This capability enhances its utility for targeted quantification in analytical workflows. Recent advancements include the integration of for automated spectral matching, such as the FastEI method introduced in 2023, which leverages techniques to rapidly and accurately identify compounds against large in-silico libraries.

Disadvantages

Electron (EI) exhibits low ionization efficiency, typically on the order of 0.001% to 0.1% of molecules, which results in poor sensitivity for detecting trace-level s at nanogram quantities, in contrast to picogram-level detection achievable with (ESI). This limited efficiency arises from the sparse interaction between the high-energy electron beam and gas-phase molecules under high-vacuum conditions, where only a small fraction of molecules are ionized before being pumped away. EI requires samples to be volatile and thermally stable to facilitate and into the without decomposition, restricting its use to low-molecular-weight compounds that can withstand temperatures up to 250–300°C. Non-volatile or thermally labile analytes necessitate prior derivatization to enhance or to generate volatile fragments, adding complexity and potential artifacts to the analysis. The high-energy electron bombardment (typically 70 ) in EI induces extensive fragmentation of the molecular , often resulting in its low abundance—below 5% relative intensity for approximately 40% of compounds in standard spectral libraries—which complicates accurate molecular weight determination. This fragmentation pattern, while informative for elucidation, frequently obscures the parent signal, making EI less reliable for identifying unknowns without complementary techniques. Operation under high vacuum (approximately 10^{-5} ) is essential to minimize ion-molecule collisions and maintain spectral reproducibility, but it exacerbates source contamination when non-volatile residues deposit on ion optics, necessitating frequent —often every few weeks to months depending on sample throughput—to restore performance. EI is particularly unsuitable for large biomolecules, such as proteins or peptides, due to their poor , extensive fragmentation, and low transmission efficiency through the mass analyzer, rendering it outdated for quantitative where softer ionization methods like (APCI) or ESI provide better intact ion yields. As a hard technique, EI contrasts with soft methods that minimize fragmentation to preserve molecular information.

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