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Supersonic GC-MS

SuperMass was established in order to bring the benefits of GC-MS with supersonic molecular beams to its potential users in a compact and reliable bench top system termed Supersonic GC-MS. This document describes the various aspects and features of the Supersonic GC-MS so that you can evaluate its benefits for your research and applications.

Table of Contents 
1. Introduction - What is a Supersonic Molecular Beam 
2. Summary of Supersonic GC-MS Advantages and Unique Features  
3. Supersonic GC-MS Instrument 
4. Electron Ionization of Molecules in the SMB  
5. Hyperthermal Surface Ionization 
6. Fast and Ultra-Fast GC-MS 
7. Sensitivity Considerations and Evaluation  
8. The Analysis of Thermally Labile and Relatively Non Volatile Compounds  
9. Applications of Supersonic GC-MS and Fast GC-MS 
10. Direct/Dirty Sample Introduction Device (ChromatoProbe)  
11. Laser Desorption Fast GC-MS 
12. Links 
13. References

1. Introduction - What is a Supersonic Molecular Beam (SMB)

A Supersonic molecular beam (SMB) is formed by the expansion of a gas through a ~0.1 mm pinhole into a vacuum chamber. In this expansion the carrier gas and heavier sample molecules obtain the same final velocity so that the sample compounds are accelerated to the carrier gas velocity, since it is the major gas component. Furthermore, the uniform velocity ensures a slow intra-beam relative motion, resulting in the cooling of the internal vibrational degrees of freedom.
SMB’s are characterized by the following features that are of importance for GC-MS:

a) Supercooling of the molecular vibrational-rotational degrees of freedom. 
b) A controlled amount of kinetic energy in the hyperthermal energy range up to 30 eV. 
c) Unidirectional motion in space. 
d) High flow rate up to 240 ml/min. 
e) Heavy species concentration (jet separation). 
f) Atmospheric pressure sample inlet capability. 

We have explored over the coarse of last 15 years the use of these unique properties of SMB for improving mass spectrometry and GC-MS [1-20]. We found that the SMB results in important implications to both GC sampling and molecular ionization processes. The intra-molecular vibrational cooling conditions prevailing in SMB substantially improve the level of information available through electron impact ionization (EI). Hyperthermal surface ionization, which is unique to the use of SMB, provides an ultra sensitive and selective ionization method, that is ideal for use with drugs and aromatic compounds. The use of SMB for interfacing and ionization improves all aspects of GC-MS and enables a truly optimized fast GC-MS analysis of a wide range of samples.

The basic GC-MS instrument modifications for conversion into a Supersonic GC-MS include:

a) The two injectors and columns of a Hewlett Packard 6890 GC are connected simultaneously to a supersonic nozzle with any type of column, length and flow rate, serving as a conventional or fast GC inlet; 
b) Sampling to the vacuum system is in the form of a supersonic molecular beam, as the organic molecules expand with helium or hydrogen from the supersonic nozzle; 
c) The electron ionization (EI) ion source is modified to allow for unperturbed axial passage of the molecular beam (fly through) with a higher electron emission current; 
d) A suitable surface is added to allow for surface ionization in addition to electron ionization. 

In addition to these modifications, the basic apparatus includes the Hewlett Packard 5972 or 5973 MSD quadrupole mass analyzer and ion detector in its original unmodified vacuum system, pumped by a 60L/sec diffusion pump. An additional such air cooled 60L/sec diffusion pump and 520 L/min rotary pump are added for the small supersonic nozzle vacuum chamber and its differential pumping chamber.

In a book "Supersonic Molecular Beam Mass Spectrometry - The Quest for Ultimate Performance GC-MS and Fast GC-MS" the Supersonic GC-MS technology is described and demonstrated through 51 figures and many applications.
This book is available free on request.
You may ask for it at:  amirav@supermass.co.il.
Please add a brief description of your application and range of GC-MS interests. 

We would be delighted to try your samples and meet your requirements so that you could closely evaluate the suitability of Supersonic GC-MS to solve your tough applications.  Please challenge us at: amirav@supermass.co.il.
 



2. Summary of Supersonic GC-MS Advantages and Unique Features

We consider our Supersonic GC-MS technology to be a major breakthrough, with improvements of all the major aspects of GC-MS, including the level of MS information obtained, speed of analysis, sensitivity, selectivity, scope of use, flexibility and ease of use. Supersonic GC-MS contains the broadest range of features and capabilities ("Super Enhancement Package") to provide you with the cutting edge technology and competitive advantage.

redball.GIF (649 bytes)  1. Information
The vibrational cooling effect in EI, provides the highest level of mass spectral information. The unique capabilities of the EI-SMB ion source truly make it the "Ideal Ion Source".

a) The molecular ion peak is practically always exhibited. 
b) Improved library search and confirmation capabilities due to the presence of M+. 
c) Tunable fragmentation is achieved by controlling the electron energy. 
d) Elemental and isotope information is contained in the M+ complex of peaks. 
e) Unique intra-nozzle deuterium exchange enables OH and NH identification (optional). 
f) Increased isomer and structural information is provided. 
g) M+ is the predominant or only peak exhibited at low electron energy for increased orthogonal MS separation power. 
h) Tailing-free fast ion source response is provided without any vacuum memory effects. 

redball.GIF (649 bytes)  2. Speed
SMB enables the highest capability fast GC-MS, from the reduction or elimination of sample preparation to the final fast analysis results. This fast GC-MS approach is based mostly on the high flow rate capability of the SMB inlet and on the improved separation power of the MS with EI or HSI of the SMB compounds, as well as on several other SMB features. Fast GC-MS (a few minutes down to a few seconds) is achieved, characterized by unrestricted column type, length and flow rate, very high temperature operation capability, thermally labile compound analysis capability, higher sensitivity, selective ionization with HSI and enhanced molecular ion peak in EI. SMB uniquely enables ultra fast ion source response time, simple syringe based large size fast splitless injections and compatibility with the scanning speed of quadrupole mass analyzers through the use of high flow megabore (or widebore) columns. The unique capabilities of "Extract-Free Dirty Sample Introduction" with the optional ChromatoProbe sample introduction device and Laser Desorption sampling method are also very important to the issue of fast analysis due to reduced sample preparation requirements.

