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Miniature DMS-IMS detector for enhanced revolving power Abstract ...

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IJ<strong>IMS</strong> 10(2007)1 - 5<br />

<strong>Miniature</strong> <strong>DMS</strong>-<strong>IMS</strong> <strong>detector</strong> <strong>for</strong> <strong>enhanced</strong> <strong>revolving</strong> <strong>power</strong><br />

E.G. Nazarov * , A.G. Anderson * , E.V. Krylov * , S. L. Coy * , R.A. Miller * , D. Burchfield @ ,<br />

and G. A. Eiceman#<br />

* Sionex Corporation, Bed<strong>for</strong>d, MA<br />

@ Hamilton Sundstrand, Pomona, CA.<br />

# New Mexico State University, Las Cruces, NM.<br />

<strong>Abstract</strong><br />

Ion mobility based gas analyzers provide high sensitivity detection and identification of<br />

trace levels of ions in gases. Because these analyzers operate at ambient pressure, they<br />

are of reduced complexity and suitable <strong>for</strong> field applications. However, dealing with the<br />

real world complexity of mixtures, field applications continue to be a challenge.<br />

Currently there are two types of ion mobility based gas analyzers. These are based on<br />

Ion Mobility Spectrometer (<strong>IMS</strong>) and Differential Mobility Spectrometer (<strong>DMS</strong>) technologies.<br />

The two methods operate on different principles of ion separation. In <strong>IMS</strong>, ion<br />

species separation is a function of the coefficient of mobility (K 0 ) of the ions, resulting in<br />

different drift times. In <strong>DMS</strong>, ion separation is a function of the electric-field-dependence<br />

of mobility ((E) parameter). For <strong>enhanced</strong> ion identification it is desirable to use the value<br />

of the comprehensive mobility coefficient, K(E) = K 0 (1+(E)). Combining <strong>DMS</strong> and <strong>IMS</strong><br />

will take advantage of complementary data on a given ion species and enhance chemical<br />

identification.<br />

The new Sionex portable tandem <strong>DMS</strong>-<strong>IMS</strong> instrument includes a <strong>DMS</strong> <strong>for</strong> rapid separation<br />

of positive and negative ions, and two short (1.5cm) <strong>IMS</strong> drift tubes <strong>for</strong> further resolution<br />

of <strong>DMS</strong> pre-filtered ions. The sensor system is compact; measuring only<br />

2"×2.5"×3". The design has been optimized through computer modeling using the<br />

Sionex-proprietary microDMx TM modeling software package. In the tandem system,<br />

<strong>DMS</strong> provides compensation voltage (Vc) separation while the <strong>IMS</strong> provides drift time<br />

separation. Figure 4 shows a <strong>DMS</strong>-<strong>IMS</strong> images <strong>for</strong> positive toluene ions in nitrogen (left<br />

frame, 45ppb) and in air (right frame, 17.5ppb). The right frame shows that in air, toluene<br />

<strong>for</strong>ms four ion species that can be resolved using the tandem system. The current prototypes<br />

have high sensitivity (ppb level) <strong>for</strong> a wide range of chemicals including CWA simulants,<br />

explosives, TICs, TIMs, and environmental pollutants.<br />

Introduction<br />

An ion mobility spectrometer includes stages <strong>for</strong> ionization, ion separation by electric<br />

field and ion current measurement. Ion separation is based on the ion mobility coefficient.<br />

Two main types of ion mobility spectrometers are most popular at present: the low-field<br />

Ion Mobility Spectrometer (<strong>IMS</strong>, Figure 1 top right) and the Differential Mobility Spectrometer<br />

(<strong>DMS</strong> Figure 1 top left). The two devices operate on different principles of ions<br />

separation. In <strong>IMS</strong>, ion species are separated by their coefficient of mobility 1 (K 0 ). In<br />

<strong>DMS</strong> ion species are separated by their field mobility dependence 2 ((E)). Enhance resolving<br />

<strong>power</strong> results if the ion mobility based gas analyzers utilize both K 0 and (E) properties<br />

<strong>for</strong> ion separation. Combining <strong>DMS</strong> and <strong>IMS</strong> 3 takes advantage of the comprehensive<br />

coefficient mobility, K(E) = K 0 (1+(E)). Prototype of Sionex <strong>DMS</strong>-<strong>IMS</strong> 2 tandem system<br />

(Figure 1, bottom) provides this complementary ion in<strong>for</strong>mation.


