# US 2018/0025898 A1 · Time-of-Flight Analysis of a Continuous Beam of Ions by a Detector Array

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- Number: US 2018/0025898 A1
- Document ID: US20180025898A1
- Status: Published application
- Kind: A1
- Application number: 15/713,416
- Filed: 2017-09-22
- Published: 2018-01-25
- Earliest claimed: 2013-12-31
- Assignees: DH Technologies Development Pte. Ltd.
- Applicants: DH Technologies Development Pte. Ltd.
- Inventors: Robert Alois Grothe, JR.
- Web page: https://patentgrep.com/patent/US20180025898A1

## CPC

- H01J 49/40: Time-of-flight spectrometers (H01J49/36 takes precedence)
- H01J 49/0031: {Step by step routines describing the use of the apparatus (H01J49/0081 takes precedence)}
- H01J 49/025: {Detectors specially adapted to particle spectrometers (data acquisition H01J49/0036; detectors per se G01T, e.g. G01T1/28, G01T1/29)}
- H01J 49/20: Magnetic deflection
- H01J 49/22: Electrostatic deflection
- H01J: ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS (spark-gaps H01T; electric arc lamps H05B31/00; particle accelerators H05H)

## Abstract

Systems and methods are provided for time-of-flight analysis of a continuous beam of ions by a detector array. A sample is ionized using an ion source to produce a continuous beam of ions. An electric field is applied to the continuous beam of ions using an accelerator to produce an accelerated beam of ions. A rotating magnetic and/or electric field is applied to the accelerated beam to separate ions with different mass-to-charge ratios over an area of a two-dimensional detector using a deflector located between the accelerator and the two-dimensional detector. An arrival time and a two-dimensional arrival position of each ion of the accelerated beam are recorded using the two-dimensional detector. Alternatively, an electric field that is periodic with time is applied in order to sweep the accelerated beam over a periodically repeating path on the two-dimensional rectangular detector.

## Claims

### Claim 1

A time-of-flight mass (TOF) spectrometer for analyzing a continuous beam of ions that optimizes the utilization of the area of a rectangular detector, comprising:
an ion source that ionizes a sample producing a continuous beam of ions;
a mass filter that receives the continuous beam and admits ions with a desired range of mass-to-charge ratios and blocks ions outside the desired range producing a filtered beam of ions;
an accelerator that receives the filtered beam and applies an electric field to the continuous beam of ions producing an accelerated beam of ions;
a two-dimensional rectangular detector that records an arrival time and a two-dimensional arrival position of each ion in the accelerated beam; and
a deflector located between the accelerator and the two-dimensional rectangular detector that receives the accelerated beam and applies an electric field that is periodic with time to the accelerated beam in order to sweep the accelerated beam over a periodically repeating path on the two-dimensional rectangular detector,
wherein the repeat period is set to the difference in the times required for ions with the highest and lowest mass-to-charge ratios in the filtered beam to travel from the deflector to the two-dimensional rectangular detector and
wherein the path has a maximum length among all paths that satisfies the following constraint:
for any point x on the two-dimensional rectangular detector, the intersection between a circular region of diameter s centered about x and the path contains no more than one segment, where s denotes the diameter of the accelerated beam's cross section measured at the two-dimensional rectangular detector.

### Claim 2 (depends on 1)

The TOF mass spectrometer of claim 1, wherein the path comprises a raster pattern.

### Claim 3 (depends on 1)

The TOF mass spectrometer of claim 1, wherein the path comprises at least two parallel rows and each row is connected to an adjacent row by a semi-circular arc.

### Claim 4 (depends on 1)

The TOF mass spectrometer of claim 1, further comprising
a processor in communication with the accelerator, the deflector, and the two-dimensional detector that
receives an arrival time and a two-dimensional arrival position for each ion impacting the two-dimensional rectangular detector and
calculates a time-of-flight for each ion impacting the two-dimensional rectangular detector from the arrival time and the two-dimensional arrival position.

### Claim 5

A method for analyzing the time-of-flight of a continuous beam of ions that optimizes the utilization of the area of a rectangular detector, comprising:
ionizing a sample using an ion source to produce a continuous beam of ions;
admitting ions with a desired range of mass-to-charge ratios and blocking ions outside the desired range using a mass filter producing a filtered beam of ions;
applying an electric field to the filtered beam producing an accelerated beam of ions;
applying an electric field that is periodic with time to the accelerated beam in order to sweep the accelerated beam over a periodically repeating path on a two-dimensional rectangular detector using a deflector,
wherein the repeat period is set to the difference in the times required for ions with the highest and lowest mass-to-charge ratios in the filtered beam to travel from the deflector to the two-dimensional rectangular detector and
wherein the path has a maximum length among all paths that satisfies the following constraint:
for any point x on the two-dimensional rectangular detector, the intersection between a circular region of diameter s centered about x and the path contains no more than one segment, where s denotes the diameter of the accelerated beam's cross section measured at the two-dimensional rectangular detector; and
recording an arrival time and a two-dimensional arrival position of each ion in the accelerated beam using the two-dimensional rectangular detector.