redball.GIF (649 bytes)  3. Sensitivity

a) HSI provides record low detection limits for a wide range of drugs and aromatic compounds. An ionization efficiency of over 10% was achieved using an experimental system with a MDA of 400 attograms. 
b) Enhanced single ion monitoring (SIM) sensitivity is exhibited in EI due to an enhanced M+. 
c) Large fast splitless injections are possible (i.e. 100 microL) without sample discrimination due to a very high column flow rate of up to 240 ml/min.
d) Noise levels are reduced due to vacuum background elimination and reduced column bleeding through the use of short columns and high flow rates at lower temperatures ("MDA Everyday"). 
e) Large extract sample volumes can be introduced with the unique DSI (ChromatoProbe) device which retains the contaminating matrix components residue in a disposable vial, for lower detected concentration. 

redball.GIF (649 bytes)  4. Scope of use
SMB enables the ultimate scope of use and range of GC-MS applications.

a) Thermally labile molecules are amenable for fast and ultra fast GC-MS analysis. 
b) The highest temperature tailing-free GC-MS combined with enhanced molecular ion information is achieved through background ion filtration and short column fast GC-MS. 

redball.GIF (649 bytes)  5. Selectivity

a) Tunable ionization selectivity is achieved with HSI (>10E+ 5 anthracene/decane). 
b) M+ is enhanced in EI and can be the only MS peak at low electron energy EI. 

This feature of enhanced molecular ion simplifies the deconvolution of overlapping GC peaks using the AMDIS deconvolution software of the NIST library and is thus very important for achieving fast GC-MS. The enhanced selectivity simplifies target and complex mixtures fast GC-MS analyses.

redball.GIF (649 bytes)  6. Flexibility  (and ease of use)

a) Any column can be used without restrictions on its diameter, length and flow rate. This allows the optimal trade-off of GC resolution, speed and sensitivity. (Including the use of the Alltech "multicapillary" high flow rate fast GC column). 
b) Two columns and even two GC's with four columns can be simultaneously connected. (the coupling of two GCs is a non standard option) 
c) The column can be quickly and easily replaced, as in GC-FID, without breaking vacuum. 
d) A unique direct sample introduction (DSI) device provides fast sampling and instant DSI/GC-MS switching. This DSI device also uniquely enables the injection of very "dirty" samples without any sample preparation. (the DSI/ChromatoProbe is an option) 
e) The EI and HSI ion sources are easily interchangeable without breaking vacuum. 
f) A wide range of built-in features and capabilities are included as outlined below.

redball.GIF (649 bytes) redball.GIF (649 bytes) redball.GIF (649 bytes)   The "Super Enhancement Package" redball.GIF (649 bytes) redball.GIF (649 bytes) redball.GIF (649 bytes)

Supersonic GC-MS contains the broadest range of features and capabilities ("Super Enhancement Package") to provide you with cutting edge technology and a competitive advantage. These features are either inherent/standard or optional as marked.

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Enhanced M+ for simultaneous EI+CI information.  (standard)  
Hyperthermal Surface Ionization (HSI). (standard)  
Fast, Very-Fast and Ultra-Fast GC-MS. (standard)  
High flow rate optimal jet separation. (standard)  
Large volume fast splitless injection capability without molecular discrimination. (standard)  
Low electron energy EI for tunable or no fragmentation. (standard)  
Thermally labile compound GC-MS analysis capability. (standard)  
High temperature tail free GC-MS operation. (standard)  
Vacuum background filtration. (standard)  
Flow programming with very high flow rate ratios. (standard)  
Surface Induced Dissociation (SID). (standard)  
Simultaneous multi column and multi GC's capability. (standard, multi GC is an option)  
ChromatoProbe for "extract-free" dirty sample introduction. (option)  
SnifProbe for out of the laboratory aroma, process and air pollution sampling (option)  
Unique cluster CI mode. (option)  
Intra-nozzle deuterium exchange labeling for OH and NH information. (option)  
Intra-nozzle pyrolysis for elemental or functional group selective GC-MS. (option)  
Atmospheric laser desorption injection interface. (option)  
2000 amu quadrupole mass analyzer (Extrel). (option)  
Varian CP 3800 GC with three 1079 injectors and ChromatoProbe. (option) 


3. The Supersonic GC-MS Instrument

In the Supersonic GC-MS the sample is introduced through the Hewlett Packard GC injector as usual. The analytical column output is mixed with about 160 ml/min helium or hydrogen make-up gas and flow through a 20 cm long megabore transfer line to the supersonic nozzle. The make up gas identity, flow rate and transfer line and nozzle temperature are controlled by the ChemStation software. The nozzle is made of alumina ceramic, with a length of ~0.4 mm and a 80 micron diameter. 

The mixture of carrier gas and sample molecules expand through the supersonic nozzle into the first vacuum chamber, which is pumped by a 520 L/min rotary pump. The emerging supersonic free jet is skimmed, differentially pumped by a 60L/sec air cooled diffusion pump, and enters the electron ionization (EI) ion source in the high vacuum MS chamber (60 L/sec air-cooled original HP diffusion pumps). The sample molecules in the beam are ionized by the molecular-fly-through cylindrical EI ion source that allows free passage of the SMB. The ions are extracted by an ion optics lens system attached to the EI ion source and are guided by a 90 degrees ion deflector into a the Hewlett Packard quadrupole mass analyzer (MSD). The 90 degrees ion deflector unit also serves as the hyperthermal surface ionization (HSI) surface with a heated rhenium foil under a high transmission mesh. Computer controlled low flow rate of oxygen keeps the rhenium surface clean. The quadrupole mass analyzer is located 90 degrees relative to the SMB axis and no modification is performed to the HP MSD except in the removal of its ion source. An "exit lens" is added at the exit of the quadrupole, which is a plate with a 5 mm hole, positioned between the quadrupole and the channeltron ion detector. It is used for background ion filtration, by external voltage biasing at the ion energy plus 1-2 eV.