IJ<strong>IMS</strong> 10(2007)1 - 6<br />

Experimental<br />

The new Sionex portable tandem <strong>DMS</strong>-<strong>IMS</strong> 2 instrument (Figure 2, left) has two steps of<br />

ions separation: on the first, <strong>DMS</strong> provide pre-separation of positive and negative ions<br />

according differential mobility , and then two short (1.5cm) <strong>IMS</strong> drift tubes (one <strong>for</strong> each<br />

ion polarity) provide further separation according absolute value of ion species mobility.<br />

The sensor system is compact, measuring only 2"×2.5"×3". The design has been optimized<br />

through computer modeling using the Sionex-proprietary microDMx TM modeling<br />

software package (Figure 2, right). The <strong>DMS</strong> section provides compensation voltage<br />

(Vc) separation all ion species <strong>for</strong>med in ionization region while the two orthogonal located<br />

<strong>IMS</strong> provide drift time (DT) separation <strong>for</strong> both positive and negative ions simultaneously.<br />

Results and Discussion<br />

Since the trend lines of the mass resolution (Figure 3, left) <strong>for</strong> the <strong>IMS</strong> 1 and <strong>DMS</strong> 4 are<br />

quasi-orthogonal, a <strong>DMS</strong>-<strong>IMS</strong> tandem system has <strong>enhanced</strong> <strong>power</strong> <strong>for</strong> ions specie identification.<br />

Figure 3 ( right frame) shows that the combination in<strong>for</strong>mation obtained in the<br />

first and second steps and presented in two-dimensional space (drift time vs. compensation<br />

voltage) provides the <strong>enhanced</strong> resolving <strong>power</strong> of the <strong>DMS</strong>-<strong>IMS</strong> system. Combined<br />

with possibility to scan of the separation voltage (RF voltage) in the <strong>DMS</strong>, the<br />

analytical space can be extended to three-dimensional, and provide further in<strong>for</strong>mation<br />

related to ions fragmentation too.<br />

Figure 4 shows <strong>DMS</strong>-<strong>IMS</strong> 2-D spectra <strong>for</strong> positive toluene ions in nitrogen (left, 4.5ppb)<br />

and in air (right, 17.5ppb). The left frame shows that in air, toluene <strong>for</strong>ms four ion species<br />

which do not be resolved in each of segments of system, but using the tandem system<br />

all these species can be detected and resolved independently.<br />

Conclusions<br />

<strong>DMS</strong>-<strong>IMS</strong> tandem provides the complementary chemical in<strong>for</strong>mation provided by a<br />

<strong>DMS</strong>-<strong>IMS</strong> tandem systems improves the confidence level <strong>for</strong> detection, separation, and<br />

identification of ion species in real-world situations. The current prototypes have high<br />

sensitivity (ppb level) <strong>for</strong> a wide range of chemicals of current practical interest, including<br />

CWA simulants, explosives, TICs, TIMs, and environmental pollutants.<br />

References<br />

[1] Mason E.A.; McDaniel E.W.; Transport Properties of Ions in Gases. 1988, Wiley, New York.<br />

[2] Buryakov I.A.; Krylov E.V.; Nazarov E.G.; Rasulev U.Kh., Int. J. Mass Spectrom. Ion Proc., 1993,<br />

128, 143-148.<br />

[3] Anderson A.G.; Krylov E.K.; Nazarov E.G.; Miller R.A.; Coy S.L., PITTCON, February 2007,<br />

Chicago, USA, p.59.<br />

[4] Krylov E.; Nazarov E.G.; Miller1 R.A.; Tadjikov B.; Eiceman G.A., Journal of Physical Chemistry A.<br />

2002, 106(22), 5437-5444.


IJ<strong>IMS</strong> 10(2007)1 - 7<br />

Figures<br />

<strong>DMS</strong> = Adjustable Ion Filter<br />

<strong>IMS</strong> = Time-of-Flight Spectrometer<br />

Peak position (CV) depends on {(E); SV} Peak position (DT) depends on {K 0 ; E; L}<br />

<strong>DMS</strong>-<strong>IMS</strong> tandem<br />

Peak position depends on {(E); K 0 ; Vc; E}<br />

Figure 1. Differential Mobility Spectrometer (<strong>DMS</strong>) (top left); drift-tube Ion Mobility<br />

Spectrometer (<strong>IMS</strong>) (top right) and <strong>DMS</strong>-<strong>IMS</strong> tandem (bottom).<br />

Figure 2. Sionex portable tandem <strong>DMS</strong>-<strong>IMS</strong> instrument (left). Optimization tandem<br />

system with microDMx TM modeling software (right).


IJ<strong>IMS</strong> 10(2007)1 - 8<br />

Figure 3. Trend lines of <strong>DMS</strong> and <strong>IMS</strong> mass resolution (left). Simulation of the<br />

combined analytical space of <strong>DMS</strong> and <strong>IMS</strong> based on those trend lines (right).<br />

Figure 4. <strong>DMS</strong>-<strong>IMS</strong> 2-D spectra <strong>for</strong> positive toluene ions in nitrogen (left, 4.5ppb) and<br />

in air (right, 17.5ppb), showing resolution of multiple ions <strong>enhanced</strong> by the extended<br />

analytical space.

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