# US 10,117,626 B2 · Apparatus and method for pile-up correction in photon-counting detector

> Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt

- Number: US 10,117,626 B2
- Document ID: US10117626B2
- Status: Granted
- Kind: B2
- Application number: 14/868,826
- Filed: 2015-09-29
- Published: 2017-03-30
- Granted: 2018-11-06
- Earliest claimed: 2015-09-29
- Assignees: General Electric Company
- Applicants: General Electric Company
- Inventors: Geng Fu; Peter Michael Edic; Brian David Yanoff; Jianjun Guo; Vladimir A. Lobastov; Yannan Jin
- Web page: https://patentgrep.com/patent/US10117626B2

## CPC

- A61B 6/4241: {using energy resolving detectors, e.g. photon counting}
- A61B 6/032: {Transmission computed tomography [CT]}
- A61B 6/4208: {characterised by using a particular type of detector}
- A61B 6/4233: {using matrix detectors}
- A61B 6/4435: {the source unit and the detector unit being coupled by a rigid structure}
- A61B 6/4441: {the rigid structure being a C-arm or U-arm}
- A61B 6/5205: {involving processing of raw data to produce diagnostic data}
- A61B 6/54: {Control of apparatus or devices for radiation diagnosis}
- A61B 6/461: {Displaying means of special interest}
- A61B 6/467: {characterised by special input means}
- A61B: DIAGNOSIS; SURGERY; IDENTIFICATION (usefulness limited to only animals A61D)

## Abstract

Some embodiments are associated with an input signal comprising a first and a second photon event incident on a photon-counting semiconductor detector. A relatively slow charge collection shaping amplifier may receive the input signal and output an indication of a total amount of energy associated with the superposition of the first and second events. A relatively fast charge collection shaping amplifier may receive the input signal and output an indication that is used to allocate a first portion of the total amount of energy to the first event and a second portion of the total amount of energy to the second event.

## Claims

### Claim 1

A system, comprising:
a detection system comprising a photon-counting semiconductor detector, configured to receive an input signal associated with a first event and a second event;
a relatively slow charge collection shaping amplifier configured to receive the input signal and to output an indication of a total amount of energy associated with a combination of the first event and the second event; and
a relatively fast charge collection shaping amplifier configured to receive the input signal and further configured to output an indication that is used to allocate a first portion of the total amount of energy to the first event and a second portion of the total amount of energy to the second event.

### Claim 2 (depends on 1)

The system of claim 1, wherein the relatively slow charge collection shaping amplifier has a first time constant and the relatively fast charge collection shaping amplifier has a second time constant, the first time constant and second time constant being characterized by at least one of: (i) a detector weighting potential profile, (ii) an applied electric field, and (iii) semiconductor material properties.

### Claim 3 (depends on 2)

The system of claim 2, wherein the relatively slow charge collection shaping amplifier comprises a low-bandwidth, band-pass filter, and the relatively fast charge collection shaping amplifier comprises a high-bandwidth, band-pass filter.

### Claim 4 (depends on 1)

The system of claim 1, further comprising a charge sensitive amplifier configured to receive the input signal, wherein the charge sensitive amplifier is coupled to the photon-counting semiconductor detector.

### Claim 5 (depends on 1)

The system of claim 1, wherein the relatively fast charge collection shaping amplifier is configured to: record a photon count in one of a plurality of bins based on an energy threshold, and further configured to use a number of photons in each bin of the plurality of bins to allocate the first portion of the total amount of energy to the first event and the second portion of the total amount of energy to the second event.

### Claim 6 (depends on 5)

The system of claim 5, wherein the plurality of bins include: (i) a noise bin, (ii) a low-energy bin, and (iii) a high-energy bin.

### Claim 7 (depends on 1)

The system of claim 1, wherein the relatively fast charge collection shaping amplifier comprises a peak analog-to-digital converter or a charge-to-digital converter and is configured to: measure a first amplitude value associated with the first event using the peak analog-to-digital converter or the charge-to-digital converter, measure a second amplitude value associated with the second event using the peak analog-to-digital converter or the charge-to-digital converter, and allocate the total amount of energy to the first event and the second event based on the first amplitude value and the second amplitude value.