Fast GC is achieved with the 6890 GC without any modification, using split or splitless standard syringe based injections. Alternatively (option), the sample could be loaded in a micro vial with the ChromatoProbe direct/dirty sample introduction device for intra injector thermal desorption. Short columns (3-6 meters long, 0.53 or 0.25 mm ID) with high flow rates (4-200 mL/min) can be used for fast GC and even the Alltech Multicapillary high column flow rate is acceptable without splitting. 

Supersonic GC-MS is designed specifically to bring the supersonic molecular beam GC-MS technology to the public as a commercially available bench-top GC-MS product. This new system design is based on the several basic concepts listed as follows.

1. The industry standard Hewlett Packard bench top GC-MSD serves as the platform for the combination with the supersonic molecular beam technology. This makes it a rugged and reliable platform.
2. The HP 6890 GC is unchanged while the MSD is only slightly modified through the elimination of its EI ion source and transfer line. No irreversible modifications are performed.
3. The SMB pneumatics is fully computer controlled (ChemStation) by the Auxiliary EPC that controls the hydrogen and helium SMB make-up gas as well as the HSI oxygen gas flow rate through an additional low flow rate valve.
4. The GC-SMB nozzle source transfer-line is temperature controlled by the ChemStation. It is heated by the same heater element and temperature sensor as that of the original transfer-line.
5. The transfer-line simultaneously accepts two column outputs that are mixed after a short distance with a high flow rate make up gas (160 ml/min, 22 cm transfer line length). Column replacement is very simple, and does not require a break of the vacuum.
6. The supersonic nozzle is made from alumina with 80 micron diameter by 0.4 mm nozzle length. The nozzle-skimmer position is XYZ controlled and optimized from outside the vacuum.
7. The supersonic nozzle vacuum chamber is pumped by a single 520 L/min Edwards rotary pump. The miniaturized nozzle vacuum chamber requires added bench space of less than 13 cm. A second Convectron vacuum gauge is added to this chamber.
8. The differential pumping chamber is pumped by a single 60 L/sec Edwards air-cooled diffusion pump that is identical to that provided by HP for the third MSD vacuum chamber.
9. The HP provided rotary pump and Convectron vacuum gauge are now connected to the second stage differential pumping chamber and the original diffusion pump is backed by the second stage diffusion pump.
10. A fly-through Electron Ionization (EI) ion source is positioned at the entrance of the MSD vacuum chamber in place of the original transfer-line. It is based on a unique computer optimized third generation design, combined with a high electron emission current for optimized SMB compound ionization. It is powered by a dedicated electronic controller and power supplies.
11. A newly designed HSI surface and surface holder replaces the HP EI ion source. It is also combined with the 90 degrees EI ion mirror. No change was made in the HP ion source house and thus the HP ion source can be re mounted if so desired. Two out of the three original HP ion optics lenses are used, coupled with a new front lens in the coupling to the MSD.
12. The HSI surface is indirectly heated and is at a fixed 45 degrees position to both the SMB and mass analyzer. Oxygen is directed onto the HSI surface from a side slit near it. The surface heater also serves to maintain the mass analyzer above room temperature.
13. The MSD original ion detector is unchanged but an exit lens is added in front of it for background ion filtration.
14. A new electrical feed-throughs connector in a small vacuum chamber is added and placed instead of the original ionization gauge. It also includes a new position for the ionization gauge and a tube for transferring the HSI oxygen gas.
15. A small control board is mounted on the 6890 GC to control the added few components. 

This new Supersonic GC-MS system brings the SMB technology to a user friendly bench top system in a design that targets reliability as a prime consideration.



4. Electron Ionization of Molecules in the SMB

Supersonic expansion of a gas into a vacuum system results in a uniform velocity to all the expanding species. Accordingly, the supersonic expansion leads to low relative velocity collisions of the sample compounds and the carrier gas atoms, resulting in substantial supercooling of the sample compound vibrational temperature to well below 70K. This is like having the ion source at an ultra-low temperature but without condensing the sample compounds. As a result, the level of information contained in the EI mass spectra is greatly increased. We consider EI with SMB to be the ideal ionization method, having an enhanced molecular ion peak and superior detailed molecular and structural information with the following features and advantages: [6, 11, 19]

1. The exact molecular ion peak practically always exists in 70 eV electron ionization (EI) MS with SMB. The relative height of the molecular ion peak is increased by up to several orders of magnitude due to the vibrational supercooling. On the other hand, the conventional EI fragmentation pattern is retained. Actually, the EI-MS of small molecules is relatively unchanged while for large molecules, due to their large vibrational heat capacity, a substantial increase in M+ can be observed.
2. The level of information achieved in a single EI-SMB-MS scan, is greater than that provided by standard EI and CI combined, without the CI problems, and with the uniform high sensitivity of EI to all molecules. This is one of the reasons for our consideration of EI-SMB as the ideal ionization method.
3. Total fragmentation tunability and fragment order of appearance information is achieved through the control of the electron energy. Due to the molecular vibrational supercooling, the electron energy is the only parameter that governs the degree of ion fragmentation. Thus, this control over the degree of fragmentation is achieved with a minimal loss of sensitivity since the reduced electron ionization cross section at low electron energy is compensated for by the reduced degree of fragmentation so that the molecular ion intensity is relatively unchanged.
4. Unique structural and isomeric information is provided due to the vibrational supercooling. Any small isomer mass spectral difference is amplified (sometimes considerably amplified) with EI-SMB.
5. Improved library search and confirmation is achieved due to the molecular weight information by confining the search to library molecules having this molecular weight only. Note that about 30% of the NIST library compounds have no molecular ion (below 2% normalized intensity). This value grows to 50% for compounds with molecular weight over 300 amu.
6. Elemental analysis is possible by accurate isotopic abundance analysis of the relative intensity of the molecular ion group of mass spectral peaks. The features of enhanced molecular ion abundance combined with total lack of residual intra-ion source chemical ionization and reduced vacuum background enable an accurate measurement of the intensity ratios of the molecular ion peaks, resulting in elemental analysis with a unit resolution mass analyzer. If the elemental content is known, then geo-chemical and isotope abundance information is available through the analysis of these molecular ion peak ratios.
7. Deuterium exchange at the supersonic nozzle can be employed (option) for NH and OH labeling. The on-line mixing of the carrier gas with deuterated methanol or heavy water enables effective and fast deuterium exchange before the supersonic expansion. It provides unique structural and isomeric information. 


