Dale A Gedcke

6347288, Feb 12, 2002

Nov 10, 1999

09/437857

Rex C. Trammell - Andersonville TN
Russell D. Bingham - Knoxville TN
Dale A. Gedcke - Oak Ridge TN

PerkinElmer Instruments - Knoxville TN

H03H 1700

702107, 702106, 702 69, 2503361, 25037001, 330305

An automatic pole-zero (APZ) adjustment circuit for an ionizing radiation spectroscopy system. An output of a preamplifier is sampled to identify the decay time constant of the preamplifier output. A correction based upon the identified decay time constant is generated by a correction signal generator and applied through either an analog pole-zero adjustment network or a programmable digital shaping filter to accomplish pole-zero correction.

6785194, Aug 31, 2004

May 15, 2002

10/146842

Jeffrey V. Peck - Knoxville TN
Dale A. Gedcke - Oak Ridge TN
Russell D. Bingham - Knoxville TN

Advanced Measurement Technology, Inc. - Oak Ridge TN

G04F 1000

368113, 368118, 368120, 370518

A method and apparatus for precision time interval measurement in a time-of-flight mass spectrometer (TOF-MS). The method and apparatus produces an instrument capable of measuring bursts of data occurring at rates much higher than the average data rate. An asynchronous serial stream of data, consisting of a start pulse followed by an arbitrary number of stop pulses, repeated an arbitrary number of times, is converted into a digital stream of data synchronized to a precision master clock. Conversion of the asynchronous, analog data to synchronous digital data simplifies the measurement task by allowing the use of powerful, low-cost digital logic in the measurement.

61005339, Aug 8, 2000

May 11, 1998

9/076296

Mario Pierangelo Martini - Oak Ridge TN
Dale A. Gedcke - Oak Ridge TN
Thomas W. Raudorf - Oak Ridge TN
Pat Sangsingkeow - Knoxville TN

EG&G Instruments, Inc. - Oak Ridge TN

H01L 2906

25037001

A three-axis radiation detection system whose inner and outer electrodes are shaped and positioned so that the shortest path between any point on the inner electrode and the outer electrode is a different length whereby the rise time of a pulse derived from a detected radiation event can uniquely define the azimuthal and radial position of that event, and the outer electrode is divided into a plurality of segments in the longitudinal axial direction for locating the axial location of a radiation detection event occurring in the diode.

59959894, Nov 30, 1999

Apr 24, 1998

9/065733

Dale A. Gedcke - Oak Ridge TN
Russell D. Bingham - Knoxville TN
Susan Haywood - Oak Ridge TN

EG&G Instruments, Inc. - Wellesley MA

G06F 1710

708300

A method and apparatus for compression and filtering of data associated with spectrometry. The method and apparatus serves to recognize peak events and filter data associated with background noise, thereby reducing the volume of data to be transferred to storage and the data transfer rate required for storing the desired data. The method of the present invention monitors the value of each data point as it is encountered and compares it to the previously encountered data to determine whether it is on or very near a peak. The y values for each data point are continuously summed and averaged to determine the average background level. The deviation. delta. sub. i is determined for each subsequent data point and is used to determine a threshold. Each subsequent data point is compared to the threshold and, if found to be above the threshold, is assumed to be part of or very near a peak. At this point, the averaging is stopped until a subsequent data point is determined to be below the threshold.

60285435, Feb 22, 2000

Sep 16, 1998

9/154134

Dale A. Gedcke - Oak Ridge TN
Jeffrey V. Peck - Knoxville TN
Russell D. Bingham - Knoxville TN
Rex C. Trammell - Andersonville TN

EG&G Instruments, Inc. - Wellesley MA

H03M 120

341131

A method for improving the speed of convergence to sub-least-significant-bit accuracy and precision in a digital signal averager when the measurements are averaged over many samples where the noise inherent in the signal is not large compared to 1 LSB. A slider offset circuit implements the method which adds offsets to an analog input signal acquired from an analog sensor. The slider offset circuit compensates for limitations in the resolution of an analog-to-digital converter by adding a sub-least-significant-bit offset to the input signal. Similarly, the slider offset circuit compensates for the differential non-linearity using a Gatti offset which are whole number multiples of the average voltage bin width. Speed of convergence to sub-LSB accuracy is further improved by employing non-consecutive increments in the two sliders.

6327549, Dec 4, 2001

Jul 12, 2000

9/614273

Russell D. Bingham - Knoxville TN
Dale A. Gedcke - Oak Ridge TN
Rex C. Trammell - Andersonville TN
Timothy R. Twomey - Berkshire, GB
Ronald M. Keyser - Clinton TN

PerkinElmer, Inc. - Oak Ridge TN

G06F10114
G06F 1500

702180

A differential correction apparatus for use with a spectroscopy device. The spectroscopy device simultaneously produces two histograms corresponding to the spectrum acquired. The first histogram contains the counts recorded by a differential correction method (DCM), giving the best estimate of the counts per channel in the absence of dead time. The second histogram is the error spectrum, giving the variance of the counts in each channel of the first spectrum. The two spectra have the same size, true acquisition time, and energy calibration with the only difference being the number of counts in each channel. By obtaining both histograms, it is possible to both obtain an accurate spectrum when the energy peaks have varying decay times and retain the necessary information about the spectrum to allow the statistical error to be calculated.

57773335, Jul 7, 1998

Mar 26, 1997

8/824514

Mario Pierangelo Martini - Oak Ridge TN
Dale A. Gedcke - Oak Ridge TN
Thomas W. Raudorf - Oak Ridge TN
Pat Sangsingkeow - Knoxville TN

EG&G Instruments, Inc. - Oak Ridge TN

G01N 2304

25037001

An radiation detection system whose inner and outer electrodes are shaped and positioned so that each path between them is a different length is a different length whereby the rise time of a pulse derived from a detected radiation event can uniquely define the azimuthal and radial position of that event.

6094627, Jul 25, 2000

May 4, 1998

9/072388

Jeffrey V. Peck - Knoxville TN
Dale A. Gedcke - Oak Ridge TN
Russell D. Bingham - Knoxville TN

PerkinElmer Instruments, Inc. - Wellesley MA

H03M 100
H03M 120

702199

A digital signal averager for averaging data collected by an analog detector is provided. The digital signal averager includes an analog-to-digital converter for converting the analog detector output to a digital signal for processing, a timing device for generating delayed timing pulses for sequencing operation of the digital signal averager, an averaging device for summing and storing data. The delayed timing pulses allow data to be acquired by the ADC at a series of variably offset timing sequences relative to a trigger pulse. Offsetting the data acquisition timing sequences by time slices smaller than the actual sample rate of the ADC allows data to be acquired at a higher effective sampling rate. One complete series of offset timing sequences provides a data set containing all the information which would be acquired by a ADC having a faster sampling rate. Accuracy of the data is further enhanced by a series of parallel averaging devices, including one processing device and multiple memory devices, which perform real-time averaging of data.