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Introduction Chris Heintz, Walter Wißdorf, Thorsten Benter, Hendrik Kersten Physical & Theoretical Chemistry Wuppertal, Germany Institute for Pure and Applied Mass Spectrometry The Bessel-box is a kinetic energy filter, first introduced in 1976 by Allen et al. Herein a beam of charged particles with a certain kinetic energy distribution enters a cylindrical electrode through a pinhole entrance. The beam is deflected from its straight path through the cylinder by a small center electrode. Consequently, only particles with a kinetic energy matching the forces of the electrical field inside the box follow a trajectory around the center plate and can leave the Bessel-box through a second pinhole in the exit electrode. This energy filter is used, e.g., by Hiden Analytical, upstream of the quadrupole analyzer. We present numerical results on the transmission and filter characteristics of this particular Bessel-box. Simulation of ion trajectories in an electrostatic Bessel-box type energy filter Methods Conclusions Acknowledgement Literature [1] Heintz, C. : Numerische Ionentrajektoriensimulation in einem elektrostatischen Bessel-Box Energiefilter. Bachelorthesis, DE (2017) [2] J. D. Allen, J. D. Durham, G. K. Schweitzer und W. E. Deeds, „A New Electron Spectrometer Design: II,“ Journal of Electron Spectroscopy and Related Phenomena, Bd. 8, pp. 395-410, 1976. [3] P. M. Thompson, J. W. Taylor und R. E. Negri, „Retardung- field differential-output energy prefilter for high- performance secondary ion mass sepectrometry,“ Review of Scientific Instruments, Bd. 56, Nr. 8, pp. 1557- 1593, 1985. [4] Scientific Instrument Services, Inc., SIMION 8.0 User Manual, 2008. [5] Hiden Analytical Limited, Power Supply and Trip Unit User Manual, Warrington: Hiden Analytical Limited, 2005. Potential Dependency The bessel-box voltage U B adjusts the transmitted kinetic energy range with virtually constant transmission width. The transmission width is essentially a linear function of the endcap voltage U E for bessel-box voltages U B > 2.5V: , =ቊ 0.0278 · + −0.0174 · + 00611 , < 2.5 00648 · + 0564 , ≥ 2.5 The transmission efficiency mainly depends on the endcap voltage and ranges between 5 and 30%. Fitted functional correlation between the high energy cut-off of the transmitted energy range and U B /U E : []( , ) = 0.937 ∙ + (−0.0322 ∙ + 0.5146) Additional simulation of the subsequent quadrupole geometry. Simulation of the overall ion transmission efficiency (bessel-box and analyzer). Experimental validation of the simulated results. Financial support by iGenTrax UG (Haan, Germany) is greatfully acknowledged. The geometry of the Bessel-box under investigation was taken from the user’s manual of the HPR60 quadrupole mass spectrometer from Hiden Analytical Ltd.. Electrical fields and corresponding ion trajectories were simulated with Simion 8.1. Custom Lua scripts and python code allowed for automated simulation processing, data visualization and analysis. Each simulation started with an initial ion population of 10 000 singly charged particles with a mass of 3 Da and an evenly distributed initial kinetic energy ranging from 0 to 10 eV. Goal Simulation of ion trajectories inside a Bessel-box type energy filter with SIMION® Investigate the relation between the different potentials and ion trajectories, transmission range and transmission width Determination of energy distributions of the transmitted ions in dependence of the applied potentials Geometry Source Case Endcap Centerstop/ Bessel-box Quadrupole-Rods Endcap Entrance Entrance Transmission Bessel-Box: 0.1 V Bessel-Box: 1.0 V Bessel-Box: 2.6 V Bessel-Box: 5.0 V Fig. 2: Simulated ion trajectories with initial kinetic energies between 1 eV and 10 eV at different bessel-box settings. Endcaps were kept at -26.5 V. Transmission range correlates strongly with bessel-box Potential Fig. 3: Initial kinetic energy (KE) distribution of transmitted ions with varying bessel-box settings and -25 V endcap potential. Fig. 4: (above) Kinetic energy (KE) distribution of transmitted ions with constant bessel-box potential. (right) The transmission width as a function of the endcap potential at a fixed bessel-box voltage of 5 V (good approximation for bessel-box seetings >2.5 V). Transmission width and intensity correlates strongly with Endcap Potential Fig. 8: Kinetic energy distribution of transmitted ions (orange) in contrast to the KE distribution of all simulated ions (blue) with varying endcap voltage at 5 V bessel-box potential. Outlook the ratio of transmitted ions is virtually independent of the bessel-box voltage the ratio of transmitted ions strongly depends on the endcap voltage bend slope for bessel-box voltages > 8 V due to simulation conditions Figure 3 depicts the gaussian like distributions for bessel-box settings below 2.5 V. The transmission distribution for bessel-box settings at 2.5 V and higher show a clear KE cut off on both sides. Fig. 5: The standard deviation of the transmission distribution as a measure for the transmission range plotted as a function of the bessel- box voltage for different endcap settings. Fig. 6: Transmission width as a function of the endcap voltages for bessel-box settings below 2.5 V. Maximal transmitted kinetic energy as measure for the transmission range Fig. 10: Maximal transmitted kinetic energy as a function of the Bessel-box potential for several endcap voltages. Fig. 11: Maximal transmitted kinetic energy as a function of the endcap potential at zero bessel-box voltage (y-intercepts of the fitting functions from Fig. 10). Fig. 7: Kinetic energy (KE) distribution of transmitted ions (orange) in contrast to the KE distribution of all simulated ions (blue) with varying bessel-box voltage at -25 V endcap potential. Fig. 1: 3D and 2D schematic drawing of the ion source, simulated bessel-box and subsequent quadrupole analyzer (HPR60, Hiden Analytical Ltd.). Fig. 9: Transmission ratio as a function of the bessel-box voltage for different endcap settings. good approximation for bessel-box settings > 2.5 V good approximation for bessel-box settings < 2.5 V