5. Hyperthermal Surface Ionization

The uniform velocity of all species in the supersonic molecular beam means that the velocities of the carrier gas (hydrogen or helium) and that of the sample molecules are equal. Since the sample compounds are a minor component of the SMB, the velocity of the sample compounds is increased to that of the carrier gas while the carrier gas is only marginally decelerated. Accordingly, the sample compounds are accelerated and their kinetic energy is increased, by about the mass ratio of the sample compound and the carrier gas, to the hyperthermal kinetic energy range of 1-30 eV. Thus, the kinetic energy of the sample molecule increases with its molecular weight and the nozzle temperature and it is reduced by increasing the carrier gas atomic or molecular weight.
We have found that the surface ionization yield of organic molecules acquired with hyperthermal kinetic energy is increased by many orders of magnitude relative to thermal surface ionization and it can be up to three orders of magnitude higher than EI. This phenomenon of hyperthermal surface ionization (HSI) was discovered by Amirav and Danon [1, 2, 6] and studied in detail from its various mechanisms through its analytical applications [4, 7-10, 12, 16, 19, 20].

HSI is based on a molecule-surface electron transfer process which is promoted by the image potential formed between the ion and the surface. This image potential facilitates the molecule-surface electron transfer and ionization process. The molecular ionization requires the energy difference between the molecular ionization energy and the surface work function (surface ionization energy). When an ion approaches the surface, an image potential is formed between the ion and surface. This image potential reduces its potential energy that can be lower than that of the scattered neutral compound at a given distance from the surface. This critical distance is called the curve crossing distance (Rc). Below this distance a spontaneous electron transfer from the molecule to the surface may occur and can be calculated using a modified Landau Zenner curve crossing equation. If the sample compound has hyperthermal kinetic energy above the thermodynamic energy requirement, it can be scattered as an ion from the surface. Since a portion of the molecular kinetic energy is lost, either to the surface or to internal vibrational degrees of freedom, most of the ionized compounds are reneutralized. As a result, the ionization efficiency is dramatically increased with the molecular kinetic energy, since an increased portion of the scattered ions have sufficient kinetic energy to overcome the image potential in their exit trajectories. Other HSI mechanisms, including negative ion HSI, are described in references 2 and 6 but the mechanism briefly described above is analytically the most significant.

The degree of ionization also depends on the surface work function and molecular ionization energy. Rhenium oxide has proven to be an ideal surface for HSI as it combines a high work function with excellent long term stability that is essential for analytical applications. This is achieved by the direct current heating of a rhenium foil to about 1000K while bleeding oxygen on it at a partial pressure of 2-3x10-5 milliBar. As a result, the oxygen catalyticaly combusts all the organic surface impurities and maintains a steady state of surface cleanliness.
We found that HSI can serve as a universal, ultra sensitive ion source with tunable selectivity that is ideal for compounds with low ionization energies such as drugs and aromatic compounds. This tunable selectivity was demonstrated combined with the very high HSI yield that is estimated to be over 10% at the surface, and about 2% for the ratio of ions at the surface to nozzle flux (assuming 20% jet separation efficiency).

While HSI provides molecular ions only for polycyclic aromatic hydrocarbons, the HSI mass spectra are usually characterized by a rich and informative fragmentation pattern. The degree of HSI fragmentation naturally depends on the compound but it also depends on the molecular kinetic energy. The HSI fragments usually correspond to those which appear in EI mass spectra albeit with different relative peak intensities. In some cases, such as with cocaine, the HSI MS can be identified by the NIST EI library. In other cases a HSI library must be built and can be effective.

In summary, HSI is characterized by the following two major features and advantages:

A) Increased Sensitivity.
Hyperthermal surface ionization is the most sensitive ion source for  positive ion formation due to:

1.

Very high ionization efficiencies of over 10% (100 Coulomb/gram). 
2. The background of the vacuum chamber molecules is reduced or eliminated since they do not possess the required  hyperthermal kinetic energy. 
3. For many important classes of molecules such as drugs, amines, PAH's etc., only a single molecular or fragment ion appears. 

Minimum detected amount of 400 attograms was demonstrated in an experimental system.

B) Tunable Ionization Selectivity.
The hyperthermal surface ionization yield depends on the surface  work-function, sample molecule and molecular kinetic energy. These parameters can be easily controlled through the choice of the carrier gas such as helium, hydrogen or their mixture (on-line prepared with the ChemStation), the nozzle temperature and/or the choice of surface such as rhenium oxide or molybdenum oxide. Over 1E+5 anthracene/dodecane selective ionization was achieved. The high selectivity may involve only a minor ionization yield reduction of the selected molecules. Selective ionization can help to simplify complex mixture analysis and opens the door for a much faster GC-MS analysis, such as of cocaine in a single hair [20].