### Claim 8

A method, comprising:
receiving an input signal associated with a first event and a second event in a photon-counting semiconductor detector;
generating, by a relatively slow charge collection shaping amplifier based on the input signal, an indication of a total amount of energy associated with the first event and the second event; and
allocating, in accordance with information from a relatively fast charge collection shaping amplifier based on the input signal, a first portion of the total amount of energy to the first event and a second portion of the total amount of energy to the second event.

### Claim 9 (depends on 8)

The method of claim 8, wherein the relatively slow charge collection shaping amplifier comprises a low-bandwidth, band-pass filter having a first time constant and the relatively fast charge collection shaping amplifier comprises a high-bandwidth, band-pass filter having a second time constant.

### Claim 10 (depends on 9)

The method of claim 9, wherein the first time constant and the second time constant are characterized by at least one of: (i) a detector weighting potential profile, (ii) an applied electric field, and (iii) semiconductor material properties.

### Claim 11 (depends on 8)

The method of claim 8, further comprising recording a photon in one of a plurality of bins based on an energy threshold with the relatively fast charge collection shaping amplifier, and allocating the first portion of the total amount of energy to the first event and the second portion of the total amount of energy to the second event using a number of photons in each bin of the plurality of bins, wherein the plurality of bins include: (i) a noise bin, (ii) a low energy bin, and (iii) a high energy bin.

### Claim 12 (depends on 8)

The method of claim 8, further comprising measuring a first amplitude value associated with the first event using a peak analog-to-digital converter or a charge-to-digital converter, measuring a second amplitude value associated with the second event using the peak analog-to-digital converter or the charge-to-digital converter, and allocating the total amount of energy to the first event and the second event based on the first amplitude value and the second amplitude value.

### Claim 13 (depends on 12)

The method of claim 12, further comprising recording a first timing value in connection with the first event, recording a second timing value in connection with the second event, and correcting an allocation of the total amount of energy based on the first timing value and the second timing value.

### Claim 14

An imaging system, comprising:
an X-ray source configured to transmit X-rays toward an object;
a photon-counting semiconductor detector configured to detect the X-rays traversing the object and to generate a detector signal associated with a first event and a second event;
a charge sensitive amplifier configured to receive the detector signal and generate an output signal based on the detector signal;
a relatively slow charge collection shaping amplifier configured to receive the output signal from the charge sensitive amplifier and to output an indication of a total amount of energy associated with a combination of the first event and the second event; and
a relatively fast charge collection shaping amplifier configured to receive the output signal from the charge sensitive amplifier and to output an indication that is used to allocate a first portion of the total amount of energy to the first event and a second portion of the total amount of energy to the second event.

### Claim 15 (depends on 14)

The imaging system of claim 14, wherein the relatively slow charge collection shaping amplifier comprises a low-bandwidth, band-pass filter having a first time constant and the relatively fast charge collection shaping amplifier comprises a high-bandwidth, band-bass filter having a second time constant.

### Claim 16 (depends on 15)

The system of claim 15, wherein the first time constant and the second time constant are characterized by at least one of: (i) a detector weighting potential profile, (ii) an applied electric field, and (iii) semiconductor material properties.

### Claim 17 (depends on 14)

The imaging system of claim 14, wherein the relatively fast charge collection shaping amplifier records a photon in one of a plurality of bins based on an energy threshold, and a number of photons in each bin of the plurality of bins is then used to allocate the first portion of the total amount of energy to the first event and the second portion of the total amount of energy to the second event, and further wherein the plurality of bins include: (i) a noise bin, (ii) a low-energy bin, and (iii) a high-energy bin.

### Claim 18 (depends on 14)

The imaging system of claim 14, wherein the relatively fast charge collection shaping amplifier comprises a peak analog-to-digital converter, wherein the relatively fast charge collection shaping amplifier measures a first amplitude value associated with the first event using the peak analog-to-digital converter, and measures a second amplitude value associated with the second event using the peak analog-to-digital converter, and an allocation of the total amount of energy to the first event and the second event is based on the first amplitude value and the second amplitude value.
