Time-of-Flight Mass Analyzers

Transcription

1 Time-of-Flight Mass Analyzers Jonathan Karty C613 lecture 1 March 6, 8 (Section 4. in Gross, pages )

2 TOF Overview Time-of-flight (TOF) is the least complex mass analyzer in terms of its theory Ions are given a defined kinetic energy and allowed to drift through a field-free region (.5 to several meters) The time ions arrive at the detector is measured and related to the m/z ratio

3 TOF Concept A packet of stationary ions is accelerated to a defined kinetic energy and the time required to move through a fixed distance is measured First TOF design published in 1946 by W.E. Stephens Detector

4 TOF advantages Theoretically unlimited mass range Ions are not trapped (quad, IT, FTICR) nor are their flight paths curved (BE sectors) Detection efficiencies induce practical limits of a few hundred kda (M+H)+ Instrument is not scanning (it is dispersive) Analysis is very rapid (4+ khz acquisition possible) Wide range of m/z s can be measured with good sensitivity Moderate to high resolving powers (5,-,+) Moderate cost ($1k to $5k) Relatively high duty cycle Couples extremely well with pulsed ion sources (e.g. MALDI)

5 TOF Disadvantages Requires high vacuum (<1-6 torr) Coupling to continuous ion sources (e.g. ESI or EI) not straight forward Requires complex and high speed electronics High acceleration voltages (5-3 kv) Fast detectors (ns or faster) GHz sampling digital conversion Large volumes of data can be generated quickly Limited dynamic range Often 1 or 1 3 at most High resolution instruments can get rather large

6 From Physics 1: (1) KE = ½mv From Physics : () KE = z*u = ½mv All ions accelerated by the same voltage, U From Physics 1: (3) ΔX= v TOF + ½aTOF * U * z ( 4) v = m 1, Th 19 kv, v 6 km/sec X m ( 6) TOFflight _ tube = * * U z (5) TOF = ΔX/v Time-of-Flight Theory ΔX same for all ions = D (flight tube length) No acceleration in flight tube TOF α U -1 α (m/z) ½

7 Mass Scale Calibration TOF α (m/z) 1/ or m/z α TOF Mass scale is calibrated measuring flight times known m/z ions and fitting them to a polynomial equation (7) TOF = a*(m/z) 1/ + b also Higher order calibrations are often used 5 th order on some commercial instruments Form can be (7a) m/z = A*TOF + B*TOF + C

8 Resolution in TOF MS ( 8) z * U = * m* v * z * U ( 1) v t D (9) m = * z * U v m * z * U ( t D = D / t m = * 11) = *t * z * U 1) m = *t * t D ( ( * z * U ) * t m t (13) = D = m (* z * U ) *t * dt t D Easy way to improve resolution is to increase flight tube length (assuming excellent vacuum)

9 Real-world TOF MS Previous examples all assumed ions formed at rest, at the same time, and all at the same position in the source In reality, ions are formed throughout the source at various times, in various locations, with a range of initial kinetic energies Practical TOF instrument design relies on minimizing the contributions of each of these realities

10 Influence of Initial Position In EI, CI, and ESI sources, ions are NOT formed all in the exact same position These differences in initial position have profound effects on the mass spectrum Ions spend some time in the source prior to crusing through the flight tube (14) TOF obs = TOF source + TOF flight_tube A more complete treatment of the TOF requires that we consider how the ions get accelerated

11 A brief discussion of acceleration Ions are usually accelerated by using parallel plates at different potentials to create electric fields Ions in an electric field gain energy according to the equation: (15) KE = z*(e*s) or U = z*(e*s) z is charge, E is electric field strength in V/m, and s is distance the ion travels in the field (Lorentz force equation) Time of flight in the source must be computed with a differential equation

12 Initial Position Math * U * z ( 4) v = m ( 15)U = E * s (17) v s = * z * E * s m = s t (16) s = * z * E * s m t (19) s * z * E * s = m t (18) t m = * z * E 1 * 1/ s s (1) t s t = s * m z * E s 1/ s +1 V V () t s = m * z * E *s m m () t s = * s (3) t d = * D * z * E * s * z * E * s (14) TOF m = t + td = (4) * * z * E * s ( s D) s +