6. Fast and Ultra-Fast GC-MS

The unique features of SMB-MS enable a fast GC-MS which provides a complete solution for all the requirements of an optimized, high performance, fast, high temperature and thermolabile compatible GC-MS. The HP 6890 GC serves for fast GC-MS, connected to the SMB nozzle with two columns simultaneously, having no limitations on the column ID, length or flow rate. In this way the conventional GC becomes a fast GC-MS inlet that comprises a new approach for fast GC-MS. The subject of fast GC-MS with SMB is discussed in detail in a recent paper and review [17, 19] (available upon request).
In contrast to the microbore column based fast GC-MS, our approach offers a much better solution to all the requirements of fast GC-MS, from sample preparation to data analysis in that:

1. Fast injection is achieved with a conventional syringe, even for relatively nonvolatile compounds, due to the very high injector flow rate (up to 240 ml/min).
2. High repetition rate fast injection can be achieved with laser desorption injection (option) in an atmospheric or helium purged compartment provides the ultimate automated high repetition rate sample injection method.
3. A unique extract free dirty sample introduction method and device (ChromatoProbe, option), enables a true fast analysis including the step of sample preparation.
4. Fast analysis is achieved with samples having a very wide boiling point range, due to simple and fast column flow programming up to 2000 cm/sec carrier gas velocity. This unique column flow programming enables the widest column flow programming dynamic range.
5. A wide temperature range fast GC-MS is achieved with appropriate columns heated up to 460 C and without any ion source related peak tailing.
6. GC-MS of thermally labile compounds is achieved with the very fast and ultra fast GC-MS for molecules that are usually probed by particle beam or APCI LC-MS (ultra fast injection, on-column injection, short column, high carrier gas linear velocity and no ion source dissociation).
7. Compatible mass scanning rate is enabled, even with the quadrupole mass analyzer. The reduced number of separation plates associated with the use of a high flow rate short megabore column results in a normal peak width of ~ 1 sec after ~5-10 seconds which does not require TOF-MS. Thus, the quadrupole mass analyzer can be used.
8. Sufficient overall GC-MS resolving power is provided, even for complex mixture fast analysis. The GC column time separation and MS resolving power are supplemented by a tunable selective hyperthermal surface ionization, or low electron energy EI-SMB which produces a dominant or only M+ (orthogonal MS separation). Thus, many target compounds can be  analyzed in a few seconds in real world complex mixtures.
9. Ultra fast ion source response time exists with SMB, which allows the monitoring of tail free fast GC peaks originating even from relatively nonvolatile molecules.
10. Very high sensitivity is achieved with hyperthermal surface ionization. This sensitivity can be translated into simpler sample preparation for faster analysis.
11. Superior low concentration sensitivity is achieved with more than 1 microLiter fast splitless injections due to the high column flow rate. This is in marked contrast to microbore column fast GC-MS. Fast splitless injections also enable significantly faster temperature programming and GC cooling down time since the initial GC temperature can be much higher!.
12. Resolution, time and sensitivity trade-off choice is enabled for optimal results. The coupling with a conventional GC is allowed without any constraints on the column diameter, length and carrier gas flow rate. Thus, critical parameters such as chromatographic time and resolution can be optimized, with regards to and in consideration of the desired injected sample amount. This is easily achieved due to the practically unlimited column flow allowable. The recently introduced multi-capillary fast GC column from Alltech, with its very high column flow rate requirement, is ideally coupled with the SMB-MS. 

Improved Conventional GC-MS Flexibility and Capabilities
While fast GC-MS is ideally suited for the fast screening of a large number of samples, confirmation is also needed, preferably with the same GC-MS instrument. Supersonic GC-MS provides this highly desirable feature, supplementary to fast GC-MS, and can be configured with both a standard analytical and a short column which are simultaneously connected to the SMB interface. In addition, Supersonic GC-MS provides several advantages over standard GC-MS that make it a higher capability GC-MS. It provides increased available level of MS information, enhanced molecular ion peak, HSI, higher temperature operation and the many unique features mentioned above. Further contributions include:

1. Any column diameter and length can be used for optimized trade-off of chromatography parameters such as injection volume, speed of analysis and chromatographic resolution. (faster GC-MS instead of fast GC-MS)
2. Flow programming of the GC can be used without any flow limitations. Thus, the injection and analysis time of the standard chromatography can be considerably reduced. (Faster GC-MS instead of fast GC-MS)
3. A very large amount of solvent can be injected  (i.e. 100 microLiter splitless) with an injection time of 4 microLiter/sec. Large volume injections directly improve the achievable minimum detected concentration which is actually the required parameter in most analyses. Moreover, unlike with standard PTV, the high flow rate amenable with SMB enables direct injections into the column, without the split related compound discrimination that occurs with standard PTV. Note, that while the large column flow reduces the injection time, the differential pumping protects the MS from the solvent.
4. All of the available GC injectors can be used with different columns (type, ID and length) that can be simultaneously connected to the nozzle for higher analysis flexibility.
5. Column replacement does not require opening of the vacuum chamber.
6. (Option) One injector can be converted into a direct sample introduction device (ChromatoProbe) combined with a high flow short column as a transfer line. 
7. An effective coupling with an external purge and trap or thermal desorption system can be achieved due to the high flow allowed.
8. The two ion sources EI-SMB  and HSI are interchangeable without breaking vacuum.


7. Sensitivity Considerations and Evaluation

At this time sensitivity specifications are available only upon request and the general discussion pertains to the experimental apparatus at Tel Aviv University. It can serve as an initial guideline.

Hyperthermal surface ionization is the most sensitive ion source for positive ion mass spectrometry due to:

1. Very high ionization probabilities of over 10% (100 Coulomb/gram).
2. Background of the vacuum chamber molecules is largely reduced since they do not possess the required hyperthermal kinetic energy.
3. In many important classes of molecules such as drugs, amines, PAH's, organo halogens etc., only a single molecular or fragment ion appears.
4. As a selective ionization method much of the matrix interference is eliminated with HSI.

Minimum detected amount of 400 attograms was demonstrated with the experimental apparatus.

Electron Impact ionization in SMB is about as sensitive as the conventional EI. The reduced ionization probability of the faster molecules in the SMB and the inherent jet separation losses are compensated for by:

1. Background ion filtration through the use of the directional molecular hyperthermal kinetic energy before ionization for the discrimination against the thermal vacuum background ions.
2. Higher electron emission current is possible with the open EI ion source (up to 15 mA), combined with multiple path electron trajectories through the open ion source cage. This feature originates from the background filtration of thermalized or heated molecules in the open ion source.
3. The relative abundance of the molecular ion can be increased by up to several orders of magnitude. This feature is of particular importance with single ion monitoring or computer reconstructed SIM on the molecular ion.

Minimum detected amount of 60 femtograms was demonstrated with single ion monitoring of the molecular ion peak of eicosane with the experimental apparatus.