Simulation of ion trajectories in an electrostatic Bessel ... · Chris Heintz, Walter Wißdorf, Thorsten Benter, Hendrik Kersten Physical & Theoretical Chemistry Wuppertal, Germany

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Page 1: Simulation of ion trajectories in an electrostatic Bessel ... · Chris Heintz, Walter Wißdorf, Thorsten Benter, Hendrik Kersten Physical & Theoretical Chemistry Wuppertal, Germany

Introduction

Chris Heintz, Walter Wißdorf, Thorsten Benter, Hendrik KerstenPhysical & Theoretical Chemistry

Wuppertal, Germany

Institute for Pure and Applied Mass Spectrometry

The Bessel-box is a kinetic energyfilter, first introduced in 1976 by Allenet al. Herein a beam of chargedparticles with a certain kinetic energydistribution enters a cylindricalelectrode through a pinhole entrance.The beam is deflected from itsstraight path through the cylinder bya small center electrode.Consequently, only particles with akinetic energy matching the forces ofthe electrical field inside the boxfollow a trajectory around the centerplate and can leave the Bessel-boxthrough a second pinhole in the exitelectrode. This energy filter is used,e.g., by Hiden Analytical, upstream ofthe quadrupole analyzer. We presentnumerical results on the transmissionand filter characteristics of thisparticular Bessel-box.

Simulation of ion trajectories in an electrostatic

Bessel-box type energy filter

Methods

Conclusions

Acknowledgement

Literature[1] Heintz, C. : Numerische Ionentrajektoriensimulation in

einem elektrostatischen Bessel-Box Energiefilter.Bachelorthesis, DE (2017)

[2] J. D. Allen, J. D. Durham, G. K. Schweitzer und W. E.Deeds, „A New Electron Spectrometer Design: II,“Journal of Electron Spectroscopy and RelatedPhenomena, Bd. 8, pp. 395-410, 1976.

[3] P. M. Thompson, J. W. Taylor und R. E. Negri, „Retardung-field differential-output energy prefilter for high-performance secondary ion mass sepectrometry,“Review of Scientific Instruments, Bd. 56, Nr. 8, pp. 1557-1593, 1985.

[4] Scientific Instrument Services, Inc., SIMION 8.0 UserManual, 2008.

[5] Hiden Analytical Limited, Power Supply and Trip UnitUser Manual, Warrington: Hiden Analytical Limited,2005.

Potential Dependency

• The bessel-box voltage UB adjusts thetransmitted kinetic energy range withvirtually constant transmission width.

• The transmission width 𝜎 is essentially a linear function of the endcap voltage UE

for bessel-box voltages UB > 2.5V:

𝜎 𝑈𝐵 , 𝑈𝐸

= ቊ0.0278 · 𝑈𝐵 + −0.0174 · 𝑈𝐸 + 00611 , 𝑈𝐵< 2.5 𝑉00648 · 𝑈𝐸 + 0564 , 𝑈𝐵≥ 2.5 𝑉

• The transmission efficiency mainlydepends on the endcap voltage andranges between 5 and 30%.