13 Starting Position Example Both ions are 1 m/z (1.364*1-6 kg/c) Red ion is 6 mm from V plate, blue ion is 5 mm from V plate s for red is.6 m; s for blue is.5 m Distance between plates is 1 cm Electric field is 1, V/m Detector is 1 m from nd grid (4) TOF m = t + td = * * z * E * s TOF red = 94 usec TOF blue = 11 usec E red = 6 ev, E blue = 5 ev ( s D) s + Detector +1 V V This effect tends to cause peaks to tail to longer TOF

14 Initial Kinetic Energy Spread If the ion has a non-zero kinetic energy along the axis of the flight tube prior to acceleration: (5) KE total = z*u+u (U is initial KE) At 5 K, kt =.43 ev Kinetic energies perpendicular to this axis can cause the ions to miss the detector entirely The initial kinetic energy spread and initial position can be accounted for mathematically m* v 6) ( = U + z * E * s ( 7) v = *( U ) + z * E * s m

15 How long do ions spend in the source? 7) v s = *( U + z * E * s) m ( = s t 8) s = *( U + z * E * s) * t m ( (9) t s t = s m * ( U + s z * E * s ) ( m) [( ) ] U * z * E * s ± U ( 3) t s = * + t z * E (initial KE and position) (initial direction) (uncertainty of ion formation)

16 Putting this all together ( m) [( ) ] U * z * E * s ± U ( 3) t s = * + t z * E (31) t D * + ( m) * D ( U z * E * s) = D ( m) (14) TOF = t s + t [( ) ] ( ) m * D U * z * E * s ± U + * ( U + z * E * s) ( 3) TOF = * + t z * E Source design is used to minimize the variables that contribute to peak broadening High U to minimize U Narrow ion formation regions to minimize s Pulsing ions out of source to minimize t

17 TOF designs to maximize resolving power High acceleration voltages can reduce impact of initial KE distribution Initial position effects are harder to minimize Additional ion optical elements can be introduced to compensate for these two effects Set flight tube axis perpendicular to major vector of KE distribution orthogonal extraction

18 Time-lag focusing There is a point in the flight tube where ions starting at different positions arrive simultaneously m m ( 33) ts = t D (34) * s = * D (35) D = s Adding a third grid allows the analyst to move this focus plane to the detector +1 V +9 V ( * z * E * s) ( * z * E * s) 1955, Wiley and McLaren 1994, Colby, King, and IU (special case for MALDI) s is related to initial KE since all ions formed simultaneously Detector V +1 V

19 Reflectrons? In 1966, B. Mamyrin patented an ion mirror device for energy focusing and resolution improvement A reflectron is a long series of electrodes that create an electric field to reverse the direction the ions travel Higher energy ions spend more time in reflectron than lower energy ions By adjusting parameters, ions with same m/z but slightly different KE s can be made to arrive at a detector simultaneously

20 Reflectron drawing +11 V V V +1 V Detector m 36) TOF = * 1 4 * z * E ( ( D + D + ) D ref m 37) TOF = * 1 4 *( z * E + U ) ( z * E + U (38) D = * z * E ref D ref ( D + D + ) D ref

21 Reflectron Pros and Cons Advantages Focuses kinetic energies Better resolution Allows one to use same flight tube twice Remember, res power increases with D Cons Only a narrow range of KE can be focused Usually 85%-15% of E Metastable ions are not focused by reflectron If ion fragments in flight tube, products have same velocity as precursors (but KE is proportional to mass of product) Reflectron focuses by energy

22 Measuring TOF Signals Oscilloscope (aka multi-channel scaler) Analog recorder (ion current vs. time) Great for intense signals Generates large data files (all times recorded) Noise recorded as well as signal Time to Digital Converter Records only when an event occurred Threshold is set so an event is arrival of 1 ion Excellent for low signals (single ion counting) Does NOT take into account intensity ions arriving simultaneously counts as 1 event Limited dynamic range

23 Factors that Influence Resolution Laser pulse width in MALDI Detector response profile Digitization rate and amplifier bandwidths Kinetic energy distribution of ions Initial position of ions in source Power supply stability Response profiles of pulsing electronics

24 Waters LCT Drawing Mass range: 6-, m/z Resolving power: ~5, 54 psec resolution TDC ESI or APCI source MS recorded at ~ khz Table-top MS (1.5x1x1 m) Cost ~$,