Unique Supersonic GC-MS and Fast Supersonic GC-MS further contributes to enhanced sensitivity through:

1. Fast GC-MS with a supersonic molecular beam results in narrower GC peak width (about 1 sec) and therefore higher peak molecular flux. The use of a short column proportionally reduces the amount of background from column bleeding that is further reduced at the high flow rate lower temperature  fast Supersonic GC-MS operation.
2. Large sample volumes can be injected splitless with a conventional or fast GC for achieving a lower detected concentration limit. 
3. Larger extract sample volumes can be introduced with the optional direct sample introduction device (ChromatoProbe) without column and liner contamination, for achieving a lower detected concentration limit.


8. The Analysis of Thermally Labile and Relatively Non Volatile Compounds

The use of SMB for sampling and ionization considerably increases the scope of use of GC-MS and broadens the range of compounds amenable for such analysis in two areas:

A)  Thermolabile GC-MS
The analysis of thermally labile molecules is considerably improved in comparison with conventional GC-MS owing to the following reasons:

1. On column (megabore) -temperature programmable injection can be coupled with very high carrier gas flow rate to minimize both the injector temperature during the vaporization, and the residence time at the injector.
2. The very short column length and very high carrier gas flow rate minimizes thermal dissociation in the column.
3. The vibrational supercooling and fly-through EI ion source eliminate both molecular decomposition and molecular ion dissociation in the ion source. 

When these three elements are combined, fast GC-MS with the Supersonic GC-MS can be considered equivalent to, or in some cases even softer than particle beam LC-MS which involves high temperature thermal vaporization from reactive metal surfaces in the EI ion source [14].

B)  The Highest Temperature Tailing-Free GC-MS
Tailing-Free GC-MS is achieved without any mass spectrometric ion source related limitations. The vacuum background elimination processes ensures tailing-free GC at any temperature, and the fly-through EI ion source provides an enhanced M+ due to the vibrational supercooling. Currently, the limitation is 460 C with the SGE-HT-5 column. Note that the combination of short column and 2000 cm/sec potential column flow velocity, further extends the range of non volatile molecules amenable for GC-MS analysis.



9. Applications of Supersonic GC-MS and Fast GC-MS

Supersonic GC-MS and fast GC-MS excel in a wide range of applications due to the broad range of advantages and unique features available as listed in section 2. Accordingly, in any non-standard applications it can replace the available standard instrumentation and provide a competitive advantage. A list of a few major such applications include:

1. Petroleum-MS.
Petrochemical analysis should benefit from many of the unique features of SMB-MS including molecular ion information in alkanes, molecular ion only MS at low electron energies EI, unique isomer information, aromatic selective detection and higher temperature GC-MS.
The added information can quickly be translated into saved money.

2. Forensic Analysis
The system flexibility and broad range of new capabilities are all important for a variety of forensic applications including fast GC-MS of thermally labile explosives, molecular ion information for arson investigations, trace level of drug detection with HSI and including the optional ChromatoProbe serving as a probe for dirty samples.

3. Clinical Toxicology - Screening of Drugs in Urine.
The sensitivity and selectivity of HSI combined with fast GC-MS enables the injection of small samples of untreated urine for drug screening in a few minutes from the sample to the results. This can turn Supersonic GC-MS into a potential competitor for the multi-billion Dollar market of drug screening in urine that is currently dominated by immunoassay techniques. The same GC-MS with a second longer column can serve for confirmation, featuring enhanced M+ in EI. In some cases the exceptional sensitivity of HSI will enable the detection of ultra trace levels of drugs in plasma and urine extracts. A unique capability of fast drug detection in a single, untreated human hair opens up many new possibilities.

4. Process Control.
The very fast analysis capability and selectivity enable simple and effective process control.

5. GC-MS research and General Organic and Inorganic Mass Spectrometry.
The easy to use ChromatoProbe direct sample introduction (Option), fast GC-MS capability, extended temperature range, enhanced molecular ion peak, isotope and elemental information, tunable fragmentation, possible choice between two columns without any hardware change and many other features are all important to this application.

6. Environmental Analysis.
The analysis of thermally labile pesticides (carbamates) is important application. Environmental analysis can further benefit from improved sensitivity with HSI in the analysis of PAH's, large splitless injection capability, fast GC-MS screening ability and enhanced M+. The optional DSI device (ChromatoProbe) enables extract free pesticide analysis in fruit, vegetables, spices and other food items.



10. Direct/Dirty Sample Introduction Device (ChromatoProbe)

A unique (US patent) Direct Sample Introduction (DSI) device was developed by us which is especially suitable for use with Supersonic-GC-MS. This "ChromatoProbe" serves for three major applications, each with many advantages. A dedicated booklet is available upon request with detailed description of ChromatoProbe, SnifProbe and its applications.