• Fitted functional correlation between thehigh energy cut-off of the transmittedenergy range and UB/UE:

𝐸𝑘𝑖𝑛[𝑒𝑉](𝑈𝐵 , 𝑈𝐸)= 0.937 ∙ 𝑈𝐵 + (−0.0322 ∙ 𝑈𝐸 + 0.5146)

• Additional simulation of the subsequentquadrupole geometry.

• Simulation of the overall ion transmissionefficiency (bessel-box and analyzer).

• Experimental validation of the simulatedresults.

Financial support by iGenTrax UG (Haan, Germany) is greatfully acknowledged.

The geometry of the Bessel-boxunder investigation was taken fromthe user’s manual of the HPR60quadrupole mass spectrometer fromHiden Analytical Ltd.. Electrical fieldsand corresponding ion trajectorieswere simulated with Simion 8.1.Custom Lua scripts and python codeallowed for automated simulationprocessing, data visualization andanalysis. Each simulation started withan initial ion population of 10 000singly charged particles with a massof 3 Da and an evenly distributedinitial kinetic energy ranging from 0 to10 eV.

Goal

• Simulation of ion trajectoriesinside a Bessel-box type energyfilter with SIMION®

• Investigate the relation betweenthe different potentials and iontrajectories, transmission rangeand transmission width

• Determination of energydistributions of the transmittedions in dependence of the appliedpotentials

Geometry

Source CaseEndcapCenterstop/Bessel-box

Quadrupole-Rods Endcap

Entrance

Entrance

Transmission

Bessel-Box: 0.1 V Bessel-Box: 1.0 V

Bessel-Box: 2.6 V Bessel-Box: 5.0 V

Fig. 2: Simulated ion trajectories with initial kinetic energies between 1 eV and 10 eV at different bessel-box settings. Endcaps were kept at -26.5 V.

Transmission range correlates strongly with bessel-box Potential

Fig. 3: Initial kinetic energy (KE) distribution of transmitted ions with varying bessel-box settings and -25 V endcap potential.

Fig. 4: (above) Kinetic energy (KE) distribution of transmitted ions withconstant bessel-box potential. (right) The transmission width as a function ofthe endcap potential at a fixed bessel-box voltage of 5 V (goodapproximation for bessel-box seetings >2.5 V).

Transmission width and intensity correlates strongly with Endcap Potential

Fig. 8: Kinetic energy distribution of transmitted ions (orange) in contrast to the KE distribution of all simulated ions (blue) with varying endcap voltage at 5 V bessel-box potential.

Outlook

• the ratio of transmitted ions is virtuallyindependent of the bessel-box voltage

• the ratio of transmitted ions strongly dependson the endcap voltage

• bend slope for bessel-box voltages > 8 V due tosimulation conditions

• Figure 3 depicts the gaussian like distributions forbessel-box settings below 2.5 V.

• The transmission distribution for bessel-box settingsat 2.5 V and higher show a clear KE cut off on bothsides.

Fig. 5: The standarddeviation of thetransmission distribution asa measure for thetransmission range plottedas a function of the bessel-box voltage for different endcap settings.

Fig. 6: Transmission width as a function ofthe endcap voltagesfor bessel-box settingsbelow 2.5 V.

Maximal transmitted kinetic energy as measure for the transmission range

Fig. 10: Maximal transmitted kineticenergy as a function ofthe Bessel-box potential for severalendcap voltages.

Fig. 11: Maximal transmitted kinetic energy as a function of the endcap potential at zero bessel-box voltage (y-intercepts of thefitting functionsfrom Fig. 10).

Fig. 7: Kinetic energy (KE) distribution of transmitted ions (orange) in contrast to the KE distribution of all simulated ions (blue) with varying bessel-box voltage at -25 V endcap potential.

Fig. 1: 3D and 2D schematic drawing of the ion source, simulated bessel-box and subsequent quadrupole analyzer (HPR60, HidenAnalytical Ltd.).

Fig. 9: Transmission ratio as a function of the bessel-box voltage for different endcap settings.

good approximation for

bessel-box settings > 2.5 V

good approximation for

bessel-box settings < 2.5 V