1. Direct Sample Introduction for Mass Spectrometry Studies.  
The ChromatoProbe, effectively transforms a conventional GC injector, (second GC injector in the GC-MS) followed by a short column, into a cost-effective alternative to the standard direct probe. It possesses the advantages of faster and easier operation, faster ChromatoProbe/GC-MS interchange, capability of sampling solutions, possible use as a micro-chemical (derivatization) reactor and easy conversion into a fast GC-MS channel.
2. Extract-Free Dirty Sample Introduction For GC-MS Analysis.  
This new method is based on sampling in a micro vial that retains the harmful and non-volatile matrix residue of real world samples. Thus, it eliminates the need for further sample clean-up, while the test tube is a disposable item. Each analysis begins with gentle solvent vaporization, preferably at a relatively low injector temperature such as 120 C for water/urine (20 C above the solvent boiling temperature), followed by brief injector heating to the temperature required for achieving effective intra injector thermal extraction and sample compound vaporization. The sample semi-volatile compounds are focused on the early portion of the column and are analyzed by the chromatography as usual. This method brings the many known advantages of thermal extraction in an easy to use low cost fashion, combined with the many advantages of SMB-MS. It facilitates extract free analysis of drugs in urine or hair, or pesticides in blended fruit and vegetable items, or in milk, juice and slurries. The DSI also uniquely allows large size sample injections of conventional extracts without the associated residues that usually restrict the sample size, and thus lower detected concentration limits can be achieved. The containment of the non-volatile compounds in the disposable test tube also results in faster analysis that can end at a lower column temperature.
3. SnifProbe Gas Analysis  
SnifProbe (option) is based on the use of 15 mm short pieces of standard 0.53 mm ID capillary or PLOT column for sampling air born, head space, aroma or air pollution samples. Thus, SnifProbe extends the ChromatoProbe range of samples that now also includes gas phase samples. The short (15 mm) column is inserted into the SnifProbe easy-insertion-port and the SnifProbe is located or aimed at the sample environment. A miniature pump is operated for pumping 6-60 ml/min of air sample through the sample collection short piece of column. After a few seconds of pumping, the short column is removed from the SnifProbe with tweezers and placed inside a ChromatoProbe glass vial having a 0.5 mm hole at its bottom. The ChromatoProbe sample holder with its glass vial and sample in the short column are introduced into the GC injector as usual. The sample is then quickly and efficiently vaporized from the short sample column and is transferred to the analytical column for conventional GC and or GC-MS analysis.  
SnifProbe enables many of the manual SPME, air bags and Tenax tube applications, with a few advantages. SnifProbe is ideal for field or process operation, it is small, enables fast sampling, compatible with the full range of semi volatile compounds and enables low cost sensitive analysis.

Note that the combination of Supersonic GC-MS with the ChromatoProbe (DSI) is especially effective since:

1. The high injector splitless carrier gas flow rate enables larger sample volume in the ChromatoProbe vial to be vaporized in a shorter amount of time for higher sensitivity analysis. 
2. The ChromatoProbe enables fast sampling with minimal sample preparation that is ideally coupled with the fast GC-MS analysis enabled by the Supersonic GC-MS.
3. The high injector carrier gas flow rate enables the ChromatoProbe sampling of thermally labile compounds, at lower injector temperatures.
4. The high carrier gas flow rate used with the Supersonic GC-MS enables the use of a single medium length column both as a transfer-line for probe type MS measurements and as a short analytical column for fast GC-MS without any change of hardware. (for example 6 meter, 0.25 mm ID column) 
5. When the ChromatoProbe vial is taken out the column is fully protected from any air leak into the column by the high flow-rate helium make up gas. In addition, the end of the analytical column is at ambient pressure (or slightly above it) and thus no air penetration into the column is even possible. 


11. Laser Desorption Fast GC-MS

An important additional aspect of fast GC-MS pertains to the issue of high repetition rate automated sample injection method. The quest for such a method is further complicated by the need to achieve it for a large variety of samples, on/in a variety of complex matrices, and without sample preparation. Today, automated sample injection is performed with an autosampler that is capable of performing about one injection per minute. It is also limited to relatively clean samples, in the form of liquid solutions (or gases) introduced in crimped vials that are located on a sample tray. As a result, the standard autosampler is practically incompatible with the majority of ultra-fast GC-MS analyses, and a new and much faster injection method is desirable for ultra-fast GC-MS.
The use of focused or slightly defocused laser light for sample desorption and volatilization seems to be the ideal injection method for ultra-fast GC-MS, comprising several inherent desirable features [18] including:

1. High repetition rate automated injection is enabled. With laser desorption injection, the chromatography is the limiting time step since 10 Hz laser operation is standard.
2. Sample preparation is eliminated through the ability to reproducibly desorb and inject a very small sample amount that does not require further clean up.
3. Laser desorption injection can uniquely provide an additional dimension of spatial information  for two dimensional surface chemical mapping. For this purpose, ultra-fast analysis is clearly essential, otherwise the total mapping time could be prohibitively long.
4. Laser desorption injection is especially suitable for the analysis of of organic compounds on surfaces, while it can also be used for drilling into the bulk of solids in order to achieve an additional dimension of information. 

The subject of laser desorption for analytical purposes is not new, and matrix assisted laser desorption ionization is a major subject of research today. However, most of the laser desorption schemes are based on laser desorption of samples that are placed inside the mass spectrometer vacuum chamber. Our recently developed novel method of laser desorption is based on the “injection” of samples placed at ambient atmospheric pressure, either under helium purging conditions or in the open air [18]. The laser desorption unit was mounted on a home made ultra-fast GC-MS injector inlet, with a thermally insulated clamp and mounting rod. The sample was placed on the sample holder, located inside the sample compartment. The laser used was a pulsed XeCl Excimer laser with 30-50 mJ 308 nm laser pulses of about 12 nsec duration. The laser pulse energy at the sample was only 3-5 mJ due to its energy reduction through the light transfer optics. The laser pulses were controlled by a pulser and either a single laser pulse or a train of typically 20 pulses at a repetition rate of 50 Hz was employed for 0.4 sec injection time. The laser light was softly focused on the sample with about a 0.1 mm desorption point diameter. After laser desorption, the sample vapor or particles were swept by a helium carrier gas that was provided by a tube above the sample. This sweeping helium gas also served as both a purge gas and fast GC carrier gas. A very high carrier gas flow rate of over 300 ml/min was essential for achieving effective and fast laser desorption injection, since, depending on the laser pulse energy, the desorbed sample volume could be over 1 ml. The thermal insulation of the sample from the separately heated injector enabled the analysis of relatively volatile compounds. The laser desorbed vapor and particles were further transferred through a glass frit filter that prevented nozzle clogging and also acted as a thermal vaporizer for the sample particles. After the glass frit, the sample passed through a 50 cm long megabore column that enables ultra-fast GC separation, followed by supersonic expansion, ionization and mass analysis as described throughout this document.
The application of laser desorption fast GC-MS analysis was employed and studied by us using a variety of samples and matrices, including: a) The analysis of dioctylphthalate oil (and its cleaning procedure) on a stainless steel surface; b) The analysis of methylparathion and aldicarb pesticides on an orange leaf; c) The analysis of methylparathion pesticide on the surface of liquid water. d) The analysis of paracetamol and codeine in a tablet; e) The analysis of lidocaine at one ppm level in coagulated blood.

The Laser desorption inlet is proposed only as an optional inlet system that requires some further R&D for its coupling with the HP 6890 GC and with a new laser system.



12. Links

Enclosed are a few links for some of the technologies and components that are used in the Supersonic GC-MS and/or   that could be used in its current or future options.

1.

2.

3.

4.

5.

6.

7.

8.

9.

10.

HP 6890 Plus GC

HP 5973A Mass Selective Detector

Varian ChromatoProbe

Varian Model 3800 Gas Chromatograph

ABB Extrel Quadrupole Mass Analyzers

Professor Amirav home page at Tel Aviv university

Pulsed flame photometric detector (PFPD) for gas chromatography.

Electrolyzer powered Flame Ionization Detector (EFID) - The gas cylinder free FID.

Extract-free Dirty Sample Introduction (DSI) device (ChromatoProbe and SnifProbe)

LC-MS with supersonic molecular beams.



13. References *(recommended for reading as a review)

1. A. Danon and A. Amirav. "Kinetic Energy Induced Surface Dissociative Ionization". J. Chem. Phys. 86, 4708-4709 (1987).  
This is the first HSI paper.
2. A. Danon and A. Amirav. "Molecular Ionization and Dissociative Ionization at Hyperthermal Surface Scattering". J. Phys. Chem. 93, 5549-5562 (1989).  
Detailed study of HSI with its mechanisms.
3. A. Amirav and A. Danon. "Electron Impact Mass Spectrometry in Supersonic Molecular Beams". Int. J. Mass Spectrom and Ion Proc. 97, 107-113 (1990).
4. A. Danon and A. Amirav. "Hyperthermal Surface Ionization - A Novel Ion Source with Analytical Applications". Int. J. Mass Sepctrom and Ion Proc. 96, 139-167 (1990).
5. A. Amirav. "Processes in Hyperthermal Molecule Surface Scattering". Invited Review, Comments. At. Mol. Phys. 24, 187-211 (1990).
*6. A. Amirav. "Electron Impact and Hyperthermal Surface Ionization Mass Spectrometry in  
Supersonic Molecular Beams". Invited Review - Org. Mass. Spectrom 26, 1-17, 1991.
7. S. Dagan, A. Danon and A. Amirav, "Collision Activated Dissociation in Hyperthermal Surface Ionization Mass Spectrometry of Cholesterol", Int. J. Mass Spectrom & Ion Proc. 113, 157-165 (1992).
8. A. Danon and A. Amirav, "Isotope, Molecular and Surface Effects on Hyperthermal Surface Induced Dissociative Ionization", Int. J. Mass. Spectrom & Ion. Proc., 125, 63-74 (1993).
9. S. Dagan and A. Amirav, "High Efficiency Surface Induced Dissociation on a Rhenium Oxide Surface", J. Am. Soc. Mass. Spectrom. 4, 869-873 (1993).
10. S. Dagan and A. Amirav, "Fast, High Temperature and Thermolabile GC-MS in Supersonic Molecular Beams", Int. J. Mass Spectrom. & Ion. Proc., 133, 187-210 (1994).
*11. S. Dagan and A. Amirav, "Electron Impact Mass Spectrometry of Alkanes in Supersonic Molecular Beams"  J. Am. Soc. Mass Spectrom. 6, 120-131 (1995).
12. S. Dagan, A. Amirav and T. Fujii, "Surface Ionization Mass Spectrometry of Drugs at the Thermal and Hyperthermal Energy Range - A Comparative Study". Int. J. Mass. Spectrom & Ion. Proc. 151, 159-165 (1995).
13. S. Dagan and A. Amirav "Cluster Chemical Ionization and Deuterium Exchange Mass Spectrometry in Supersonic Molecular Beams". J. Am. Soc. Mass. Spectrom., 7, 550-558 (1996).
14. S. Dagan and A. Amirav, "Fast, Very Fast and Ultra Fast GC-MS of Thermally Labile Steroids, Carbamates and Drugs in Supersonic Molecular Beams". J. Am. Soc. Mass. Spectrom., 7, 737-752 (1996).
15. A. Amirav and S. Dagan, "A Direct Sample Introduction Device for Mass Spectrometry Studies and GC-MS Analysis", Europ. Mass. Spectrom. 3, 105-111 (1997).
16. S. Dagan and A. Amirav, "Fast GC-MS Analysis of Drugs in Urine with Hyperthermal Surface Ionization in Supersonic Molecular Beams",  Europ. Mass. Spectrom. 4, 15-21 (1998).
17. A. Amirav, N. Tzanani, S. Wainhaus and S. Dagan,  "Megabore versus Microbore as the Optimal Column for Fast GC-MS", Europ. Mass. Spectrom. 4, 7-13 (1998).
18. T. Shahar, S. Dagan and A. Amirav, "Laser Desorption Fast GC-MS in Supersonic Molecular Beams", J. Am. Soc. Mass. Spectrom. 9, 628-637 (1998).
*19. A. Amirav, S. Dagan, T, Shahar, N, Tzanani and S. B. Wainhaus. “Fast GC-MS With Supersonic Molecular Beams” A Review Chapter number 22, pages 529-562 in the book “Advances In Mass Spectrometry” Volume 14, E. J. Karjalainen Editor, Elsevier Science Publeshers, Amsterdam 1998.
20. S. B. Wainhaus, S. Dagan, M. L. Miller and A. Amirav, “Fast Drug Analysis In A Single Hair”, J. Am. Soc. Mass. Spectrom. 9, 1311-1320 (1998). 


In a book "Supersonic Molecular Beam Mass Spectrometry - The Quest for Ultimate Performance GC-MS and Fast GC-MS" the Supersonic GC-MS technology is described and demonstrated through 51 figures and many applications.
This book is available free on request.
You may ask for it at:  amirav@supermass.co.il.
Please add a brief description of your application and range of GC-MS interests.

We shall be delighted to try your samples and meet your requirements so that you could closely evaluate the suitability of Supersonic GC-MS to solve your needs.  Please challenge us at: amirav@supermass.co.il.
 

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